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Lie Algebras With Triangular Decompositions

CANADIAN MATHEMATICAL SOCIETY SERIES OF MONOGRAPHS AND ADVANCED TEXTS ✓ Monographies et Etudes de la Société Mathématique du Canada

EDITORIAL BOARD Frederick V. Atkinson, Bernhard Banaschewski, Colin W. Clark, Erwin O. Kreyszig (Chairman) and John B. Walsh

Frank H. Clarke ^Optimization and Nonsmooth Analysis Erwin Klein and Anthony C, Thompson ^Theory of Correspondences: Including Applications to Mathematical Economics /. Gohbergy P. Lancaster, and L. Rodman Invariant Subspaces of Matrices with Applications Jonathan Borwein and Peter Borwein Pi and the AGM—A Study in Analytic Number Theory and Computational Complexity John H. Berglund, Hugo D. JUnghenn, and Paul Milne "^Analysis of Semigroups: Function Spaces, Compactifications, Representation Subhashis Nag The Complex Analytic Theory of TeichmüUer Spaces Manfred Kracht and Erwin Kreyszig ^Methods of Complex Analysis in Partial Differential Equations with Applications Ernest J. Kani and Robert A. Smith The Collected Papers of Hans Arnold Heilbronn Victor P. Snaith "^Topological Methods in Galois Representation Theory Kalathoor Varadarajan The Finiteness Obstruction of C.TC. Wall G. Watson "^Statistics on Spheres F. Arthur Sherk Kaleidoscopes: Selected Writings ofH. 5. M. Coexeter *Indicates an out-of-print title

Lie Algebras With Triangular Decompositions ROBERT V. MOODY ARTURO PIANZOLA University o f Alberta Edmonton, Canada

A Wiley-Interscience Publication JOHN WILEY & SONS New York

Chichester • Brisbane • Toronto • Singapore

Photograph on title page by M. Goretz

This text is printed on acid-free paper. Copyright © 1995 by John Wiley & Sons, Inc. All rights reserved. Published simultaneously in Canada. Reproduction or translation of any part of this work beyond that permitted by Section 107 or 108 of the 1976 United States Copyright Act without the permission of the copyright owner is unlawful. Requests for permission or further information should be addressed to the Permissions Department, John Wiley & Sons, Inc., 605 Third Avenue, New York, NY 10158-0012. Library o f Congress Cataloging in Publication Data:

Moody, R. V., 1941Lie algebras with triangular decompositions / by Robert V. Moody, Arturo Pianzola. p. cm. — (Canadian Mathematical Society series of monographs and advanced texts) Includes bibliographical references. ISBN 0-471-63304-6 (alk. paper) 1. Lie algebras. 2. Decomposition (Mathematics) I. Pianzola, Arturo, 1955- . II. Title. III. Series. QA252.3.M66 1995 512'.55— dc20 92-46890 Printed in the United States of America 10 9 8 7 6 5 4 3 2 1

Our formula fo r happiness: a yea, a nay, a straight line, a goal. F. Nietzche

Contents Introduction

XI

How to Read This Book

XV

Course Outlines Chapter 1

1.1 1.2 1.3 1.4 1.5 1.6 1.7 1.8 1.9 1.10 1.11 1.12

Basic Definitions Tensor, Symmetric, and Exterior Algebras Gradings Virasoro and Heisenberg Algebras Derivations Representations Invariant Bilinear Forms Universal Enveloping Algebras Central Extensions Free Lie Algebras The Campbell-Baker-Hausdorff Formula Extensions of Modules Exercises

Chapter 2

2.1 2.2 2.3 2.4 2.5 2.6 2.7 2.8 2.9 2.10 2.11 2.12

Lie Algebras

Lie Algebras Adm itting Triangular Decompositions

Triangular and Weight Space Decompositions Highest Weight Modules Verma Modules §l2(IK)-Theorem Characters The Category & The Radical The Shapovalov form Jantzen Filtrations Bernstein-Gel’fand-Gerfand Duality Embeddings of Verma Modules Decomposition of Modules in Category Û Exercises

xix

1

9 15 20 23 28 35 38 49 59 65 71 80 90 91 103 106 116 128 141 160 168 175 184 200 204 209

vüi

Contents

Chapter 3 Lattices and Root Systems 3.1 3.2 3.3 3.4 3.5 3.6 3.7 3.8

Lattices Finite Root Systems Bases for Finite Root Systems Graphs and Coxèter-Dynkin Diagrams Classification of Cartan Matrices and FiniteRoot Systems The Perron-Frobenius Theorem and Its Consequences Constructing Lie Algebras from Lattices Central Extensions of Lattices Exercises

Chapter 4 Contragredient Lie Algebras 4.1 4.2 4.3 4.4 4.5 4.6 4.7

Contragredient Lie algebras Realizations of Contragredient Lie Algebras Embeddings, Field Extensions, and Decomposability Invariant Bilinear Forms Casimir-Kac Operators The Radical Theorem Hermitian Contragredient Forms Exercises

Chapter 5 5.1 5.2 5.3 5.4 5.5 5.6 5.7 5.8 5.9

The Weyl Group and Its Geometry

Root Data The Length Function Coxeter Groups and the Exchange Condition The Bruhat Ordering Morphisms of Root Data: Subroot Systems The Geometry of a Set of Root Data Subroot Systems Imaginary Roots Conjugacy of Bases Exercises

Chapter 6 Category 0 for Kac-Moody Algebras 6.1 6.2 6.3 6.4 6.5 6.6 6.7

Integrable Modules Weight Systems The Triangular Decomposition of G The Formulas of Weyl-Macdonald-Kac Complete Reducibility Shapóvalov Determinant Formula for Kac-Moody Algebras The BGG Theorem and Generalization

216 217 229 239 247 258 272 280 289 302 309 310 330 342 355 367 375 382 385 395 396 408 418 425 430 436 457 464 472 476 483 484 508 516 531 542 545 556

Contents

6.8 Translation Functors and the Generalized Character Formula Exercises Chapter 7 Conjugacy Theorems 7.1 Locally Finite Endomorphisms and Jordan-Chevalley Decompositions 7.2 Locally Finite Elements in Kac-Moody Algebras 7.3 The Kost2mt Cone 7.4 Conjugacy of Split Cartan Subalgebras Exercises

564 574 586

586 606 612 623 639

Appendix .4\*)-An Extended Example

647

Bibliography

675

Index

681

Introduction

One of the great achievements of nineteenth-century mathematicians was the formalization of the notion of symmetry through the introduction of groups and their representations. Now, in the late twentieth century, we can see the pervasive way in which group theory has entered almost every area of mathematics. The Lie groups in particular, which are those that permit infinitesimal motions, have turned out to be of fundamental significance in numerous areas including differential equations, differential geometry, alge­ braic geometry, quantum mechanics, particle physics, special functions, alge­ braic topology, combinatorics, and probability theory, not to mention their role within group theory itself. The entire local structure of a Lie group is codified in a much simpler and purely algebraic structure called its Lie algebra. One of the early accomplishments of the theory of Lie groups was the classification by W. Killing and E. Cartan of the simple and semisimple Lie groups via the classification of their Lie algebras. At the heart of this classification lie some combinatorial objects, the finite root systems, and finite Weyl groups, which are of amazing beauty and to which innumerable problems involving semisim­ ple Lie groups finally come to rest. All of these combinatorial objects admit natural infinite-dimensional gen­ eralizations, and it is possible to develop from them an infinite-dimensional generalization of the semisimple theory that parallels it to a large degree. This generalization is far from complete. In particular the Lie group side of it is still rather modest. By contrast, the Lie algebra side has proved to be very successful and has already turned out to have a variety of applications in other parts of mathematics, notably in differential equations, combinatorics, the theory of modular forms, singularity theory, and string models and conformal field theories in physics. This book is intended as an introduction to the theory of these infinite-dimensional Lie algebras. They have gone by a number of names in the literature, but now they are universally called Kac-Moody algebras. Our objective is to present a self-contained development of the algebraic theory of the Kac-Moody algebras, their representations, and their close relatives, the Virasoro and Heisenberg algebras. We have tried to make the exposition accessible to anyone with a reasonable background in linear

Introduction

algebra. There are a few exceptions, but these are clearly signaled in advance and are not critical to reading the book as a whole. This permits a graduate student who is just beginning Lie theory to get quickly into recent areas in which there are still plenty of accessible open problems. Since the important monograph by V. Kac in 1983 [Ka5], there have been a number of notable developments in Kac-Moody algebras, often at the hands of Kac and his collaborators. We have been able to include the axiomatic description of root data, the structure of Verma modules, and the conjugacy theorems. In recent years there have also been developments in the theory of the Virasoro algebra and its representations. A common feature of both of these algebras, as well as of the Heisenberg algebra and the contragedient algebras, is the existence of triangular decompositions. It was a paper by Rocha-Caridi and Wallach [RC-W] that led us to think about developing the book from this point of view. Indeed one of the most satisfying results of writing this book has been the realization of how much of the theory depends only on this concept and how much unity and economy are achieved by systematically adopting it at the outset. As the scope of the present work became increasingly apparent, we realized the futility of trying to encompass so much material into one volume while remaining true to the style and level of presentation that we hoped to achieve. Thus there is a notable absence of some standard theorems from finite-dimensional Lie algebras (though some of the theory is covered in the exercises). Rather we have concentrated on developing the theory of triangu­ lar decompositions and the part of the Kac-Moody theory not specific to the affine case. In fact many results of the affine case are special instances of results here; there is an extended example of the affine Lie algebra in the appendix that serves to highlight how the affine case looks and to exemplify almost everything that we discuss in the body of the text. For a guide to developments in the affine case, we recommend [Ka5] and [KMPS]. Another important omission is the remarkable representation theory of the Virasoro algebra. For more on this, the reader can consult [GO]. A secondary theme running through the book is the. subject of lattices (discrete subgroups of R" carrying an integral-valued symmetric bilinear form). Root lattices and weight lattices have long been part of the finite­ dimensional theory. They are equally important in the infinite-dimensional theory. We have tried to emphasize Lie algebra-lattice connections by introducing lattices early and keeping them in mind in subsequent sections. Since some readers will not be familiar with the finite-dimensional semisim­ ple theory, we devote considerable attention to finite root systems and their Weyl groups before getting into the infinite-dimensional theory. After con­ structing the root lattices of types A, D, E, we use the cocycle method of Garland-Frenkel-Lepowsky to construct the finite-dimensional Lie algebras of types A, D, E, complete with triangular decompositions. These serve as motivating material for the contragredient and Kac-Moody algebras. Depending on their background, readers will approach this book in different ways. Some suggestions are given in “How to Use This Book.” In

Introduction

xiii

OUI bibliography we list only works that we have referred to in the text. We apologize to the many researchers in the field whose work has not been quoted. There is a comprehensive bibliography of Kac-Moody theory by Géorgie Benkart [Bk] that covers the literature up until about 1985. Other good sources are [LMS], [FLM], and [Hu2]. Together these references provide a good view of the various ways in which the theory has developed and a good departure point for further study. We have received the help of many people in writing this book. In particular we would like to mention the continued encouragement of Stephen Berman, who never gave up hope that it would be finished, and of John Bliss, Nicole Lemire, Chen Liang, Marc Fabbri, Liu Keqin, Alejandra Premat, Jorge Valencia, and Shi Zhiyong, who patiently read through many drafts as it reached its final form. We also thank Rolf Farnsteiner for several sugges­ tions. A number of typists labored through the preparation of the manuscript. We would particularly like to thank Marion Benedict for her Tex-nical skills and her tireless and cheerful efforts. R. V. M o o d y A . PlANZOLA Burro Alley Cafe Santa Fe, NM April 1994

How to Read This Book

The book can be read from cover to cover in the order of presentation. But such an approach is not necessarily the best when background and pedagogi­ cal needs or time constraints are taken into consideration. This is particularly true of Chapter 2 which develops the theory of Lie algebras with triangular decomposition in complete generality. Many readers will probably be impa­ tient to see this theory applied to the Kac-Moody situation where it takes on a life of its own. Those readers should therefore read enough of Chapter 2 to acquire the background needed for Chapter 4, returning to Chapter 2 ás required. Chapter 3 could have been placed almost anywhere before Chapter 5. Because of the impressive and beautiful combinatorial structure of finite root systems and their logical independence from Lie algebras, the material of Chapter 3 offers an excellent beginning for a course in Lie theory. The first section of Chapter 7 provides a self-contained account of the JordanChevalley decomposition of an endomorphism both in the finite-dimensional and the locally finite (infinite-dimensional) setting. To accommodate the varying needs of the readers, we have divided the contents of the book into “blocks.” Below we show the logical order in which these blocks interact, and we outline different “courses” that can be pursued. Block A: Basics o f root systems and Lie theory— Chapters 1 and 3 Sections 1.1-1.11

Basic Lie algebra theory

{ Lattices Chapter 3

Finite root systems and their classification, construction of simple lie algebras of types A, D, and E

Block B: Basic Kac-Moody theory up to the character formulaChapters 2, 4, 6, and the Appendix Section 2.1 Section 2.2

Triangular decompositions Highest weight modules

xvi

How to Read This Book

Section 2.3 Section 2.4 Section 2.5 Section 2.6 Section 4.1 Section 4.2 Section 4.3 Section 4.4 Section 4.5 Section 4.6 Section 4.7 Section 6.1 Section 6.2 Section 6.4 Section 6.5 Appendix

Verma modules § 12-theory Characters Category ^ Contragredient Lie algebras Existence of contragedient Lie algebras Embedding, etc. Invariant bilinear forms Casimir-Kac operators Gabber-Kac theorem Hermitian forms Integrable modules Weight systems The character formula Complete reducibility An Extended example

Block C: Root data and geometry o f chambers— Chapter 5 Section 5.1 Section 5.2 Section 5.3 Section 5.4 Section 5.5 Section 5.6 Section 5.7 Section 5.8 Section 5.9

Root data The length function Coxeter groups Bruhat ordering Morphisms Geometry of root data Subroot systems Imaginary roots (uses Section 3.6) Conjugacy of bases

Block c: Basics of root data theory and geometry o f chambers— Chapter 5 Section 5.1 Section 5.2 Section 5.5 Section 5.6

Root data The length function Geometry of root data Subroot systems

Block D: Structure o f Verma modules— Chapters 1, 2, and 6 Section 1.12 Section 2.8 Section 2.9 Section 2.10 Section 2.11 Section 2.12

Extensions of modules Shapovalov form Jantzen filtrations BGG duality Embeddings of Verma modules Decomposition of modules in category Û

How to Read This Book

Section 6.6 Section 6.7 Section 6.8 Block E:

Shapovalov determinants BGG theorem Generalized character formula Conjugacy theorems— Chapters 6 and 7

Section 6.3 Sections 7.1-7.4

Triangular decomposition of the group All of the chapter

Logical dependence of the blocks Basics of Lie algebras

Basic Kac - Moody theory

Basic root data theory

C Root data theory

Conjugacy theorems

Course Outlines Course 1 Contains: Description: Comments:

Suggestions:

Block A, Sections 3.7 and 3.8 A first course in Lie theory directed towards the Kac-Moody approach This course falls short of providing the classical background in Lie algebras (e.g., Lie’s theorem and Cartan’s criterion are not present). These deficiencies can be corrected by the instructor in a one-term course. After block A is completed, Sections 3.7 and 3.8 might be used to show the relationship between lattices and Lie alge­ bras. Assignments should be designed to incorporate as much of the classical theory as possible into the course. Course 2

Contains: Description: Comments: Suggestions:

Block B Basic Kac-Moody theory up to the character formula This course is intended for students who have already covered either Block A or a course in classical Lie algebra theory (e.g., a full-year course using Humphrey’s book). Some of Chapter 3 could be assigned, especially Sections 3.5, 3.7, and 3.8. The example at the end of the book might be used as a guide for the new concepts introduced. How the classical split semisimple theory fits into this bigger picture should be made clear. Course 3

Contains: Description: Comments:

Blocks B, C, and D Basic Kac-Moody theory, geometry of root systems, and struc­ ture of Verma modules This is a full-year course. It presupposes familiarity with the material in block A or a solid background in classical split semisimple theory.

XX

Suggestions:

Course Outlines

Exploit the background of students to cover block B in one semester. Block C could prove too time-consuming, in which case block c is adequate. Course 4

Contains: Description: Comments: Suggestions:

Chapters 3 and 4 Foundations of finite and infinite root systems This course is a good complement to Course 2. It is primarily for those interested in the combinatorial aspects of Lie the­ ory. Section 5.1 should be presented in a Lie algebra free form, using examples and assignments to show connections with Lie algebras.

Lie Algebras With Triangular Decompositions

Chapter One

Lie Algebras There is no sea innavigable, no land uninhabitable —Robert Thorne, Merchant and Geographer, 1625

This chapter introduces the basic definitions and concepts of Lie algebra theory. Because it is essentially written as a primer for the subsequent material, it covers topics such as graded Lie algebras, universal enveloping algebras, central extensions, free Lie algebras, and the Campbell-BakerHausdorif formula, which often appear much later in a book on Lie theory. For the same reason it omits standard material that is historically and mathematically important but unnecessary for our purposes. Readers new to this subject might want to broaden their knowledge by consulting standard references such as [Hu] for Lie algebra theory and [Bo2] [Vj] for the Lie group/Lie algebra connection. LI

BASIC DEFINITIONS

Let K be a field of characteristic 0. By a K-algebra (or algebra over K) we mean a vector space A over K together with a mapping (x, y) xy from A X A into A satisfying x(y+z)=xy+xz,

(x+y)z=xz+yz,

c(xy) = (cx)y =x( cy) for all x, y, z ^ A and c g IK. The mapping ( x, y) xy is called the multiplication or composition law of the algebra A, and jcy is called the product of x and y. Almost always we suppress (as we have just done) all mention of the field IK since it is understood. The dimension of A is the dimension of ^ as a vector space. Much of this beginning material, especially the definitions, uses only the fact that IK is a commutative ring with identity and that ^ is a IK-module (see

2

Lie Algebras

the end of this section). Very occasionally we will talk about algebras over Z in which the underlying Z-module is free. However, this does not involve anything in the least bit profound. To keep the material here as straightfor­ ward as possible, we simply assume that IK is a field of characteristic 0. For the reader who is not an expert in field theory, it is always safe to assume that K is the field of complex numbers C. Lie algebras over arbitrary commutative rings will be treated at the end of this section. An algebra A is said to be associative if x(yz) = (xy)z for all x , y , z ^ A and is said to be commutative if xy = yx for all x, y ^ A, There can exist at most one element 1 = ^ A with the property x l = x = l x for all x ^ A. If A (0) and A has such an element, then A is called an algebra with identity element and 1 is called the identity element of A. Although we will have occasion to deal with various types of algebras, the Lie algebras (definition below) are at the center of our study. It is a long-established custom to denote the multiplication in the Lie algebra by [*, • ] and to call the expression [jc, y] the bracket or commutator of x and y. It is also customary to use lowercase old German letters^ to denote Lie algebras, and we will adhere to this convention except where common usage has established otherwise. An algebra g with a composition law [*, *] is called a Lie algebra if it satisfies the following two identities for all x , y , z in g: LAI

[ x , y ] + [ y , x ] = 0,

LA2

[ x, [ y, z ] ] + [y,[z,jc]] + [z ,[j:,y ]] = 0.

Notice that (LAI) implies that (LA3)

[x, x] = 0

for all X e g,

and conversely (LA3) implies (LAI). The identity of (LA2) is called the Jacobi identity and we shall denote its left-hand side by Jac(jc, y, z). Because of (LAI), (LA2) is equivalent to [[x, y], z] + [[y, z], x] + [[z, j c ] , y] = 0. It is useful to note that to establish that an algebra A is a. Lie algebra it suffices to verify that (LAI) and (LA2) hold for all jc , y, z in some linear basis of A. A consequence of LAI is that a Lie algebra is commutative if and only if [ jc , y] = 0 for all JC, y ^ A . The custom is to call a Lie algebra abelian rather than commutative. Clearly any vector space V over IK can trivially be made into a Lie algebra. No Lie algebra g can have an identity element. Nor can a Lie algebra be associative except under extreme circumstances. If g is a Lie algebra and jc e g, then we define the linear mapping ad j c : 9 9 by (1)

ad x( y) :=

[

jc ,

y]

for all y e g.

We will have a lot more to say about “ad” in Section 1.6. ^Gótica textura quarata, to be precise.

1.1

Basic Definitions

If {jCy}, j e J, is a basis for an algebra A, then its multiplication is completely determined by the equations XiXj= E k^J

( 2)

The scalars are called the structure constants of A (relative to the given basis). Of course it is part of the definition of a basis that all the vectors in the space A are finite linear combinations of basis elements. Thus for a given i and j only finitely many will be nonzero. Generally speaking, structure constants are not very useful for studying algebras, especially since they depend on the basis chosen. Having said this, it is only fair to point out that we will actually construct some Lie algebras directly from their structure constants. A subset A' of a K-algebra A is called a subalgebra of A if it is a K-subspace and is closed under the multiplication, that is, if xy ^ A when­ ever X, y ey l'. For example, if g is a Lie algebra and x e g, then g^ — {y e g| [y, x] = 0} is a subalgebra called the centralizer of x in g. If A is either an associative algebra or a Lie algebra, then the centre of A defined by 3 ( ^ ) '•= {x ^ A \x y = yx for all y ^ A) is a subalgebra of

In the case of a Lie algebra we have equivalently

Z ( A ) = (x e A\[x, y] = 0 for all y ^ A ) , A mapping f : A ^ B from one algebra into another is called a homomor­ phism if it is linear, and for all x , y ^ A, f(xy) = /( x ) /( y ) . One defines monomorphisms (= injective homomorphism), epimorphism (= surjective homomorphism), isomorphism (= bijective homomorphism), endomorphism (= homomorphism of an algebra into itself), and automorphism (= bijective endomorphism) in the usual way. We will also have need of antiautomor­ phisms of an algebra A, that is, bijective linear mappings a: A -> A satisfying cr(xy) = o-(y)a(x) for all x , y ^ A. For example, it is a conse­ quence of (LAI) that for Lie algebras the mapping x -> - x is an antiauto­ morphism (of period 2). A subspace J of an algebra ^ is a left ideal (respectively a right ideal) of A if for all X e / and for all y ^ A, yx E: J (resp. xy g /). A subspace that is both a left ideal and a right ideal is called a two-sided ideal, or simply an ideal. An ideal J (left, right, or two-sided) of an algebra A is called proper if J ¥=A, For Lie algebras the identity (LAI) shows that the distinction between left and right is superfluous, so there are only ideals. In the case of a Lie algebra g it is easy to see that the centre of g is an ideal of g. Let A be an algebra, and let X and Y be subsets of A. Define X Y (or [X,Y] if ^ is a Lie algebra) to be the set of all finite sums of products xy

4

Líe Algebras

where x and y e y. If ^ or y is empty, then X V •= (0), If AT or y is a subspace, then X V is clearly also a subspace. Notice that AA (or [A, A]) is always an ideal of A. When ^4 is a Lie algebra [A, A] is called the derived algebra of A and is denoted by D (^). Let A be an algebra and J an ideal of A, Then the quotient space A/J + / U ^ A } can be made naturally into an algebra by defining xy ■•=xy, where : A ^ A / J is the natural quotient map. The resulting algebra is called the quotient algebra of A by 7. The natural mapping is an epimorphism of algebras. If A is an associative algebra (resp. a Lie algebra), then so is A /J, We have just seen how an ideal J of an algebra A gives rise to a quotient algebra and a natural homomorphism of A onto A/ J . Conversely, given any homomorphism f . A - ^ B o i algebras, we retrieve an ideal in the form of k er(/) := {x ^ A \ f ( x ) = 0}. The relationship between ideals and homomor­ phism is given in the standard type of way: Proposition 1 Let f:A B be a homomorphism o f algebras, and let J be an ideal o f A and :A A / J the natural mapping. I f J ^ ker{f), then f factors through J. In other words, there exists a homomorphism g : A / J B that makes the follow­ ing diagram commute: A

B

A /J The mapping g is unique and its kernel is (k e r(/))//. In particular, if J = ker(/), then g is a monomorphism. □ If {Aj\j e J} is a family of algebras then the K-space ® j ^ j A j may be given the structure of a IK-algebra by defining a multiplication via (

==

for all Oj, bj ^ A', j ^ J

(each sum contains only finitely many nonzero terms). This algebra is called the direct product of the algebras Aj and is denoted by (or A^ X ••• X if J = {1,..., n}). Note that this definition does not coincide with the categorical definition of the direct product Tlj^jAj, which we will not need. Many authors use the notation ®j ^ j A j and call it the “direct sum of the algebras.” We prefer not to use this notation because it is not uncommon to be in a situation in which we have a direct sum (in the ordinary vector space sense) of subalgebras of an algebra that is not a direct product. An algebra A ¥= (0) is usually called simple if it has no ideals except (0) and itself. In the case of Lie algebras the trivial one-dimensional Lie algebra is excluded, and the definition can be restated: g is simple if it has no ideals

1.1

Basic Definitions

different from (0) and itself and if [g, g] = G- We will say that a Lie algebra g is semisimple if g is isomorphic to a direct product of simple Lie algebras. Throughout the rest of this book we will make the following assumptions on associative algebras: AAl. Any space referred to as an associative algebra is assumed to have an identity element. AA2. Any subalgebra of an associative algebra A is assumed to have an identity element, and this identity element is the same as that of A, AA3. All homomorphisms between associative algebras are assumed to carry identity elements to identity elements. According to AA2, proper ideals are not subalgebras [an ideal (left, right, or two-sided) of an algebra A that contains the identity element of >1 is ^ itself]. When we speak of the subalgebra of A generated by a subset 5 of we mean the smallest subalgebra of A containing S and 1^. Notice that because of AAl, any associative algebra has a copy of the base field K as a subalgebra. If A is an associative algebra over IK then an A-module is a vector space M over K and a bilinear mapping A X M ^ M, {a,m) ^ a - m, satisfying {ab) • m = a {b • m) 1'm =m for all a,b Ei A, m E: M. Example 1 {n X n matrices) Let MJiK) denote the set of n X n matrices with entries in the field K. Then M„(IK) is a vector space over IK in the usual way, and it becomes an associative IK-algebra with identity when multiplica­ tions is taken as the usual matrix multiplication. Example 2 (Algebra of endomorphisms) The vector space Endj^(F) of IK-linear transformations of a vector space V over IK into itself becomes an associative K-algebra by defining fg = g (composition of mappings) for all f , g ^ End|,^(K). If V is of finite dimension n, then Endj^(F) and M„(IK) can be identified by fixing a basis of V. Example 3 (Lie algebra of an associative algebra) Let A be an associative K-algebra. Consider the mapping [*,•]: A X A A defined by [x,y] xy - yx, where xy is the product of x and y in A. Then A, taken as a vector space together with this new composition law, becomes a Lie algebra. Only the Jacobi identity is not immediately clear. We have Jac(o:,y,z) = [ x, y z - zy] + [ y, z x - xz] + [ z , xy - yx] = xyz —xzy — yzx + zyx + yzx — yxz — zxy + xzy -\-zxy - zyx - xyz + yxz = 0. This algebra is denoted by Li&(A) and is called the Lie algebra of the associative algebra A.

6

Lie Algebras

Example 4 (General linear algebra) If in Example 3 we set A = End(F) for some vector space V over K, then Lie(^) is commonly denoted by gI(F) and called the general linear algebra of the vector space V, Any Lie subalgebra of- qI(V) is called a Lie algebra of linear transformations (of V). If dim(K) = Az is finite and a basis of V is chosen, then we can identify End(F) with M„(1K). We will denote Lie(M„((K)) by gI„(IK). Example 5 (Special linear algebra) Let ^I„(1K) = [X ^ M„(IK)|tr(A!') = 0}. It is well-known (and easy to verify) that if X and Y belong to M„(K), then tr(AT) = tx(YXl Thus tT([X,Y]) = t i (XY - YX) = 0. As a consequence §I„(IK) is a subalgebra of gI„(IK); indeed [gI„(lK), gI„(IK)] c §I„(1K). Let 1„ denote the identity of Then for all X e M„(IK) we have

Z = i(tr(Z ))l„ + | z-^ tr(Jf)l„J so that gI„(lK) = IK1„ © §I„(1K); in fact gI„(IK) = X §I„(IK) (direct prod­ uct of Lie algebras). Clearly dim §I„(IK) = - 1. The Lie algebras of type §I„(1K) are called special linear algebras. Notice in Example 5 that though ^I„(IK) is closed under brackets, it is not closed under usual matrix multiplication whenever n >2. In particular ^I„([K) is generally not a subalgebra of M„(1K) even if we disregard our convention about existence of identities in subalgebras. This already shows that if we have an associative algebra A, we cannot expect the Lie substruc­ ture of Lie ( ^ ) to be a simple reflection of its associative substructure. Every subalgebra of an associative algebra gives rise to a Lie subalgebra of the associated Lie algebra, but not vice versa. However, we will see in Section 1.8 that any Lie algebra is a subalgebra of Lie {A) for some associative alge­ bra A. Example 6 (§I2(IK)) The three-dimensional Lie algebra ^l2(IK) plays a fundamental role in Lie theory. We fix the following standard basis for ^l2(K):

‘ “ (2 i)’

o)' '■"(J -W

Simple calculations give [/ze] = 2e, [hf] = - 2f , [ef] = h.

1.1

Basic Definitions

7

Notice in particular that e, f , h are eigenvectors for ad h with eigenvalues 2, - 2,0 and thus that ^I2(1K) = IK /0 Kh 0 Ke is an eigenspace decomposition of §I2(IK). Using this, it is straightforward to show that is simple. In fact §I„(IK) is simple for all n >2. This is also not hard to prove directly, but we will see it later in a wider context. Example 7 (Quaternions) Let H be the usual real quaternion algebra: H = Kl 0 Ri 0 Uj 0 Uk with ij = k = —ji, jk = i = —kj\ ki = j = —ik, H is well-known as the simplest example of a noncommutative associative algebra which is a division algebra (every nonzero element has a multiplicative inverse). Observing that for Lie(H) we have L L 2 ’2

k 2’

L i 2 ’2

i

k i

J

2’

2 ’2

2’

and [1,R/ 0 Ry 0

= 0,

we see that u — R/ -h R; -h RA: is a subalgebra of Lie(lHI) isomorphic to R^ with the standard vector (cross) product and Lie([H) = R1 X u.

Example 8 (Geometric description of ^l4(R)) Let Si,S2, S2 be an or­ thonormal basis for the euclidean 3-space E, and let A ==

i Sj\i # yj c

+ Zc2

^^3*

These 12 vectors define the vertices of a cube-octahedron as shown below. The edges join those pairs of vertices {y, 5} for which y • S = 1. One may observe that for such a pair, y — 8 (and 5 —y) e A also. Thus 6 = (5 - y) + y is the sum of two elements of A. In fact every pair {a, 0} such that a + /3 e A is of this form: a

0

2 = ( a + j 8 ) - ( a + j 3 ) = a * a = ) 3 - j 8 = > a - j 3 = —1.

Lie Algebras

Then a • (a + p) = 1 and ((a + j8) - a) + a = a + )8. In this case we de­ fine

(1

if the edge from a to a + /3 is positively oriented,

- 1 otherwise. We construct a Lie algebra g as follows (see Figure 1.1): As a vector space, g is a 15-dimensional vector space with basis S2, £3, and a set of 12 linearly independent vectors indexed by the a e A. Identify E with the span of £1, 82, ^3 in g. The Lie bracket is defined by

( 3) ( 4)

[ e , ,e j = 0

fo ra lli,/,

= isra)X,

[e,,Xj =

j'sgn(a,/3)A'^+^

( 5)

[ X^ , X^ ] = l - a ^ E

\0

ifa + ^ e A , ifi3=-a, otherwise.

The reader need not worry about verifying the Jacobi identity. We will do it more generally later on. In fact g = §14(1^). The point of the example is to see how remarkably the Lie algebra is related to an intrinsically beautiful geometric object. This is not a fortuitous accident. There are whole families of similar examples which we will take up beginning in Chapter 3. Remark 1 There is no compelling reason for restricting the definition of algebras to K-spaces. For example, in Section 3.4 we will encounter Lie algebras over Z.

1.2

Tensor, Symmetric, and Exterior Algebras

9

In general a Lie algebra over a commutative ring A is an ^-module M together with a bilinear map [•, ]: M X M ^ M satisfying conditions (LA2) and (LAS) above. [Note that (LAI) and (LAS) need not to be equivalent.] The concept of an arbitrary algebra over A is defined along the same lines Another abstract construction that we will encounter is that of extension of the base ring. Let M be a left ^-module, and let B be a ring containing A. Consider B as a right ^-module and form the tensor product B (S)^ M. This has a natural left 5-module structure satisfying X ' { y

^

m )

=

xy

^

m ,

which is called the 5-module obtained from M by extension of the base ring from A to 5. If M is an ^-algebra and 5 is commutative, then the 5-module B <S>^M has a natural 5-algebra structure satisfying ( j c 0 m ) ( y 0 n )

=

xy

(S> m n .

The most common occurrence of this is when ^4 is a field and 5 is a field extension of In this case if is a basis of M over A , then we can think of 5 as the 5-space with the same basis. Finally, if A and 5 are as above and M is a 5-module (resp. 5-algebra), then by restriction of scalars from 5 to >1 we give M an ^-module (resp. y4-algebra) structure. i.2

TENSOR, SYMMETRIC, AND EXTERIOR ALGEBRAS

Let us begin by constructing, in an obvious way, the polynomial ring in a number of noncommuting variables. To this effect let X = be a set of symbols. By a monomial in X we will understand an ordered sequence or string Xj^Xj^ • • • Xj^ of (not necessarily distinct) elements of X. We let M = M i x ) be the set of all monomials in X and make the following conventions: 1. The empty monomial (i.e., the string with no elements) belongs to M. This monomial is denoted by 1. 2. If equal consecutive symbols appear in a monomial, then these can be grouped together according to the usual exponent notation; for exam­ ple, we will write jc,J \ jcfJ l jc,j \ jc,J 3 instead of x,J l jc,J 2 X:J 2 jcJ,2 X:J] X:J 3 (but X:j \ jc,J 2 jc,j \ ^ ^ ’ ^ hV J 2 if a

Lie Algebras

10

We now define a multiplication • on M by juxtaposition. Thus given monomials m = jc,J l X:J 2 x,f, we can obtain a new monomial XjJp and m' = XfJ l XfJ l m m = XjXj^ XjXjfXy^ • • • Xy/ called the product of m and m'. This multiplication is obviously associative, but not commutative if card J > 1. The empty word 1 acts like an identity in the sense that m • 1 = m = 1 • m for all m e Af. M i x ) is called the free monoid on X, If N is any monoid and f : X - ^ N \ s any map, then there exists a unique extension of / to a monoid homomor­ phism /: M i x ) N, namely fixj^ • • • Xj) = fixj^) • • • f i x j ) . Now let A i X ) be the K-space admitting M as a basis. Then every element of A i X ) can be written uniquely as a finite linear combination of the form

where the a,^’s e IK and the m^’5 g M. We next define a multiplication on by bilinear extension of the multiplication on M; in other words, ( E «,«>,) • (E&yn»>) = E«,Am< ■"*;• Thus defined, A i X ) is an associative algebra (the element 1 is its identity). ^(AO is called the free associative algebra generated by X. Intuitively we may think of A i X ) as being built out of linear combinations of products of elements of X subject to no other constraints than the resulting structure be an associative algebra. The precise definition of a free associative algebra is the following: Let AT be a nonempty set. A free associative algebra on X over IK is an associative algebra A together with a mapping i:X A such that for every associative algebra B over K and every mapping f :X B there exists a unique homomorphism f : A - ^ B such that In other words, the diagram

A

/ / B

commutes. Note Recall that our conventions on associative algebras are in force. A well-known example of a free associative algebra is the polynomial ring K[x] in one variable. If A is any ring containing IK (which amounts to saying that A is an algebra over IK) and a ^ A is arbitrary, then there exists a unique homomorphism IK[x] A such that x ^ a, namely the one given by i;c ,x '

E c ,a '.

1.2

Tensor, Symmetric, and Exterior Algebras

U

It is easy to see that the algebra A{X), as constructed above, together with the identity map id: X A ( X ) is a free associative algebra on X. If A is any associative_ algebra and f : X A is any map, then there is a unique linear mapping / : A ( X ) -* A defined by • • ■^ 0 = f ( ^ h ) • • • f ( ^ 0

/(1 ) = 1-

It is trivial to see that / is a homomorphism of algebras and that /« i d = / . Now we will show that (>l(Ar),id) is unique in the following sense: If {A', i') is another free associative algebra on X , then there exists a unique isomorphism g:A{X) such that the diagram A{X)

commutes. The argument used to prove this is a very standard one that follows more from the form of the definition of freeness rather than the particular context of associative algebras. (More precisely it is a result about universal objects in categories.) We write down the argument here to serve as a model for all future occasions when universal objects are defined. Let {A, ¿X ( A , V) be any two free associative algebras over X. Using the definition of freeness on A and A in turn, we find unique homomorphisms g: A A , g': A ^ A such that both inner triangles in the diagram

commute. Thus the outer triangle of mappings X \ g ^8

is also commutative. On the other hand, the diagram

id

commutes. The definition of freeness says that only one homomorphism k: A ^ A exists, making the diagram X — ^ A

commutative. Thus g' °g = id^. Likewise g^ g' = id^r, and we have g' = g~^, proving that g is an isomorphism. Return to the initial construction of A(X). For each n e we let M%X ) denote the set of monomials involving precisely n symbols; for example, X: Xi X: X J J\

J2

Jl

J3

M \X ),

w hilel e

For each n e Z define m|in € M " (A r),a ,

A%X) =

if « > 0, if n < 0.

1 ( 0) Then A{X) = © A \ X ) , and evidently A^{ X) A^{ X)

for all m and n in Z. We will see in Section 1.3 that this means that A{ X) is graded by Z. We will make frequent use of free associative algebras in the sequel, often in the following way: Let V ¥= (ff) be a IK-space with basis [Vj}j^j, and construct the algebra A ( X ) as above. We can now identify K as a vector subspace of A ( X ) via the injective linear map defined by Uj •-> Xj. In this way we can think of A{ X) as being an associative algebra constructed out of V. We denote this algebra by T{V) in order to emphasize the identification between V and the K-span of Xy’s. If we do so then T{V) can be thought as being the space whose elements are finite linear combinations of the form

1.2

Tensor, Symmetric, and Exterior Algebras

13

where the belong to K. The algebra T(V) is called the tensor algebra of V. For all n ^ Z the linear span of the monomials involving precisely n elements of V form a subspace T%V) =A%X) . Of course the way in which we have constructed T(V) is basis dependent. It is not hard to see that a different choice of basis leads to a naturally isomorphic object. (See below for a basis-free constructing of T(V).) The construction of the free associative commutative algebra K[X] on a set X = {Xj}j^j is completely analogous to that of A ( X \ but we now allow the X:’s to commute. For example, x,- x,- x,- and x f x f x : will now be one and the same monomial. (Formally M is now the free commutative monoid in X and K[X] its algebra over K.) Of course K[X] is nothing but the familiar polynomial algebra over IK in the (commuting) variables Xj, j e J. If < is a total-ordering in J, then the set of monomials { X:J l X:J 2

X j \ j \ < j 2 ^ ■■■ <j „;n

is a basis of the IK-space K[X], The universal nature of K[X] is formally expressed as follows: Given any map / from X into an associative commuta­ tive algebra A, there exists a unique homomorphism / from IK[A"] into A such that the diagram X f

commutes. Moreover K[X] is, up to isomorphism, the unique associative commutative algebra with this property. The homogeneous monomials of degree n generate a subspace K[ XT of K[ Xl Clearly

Finally, notice that K[X] can be thought as a quotient of A(X): More precisely K[X] - A ( X ) / J , where J is the ideal of A ( X ) generated by all elements of the form XjXj^ - Xj^Xj^ with j\ and j'2 in J. Suppose now that V =5^ (0) is a IK-space and that j ¡s a basis of K As before, we can identify V with a subspace of IK[A"]. If we do so, then the elements of 1K[A!'] can be thought of as linear combinations of the form Jl,J2y-yJn but where now UjUj^ = VjVj^ for all ^ J* When emphasizing this corre­ spondence, we will write 5(F ) instead of 1K[A"], and call this algebra the symmetric algebra of F. As before, one can easily see that up to isomorphism this construction is independent of the choice of basis.

Lie Algebras

14

The descriptions we have given of T{V) and S(V) are sufficient for most of our purposes. We will, however, assume at certain points in the text that the reader is familiar with the concept of balanced maps and tensor products of modules over noncommutative rings. (We have already used this assump­ tion in Remark 1.) In this language we have the following (basic free) constructions of the tensor, symmetric, and exterior algebras. If ^ is a commutative ring and M is an ^-module, we let, T ^ ( M) = M ®

‘ 0 M,

p-times, p > 0,

T ( M) = © r ^ ( M ) . p > 0

This last is the tensor algebra of M where the algebra structure is given via the canonical isomorphism T ^ ( M) 0 T^ { M) = Let J be the two-sided ideal of T(M) generated by all elements of the form X 0 y - y 0 jc, jc, y e M. This is a graded ideal and hence S{ M) : = T { M ) / J = © 5^(M ), p > 0

where S^{M) ^ T ^ { M ) / J f l T ^ ( M) (see Section 1.3 for gradings). 5(M) is the symmetric algebra of M. Finally, if I is the ideal of T(M) generated by all elements x 0 x with X e M, then I is graded and the exterior algebra A(M) of M is defined by A (M ) = T ( M ) / L Then A ( M ) = © AP(M) p^O with A^i M) = Tf>(M)/U n r^(M )).

1.3

1.3

Gradings

15

GRADINGS

In this section we introduce the concept of graded algebras. Gradings appear in every aspect of this work and are fundamental to the subject. In fact, once we move away from the traditional finite-dimensional theory of Lie algebras, there are few established ways of pursuing the subject. Either one assumes that the Lie algebra carries some topological structure, or one assumes that it carries a grading or at least a filtration. In this book we depend on gradings, usually with the degree spaces being of finite dimension. Let K be a K-space and Q an abelian additive group. By a grading of V by Q we will understand a family eq subspaces of V such that V=

© F “. a^Q

Given such a grading, we will say that V is graded by Q or Q-graded. For each Of e 0 we call F “ the degree subspace^ of degree a. If i; e Ei;“ ^ F, i;" e F “, then is called the homogeneous component of v of degree a. An element lying in a degree subspace F “ is said to be homogeneous (of degree a). Notice that in this sense 0 is homogeneous of every degree, whereas a nonzero element of F can be in at most one degree subspace. The fact that (2 is a group comes into the picture when we consider graded algebras. Let A be an algebra over K, and let {A^}^^ q be a ^-grading of A (as a vector space). We say that the grading is compatible with the algebra structure of A and that ^4 is a Q-graded algebra if A^A^ (z A ^^^

for all a ,p ^ Q .

Assume that A is an algebra graded by Q and that F is an ^-module that is also (2-graded. These gradings are said to be compatible if c

for all a ,p ^ Q .

In this case we say that F is a graded ^-module. Referring to Section 1.2, we see that A(X) = © A \ X ) T{V) = © r"(K ) neZ

K[AT] = © K'-iA'] neZ

5 ( F ) = © 5 " (F ) neZ are all Z-graded algebras. These gradings are called the total gradings. ^We avoid using the terminology “ homogeneous subspace” because this concept has an entirely different meaning elsewhere in mathematics.

Líe Algebras

16

In the case of A{ X) or K[X] there is another obvious grading available. Let X = and let Zj := © Z,be the direct sum of card(J) copies of Z. Let aj e Zj be the element whose yth component is 1 and all other components are 0. Given a monomial "*

■■■

we assign to it a degree: deg(m) =aj^ +

+aj^ e 2 j.

Evidently for all m, n e M(AT), deg(ni • n) = deg(m) + deg(n). It follows that if we define A “( X) to be the linear span of all the monomials of degree a, then A { X ) = 0 ^ “(AT) aeZj and A{ X ) is Zj-graded. In precisely the same way IKlAf] is Zj-graded. However, T(V ) and 5(F ) cannot carry a natural Zj-grading since they are, in principle, free of any particular basis. If A is any <2-graded algebra and 0 is the identity element of Q, then for all a ^ Q , ( 1)

In particular A^A^ c A^. If A is associative with identity element 1, then \ EiA^ (Exercise 1.4). Thus in all cases A^ is a subalgebra of A. Let V and W be (2“graded IK-spaces where Q is an abelian group. Let A e g . An element / g Homn^(K, is called homogeneous of degree A if / ( F “) c W A + a for all a e g . Define Homn^CF, W Y to be the K-subspace of Hom,K(F, W ) consisting of homogeneous elements of degree A and

grHomK(F,IF) := L HomK(F,IF)" cHomK(F,IF). This sum is direct. Indeed, if

e Homu^CF, W)^ and Exeg/A = 0 (sum with

13

finite support), then for

Gradings

17

e F" of arbitrary degree a e ¡2 we have 0 = L /x(i^a)A

But

e

so that

= 0 for all A e g . Thus

grHomK(K,»^) = e

H o m ^ (F ,lT ) \

but notice that in general grHoni|,^(F, PF) c Honi|,^(F, PF) if V is infinite dimensional. If /: F PF is homogeneous of degree 0, we say that / is a graded homomorphism. Example 1 Let F be a 0-graded K-space. View K as a (2-graded K-space via = K K“ = (0)

if a ^ 0.

Then grHomo^(F, IK) c F* and grHom„^(F, K) = { / G F * |/ ( F “) = (0) for all but a finite number of a e 2}. It is customary to denote grHom„^(F, K) by restricted dual of F. Of course

or g rF * and call it the

^es = e Kts Ae0 where F4 = H om j,(F \K ) = (F")*. Example 2 Let F be 2-graded. Let gr E n d F ):= gr Horno^(F, F). If / e End,^(F)'>' and g g EndK(F)^ then for all a e 0 /g ( F “) c / ( F “ ‘^®) c

r)

so that fg G Endi^jiF)’"^®. This shows that grEndi^íF) is a 0-graded alge­ bra. Similarly [/, g] = fg - g f ^ End^(F)’'+® so that Lie (grEnd^íF)) ~ gr qK F) is a 2-graded Lie algebra.

Lie Algebras

18

Let

be a subspace of a Q-graded space A. For each a ^ Q define C\ B. We say that 5 is a graded subspace of ^ if B (the sum is necessarily direct). To say that B is a graded subspace of A is equivalent to saying (2)

whenever a = ^ a^Q

^ B,

then each homogeneous component

E: B,

That is, if B is graded and a = e B, then a can be written in the form Eb“, where e B°^ = A^ C\ B. Thus e B for all a. Conversely if (1.9) is true, then e A"^ C\ B a e EB“. Thus B = EB “. If i? is a graded subspace of A , then the quotient space A / B has an inherited grading with { A / B Y := {A^ ^ B ) / B = {a +B\a e A ^ ) / B. The point is that if Eiz“ Thus

B = B, then E a“ e B, so each

e

B by (2).

A/B = © {A/By, In addition the natural mapping A^ ^ {A^ + B ) / B has kernel A°" r \ B = J?"; thus A ^ / B ^ =- {A^ + B ) / B = { A / B Y , Let A = © ^ g g ^ “ b e a graded algebra. A 2-sided ideal / of ^ is called a graded ideal if / is a graded subspace of If / is a graded ideal of A, then the quotient space A / J = ®^^sq ( ^ / / ) “ is graded in a way compatible with its algebra structure: {A /J)\A /jY ^{A /J)

a+/3

If 5 is any subset of homogeneous elements of A, then both the subalgebra and the ideal of A generated by S are graded. We leave this as an exercise (also see the next example).

1.3

Gradings

19

Example 3 Consider the free associative algebra A ( X ) with its total grading. Let J be the ideal of A ( X ) generated by all the commutators x^Xj - XjX^, i, 7 e J. A typical element of / is a finite sum s=

Y. aij{XiXj-XjXi)bij,

where and ^ A ( X ) . Evidently j;,0Cy - XjXf is homogeneous of degree 2. Let Oij = ^ A ( X ) " , and similarly let = T,bjp. Then we can further decompose 5 as a sum of elements - XjXi)bjf, which are homogeneous of degree m + n + 2 and which are also in J. This shows that J = so / is a graded subspace, hence a graded ideal. Then A { X ) / J = IK[Ar] inherits the Z-grading with { A{ X) / j y = { A \X ) + /)//. One ej^ects that K[X] will end up with its standard Z-grading. Indeed it does: Let : A ( X ) A ( X ) / J be the natural quotient homomorphisni. Since A^^(X) is spanned by the monomials m = ♦ Xy, j \ , . • •, Jn ^ { A { X ) / J Y is spanned by the monomials Xj^ • ** Xy, which are precisely the elements of the free commutative associative algebra that generate the subspace of degree n. Let F be a (2‘graded space. We give the tensor algebra T(V) of F a ¡2-graded algebra structure as follows: Given a ^ Q define T ^ ( V) :=

52 F “* ® a, + ••• +a„=a

® F “" =

© Of, + ••• +a-=a

® • • • <8) F “"

(where by convention the right-hand side is IK if n = 0). Then the sum of the r “(F ) is direct and r ( F ) = © r “( F ) a^Q is the desired j2-graded algebra structure on T(F). This is said to be induced from F.

20

Lie Algebras

The defining ideals of both the symmetric and exterior algebras are homogeneous, so we obtain ¡2-gradings S ( V) = © 5 “( F ) a^Q and A ( V ) = © A "(F). a^Q

1.4

VIRASORO AND HEISENBERG ALGEBRAS

In this section we introduce the Virasoro algebra, which is a unique object (for a given field IK), and the Heisenberg algebras, which are a special class of nilpotent Lie algebras. These algebras are quite important in contemporary physics and provide excellent examples of graded Lie algebras. To make the definitions seem less arbitrary, and also to see how Lie algebras appear naturally as algebras of operators, we give explicit realizations of the centre­ less Virasoro and the finite-dimensional Heisenberg algebras. Let X = be an infinite-dimensional vector space over IK with basis {L„}; « e Z. Make X into an algebra by defining multiplication through for all m^n ^ Ж.

= { n - m)L„

It is trivial to check the skew-symmetry and the Jacobi identity on this basis, so AT is a Lie algebra. We call this algebra the Witt algebra or centreless Virasoro algebra and denote it by SB. The Virasoro algebra S3 is a one-dimensional central extension of SB (see Section 1.9 for central extensions). Define ss = a: 0 iKc, and define multiplication by (la) (lb)

[L ^ , L„] = (n - m )L„+„ + [c ,L „ ] = [ L „ ,c ] = 0

f o r a llm ,n e Z .

Here d is the Kronecker symbol. If m - n , then bracket of and L„ is exactly as it was before. The mysterious 1/12 is irrelevant at this point. By using a basis ^ where a is some nonzero scalar, one can replace the 1/12 in (la) by any other nonzero constant.

1.4

Virasoro and Heisenberg Algebras

21

The verification that 83 is a Lie algebra is straightforward. For example, if m + n + /? = 0 and m, n, p 0, then Jac{L^, L„, Lp) = ( p - n)[L„,L„^p] + (m - p)[L„, Lp+„] + (n - m)[Lp,L„+„] = { ( p — n) ( n

p — m) + ( m —p ) ( p

m — n)

+ (n —m) { m + n - p ) } L q + ^ { ( P - n){m^ - m) + ( m - p)(n^ ~ n) + (n - m )(p^ - P ) ] c =

0.

Although SB is a subspace of S3, SB is not a subalgebra of S3. However, we have an epimorphism 7t : S3 ^ SB defined by H^n)=Ln,

tr(c)=0.

This gives rise to the exact sequence of Lie algebras (2)

0

Kc ^ S3 ^ SB

0.

Obviously IKc is in the center S3. In fact it is the center. That is, if La„L^ + ac is central, then 0 = [L^,La„L„ + ac] = La„{n -

“ >n)c

for all m e Z, and it is clear then that all the a„’s are 0. From the point of view of the representation theory it is S3 and not SB that arises. S3 and SB display obvious Z-gradings, namely SB" = KL„ S3" =

for all n,

IKL„ IKLq 0 IKc

if Az ^ 0, if n = 0.

It is interesting to see how the Witt algebra arises naturally when one considers the space SB (over C) of complex vector fields on the unit circle U := {e'^\6 0 U}. Each vector field is a linear operator fd/dO on the space

22

Lie Algebras

S (t/) of complex valued C*-functions on i/. since

( 3) Indeed, if

d

d

is a subalgebra of 9l(^(i/))

(fdg/dd - gdf/dd)d

dé e §((/), we obtain d

d

d I dh\

dg dh

d^h dS^ ’

d

d f dh

d^h

^de^de

^de de

r _ __ f de jn de jtk

and similarly d

de^'

Then (3) follows from subtracting these two equalities. Let SB be the subspace of vector fields fd/dO for which / has a finite Fourier series expansion e C, A: e Z. Then SB has a basis

and [ L „ L j ] = - i{ e ‘V ^ d / d e - e‘^‘>ke“‘^) — = {j - k)L^^j , showing that SB is indeed a Witt algebra. Next we introduce the concept of Heisenberg algebras. Suppose that a is a Lie algebra over K admitting a one-dimensional subspace c with the following two properties

( 4)

[ a , a ] = c,

( 5)

[ a ,c ] = (0).

Then if {c} is a basis of c, we have an associated skew-symmetric bilinear form iff on a defined by

( 6)

[x, y] =

y)c

for all X, y e a.

1.5

Derivations

23

Clearly c lies in the radical of
DERIVATIONS

Let ^ be a K-algebra. A linear map 8: A it satisfies the following familiar rule: ( 1)

5(;0') = x 5 (y ) + 5 (x )y

A

called a derivation of A if

for all x, y e yl.

24

Lie Algebras

Notice that if 5 e End(^) satisfies (1) on all pairs (x, y) where x and y run through a basis of A, then 8 must be a derivation. It is simple to see that the composition of two derivations is not necessarily a derivation. However, as the following computation shows, their commutator always is [5 ,5 '](ry ) = 5 (5 '(j^ )) - 5'(5(jry)) = 5(A:5'(y) + S'(;c)y) - 5 '(x 5 (y ) + 8 ( x ) y ) = x8{d' {y)) + 8( x) 8' ( y) + 5'(;c)5(y) + 5 (5 '(^ ))y - A;5'(5(y)) - 8' {x) 8( y) - 8 ( x ) 8 \ y ) - 8' {8( x) ) y = a:[5,5'](y) + [5 ,S '](x )y . Thus the space Der(/1) of all derivations of ^ is a subalgebra of the Lie algebra Qi(A). If an algebra A is anticommutative [i.e., if (LA3) holds], then the Jacobi identity (LA2) holds in A (and A is therefore a Lie algebra) if and only if for all X e ^ the map 1/. y xy (i.e., left multiplication by a:) is a derivation of A. Thus, if g is a Lie algebra, and if for each j: e g we define ad a:: g g by ad

a::

y

y],

then ad a : is a derivation of g. Moreover the map ad: a : -» ad a: is a Lie algebra homomorphism from g into Der(g) (we will return to ad in Section 1.6). Example 1 Let A — 0^^g.<4“ b e a graded algebra, and \e,t d: Q -* K any group homomorphism (of additive groups). Define 6: A ^ A by linear extension of 5: ac„ •-> d{a)x^ for all ac„ e A “, a ^ Q. Then 5 is a derivation of A. Indeed, if a:„ e A “ and x^ e A^, then x^x^ e Therefore

= ( d ( a ) + d(p))x„Xp = d{a)x^Xp + d (^)x „ x p = x^{d{P)Xp) + {d(a)x^)xp = x„8{xp) + 8(x„)xp

Example 2 Let A be an associative algebra. For each y ^ A the map A^: A ^ A given by Ayi x ^ yx —xy is a derivation of A. Derivations of this form are called inner derivations of A.

1.5

Derivations

25

We recall for later use the following result: Proposition 1 Let Vbe a K-space, Т(У) its tensor algebra and S(V) its symmetric algebra. Then (i) given any linear map f: V ^ T(V), there exists a unique derivation 8= of T(V) making commutative the diagram T { V)

T { V)

(ii) statement (i) holds if T(V ) is replaced by S{V). Proof. Let {vj)j^j be a basis of V. Then recall that T(V) can be thought of as the polynomial algebra IK[f;]; ey in the noncommuting variables Vj. Recall also that the set of monomials on the v/s (including the empty monomial 1 e K) form a basis for the IK-space T(V). Hence the map defined on these monomials by ( 2)

5/(1) = 0,

( 3)

5/( Vj) = / ( Vj)

for all j e J,

n

(4)

••• О

= Г t'y. ••• k= l

• ^Jr,

for all admits a unique linear extension (also denoted by 5y:) to an endomorphism of T(V). It is clear that 8^ is a derivation that satisfies the required property. As to its uniqueness, notice that for any x ¥= 0, 8jr(x) = 5yr(lx) = 8f(x) + 5y^(l)x => 6y^(l) = 0. On the other hand, if the diagram above is to commute, then necessarily 8f(vj) = f(vj). This leaves no choice, but (4) if 8jr is to be a derivation. This concludes the proof of (i). To establish (ii), we observe that 8jr stabilizes the defining ideal J (ZT(,V) of 5(K). Thus 8f induces a derivation of 5(K) with the required properties. □ Remark 1 Let {Vj)j^j be a basis for a K-space V. Fix an index e /, and consider the functional / e F* given by linear extension of /: Vj^ 1,

Líe Algebras

26

/: Vj ^ 0, if j ^ Jq. Proposition 1 then shows that the usual partial derivative is a derivation of the (commuting or noncommuting) polynomial algebra An endomorphism / of a K-space V is called locally nilpotent if for each V Ei V there is an n = n{v) e N such that /"(i;) = 0. If / is locally nilpotent, Ei V, and n := maxinCfi),. . . , «(¿;^)}, then /" ( f ) = 0 for all v in the linear span of Thus if dim F < oo, a locally nilpotent endomor­ phism of V is actually nilpotent: /" ( F ) = {0} for some n. If / e End(F) is locally nilpotent, then 00

fn

E — is a well-defined endomorphism of F. It is called the exponential of /. Proposition 2 Let f, g E End(F) be locally nilpotent, and suppose that fg = gf. Then f + g is locally nilpotent and ex p (/ + g) = exp / exp g.

Proof. Let

V

e

V,

and find N

e

H

such that

since in each term of the sum either ; > is locally nilpotent, and we have

( f ^

g

) ^

£ — - — (v) n= 0 ”• 2 N - 2

=

= 0 = g ^ { v ) . Then

or 2A/^ - ; - 1 > AT. Thus / + g

2 N - 2

ex p (/ + g ) ( y ) =

f^{v)

„ =0 N - l

i:

j + k = n

f j

N

- \

f j

g k

L

!<' •

g k

= L ^ E fr(^) j=0 L

A:= 0

= e x p /e x p g (z ;)



1.5

Derivations

27

The conclusion of Proposition 2 is false if / and g do not commute. The question of whether we can write exp / exp g = exp( /z) for some h is difficult and fundamentally related to Lie theory. Formally the answer is yes, h being determined by the Campbell-Baker-Hansdorff formula (see Section 1.11). This gives /z as a series / + g + ^ [/, g ] +

** higher commutators products of / and g,

which unfortunately need not converge in End(K) ([Bo2] Ch. 2.7). In the preceding proof we have explicitly mentioned the index N = N(v) for which f ^ ( u ) = 0. This index will be omitted in the sequel. The reader ought to keep in mind that the sum T!^^Qf\u)/n\ is finite for all z; e K whenever / is locally nilpotent. Proposition 3 Let 8 be a locally nilpotent derivation o f an algebra A, Then exp(5) is an automorphism o f A. Proof It is fairly simple to show, by induction on n, that 8 satisfies the usual Leibnitz rule ^ 8\x) ;=0 for all x , y ^ A and n

j'

. We now have 8’’( x )

exp S(x)exp 8( y) = \ £

' y

..=0

[P = 0

/

^ /

= E n =0

\;=o

8"(xy) = E « = 0 n\ = exp 5(xy).

J'-

(« -/)!)

00

(Leibnitz)

We conclude that exp 8 is an endomorphism of To show that it is invertible, we produce its inverse, namely exp(-S) (see Proposition 2). □ Now let g be a Lie algebra. We say that a derivation 5 of g is inner if 5 = ad X for some x e g. (Recall that ad x e Der(g) for all x e g). We call

28

Líe Algebras

an element x ^ Q ad-nilpotent (resp. locally ad-nilpotent) in case ad jc is a nilpotent (resp. locally nilpotent) endomorphism of g. By Proposition 3, if X e g is locally ad-nilpotent exp(ad ;c) belongs to the group Aut(g) of all automorphisms of g. The set E := {exp(ad x)\x ^ q; x locally ad-nilpotent} generates a subgroup A u t/g ) of Aut(g). The elements of Aut^(g) are called elementary automorphisms of g. Notice that E is closed under inversion (exp(ad x)~^ = exp(-ad x)) but that E is not generally closed under multi­ plication.

1.6 REPRESENTATIONS We have previously seen several examples of Lie algebras “represented” as Lie algebras of linear operators on some vector space V. For example, the Heisenberg algebra in Section 1.4 was made to act as operators on a symmetric algebra. Again the mapping x ^ ad x makes a Lie algebra act on itself as operators. With both of these examples we have started with an abstract Lie algebra and represented it as linear operators. In applied mathematics or physics the situation is normally reversed—Lie algebras arise in the first place as Lie algebras of operators. Yet each of the Lie algebras that we study has many very different representations. As a simple example consider the case of §I2(1K). By definition, this is a Lie algebra of operators in a two-dimensional vector space. On the other hand, its adjoint representation jc ad x makes it act on a three-dimensional space. We will see later (Section 2.4) that these two representations are the two simplest nontrivial irreducible finite-dimen­ sional representations of ^12(^)1 in fact they are the two first members of an infinite family of such representations. Let g be a Lie algebra, and let F be a IK-space. By a representation of g on V, we will understand a Lie algebra homomorphism tt: g ^ gI(F). In other words, tt is a linear map from g into End(F) satisfying (1) for all JC, y G g and v ^ V, Through tt, g is made to “act” on V as the linear operator 7r(jc), jc e g. By an action of a Lie algebra g on a K-space V, we will understand a bilinear mapping •g X ( x , v )

F X

' V

1.6

Representations

29

satisfying [x, y ] ‘ V = X ' y

u —y x

Given an action, we say that g acts on V and that V is then called a g-module (relative to this action). These two concepts (modules and repre­ sentations) are essentially the same. If tt is a representation of g on F, then g acts on V via X ' V = 7 r(x )(f)

for all jc e g and v El V.

On the other hand, if g acts on F, then v ^ x • v is a linear mapping of F into itself. Defining tt: g ^ End(F) by '7t ( a: ) ( í;)

= X •

u

determines a representation of g on F. It is simple to verify that the two processes we have just described are inverses of each other. Although g-modules and representations of g are just different ways of looking at the same mathematical situation, we will find both concepts useful. (Notice that our correspondence is between representations of g and left g-modules. It is easy to turn this into right action by defining u ' x = —x - v ) . Given a homomorphism tt: g ^ g l ( F ) , we say that the representation tt is finite (resp. infinite) dimensional and that F is a finite (resp. infinite) dimensional g-module if the dimension of F over K is finite (resp. infinite). Let F be a g-module. A subspace F ' c F is said to be a submodule of F if F' is itself a g-module. In symbols, if X ' v' ^ V'

for all jc e g and v' e F '.

A submodule F ' of F is called trivial if V' = (0) or F ' = F, and it is called nontrivial otherwise. If F ' ¥= F, we say that F ' is proper. A module F ^ (0) is said to be simple, or irreducible, if F does not have any nontrivial submodules. The equivalent concepts for subrepresentations and irreducible representations are defined in a similar way. If F is a g-module, then the set Ann(F) = {jc e g|jc • i; = 0 for all z; e V) is an ideal of g called the annihilator of F. Of course, if tt: g -> g I(F )is the representation corresponding to F, then Ann(F) = ker(7r). We say that a g-module F (resp. a representation tt of g) is faithful if its annihilator (resp. kernel) is trivial. If Ann(F) = g so that jc • z; = 0 for all x e g, then the module (or corresponding representation) is called trivial. If F is graded space and g is a graded Lie algebra, both graded by the same group Q, and if F is a g-module with the property that g“ • F^ c F “"^^ for all a, p E: Q then we say that F is a graded g-module. Example 1 (Adjoint representation) Let g be a Lie algebra, and recall the linear map ad: g ^ End(g) is given by ad ;«:(y) = [ a:, y].

30

Lie Algebras

Then (1) is immediately satisfied because of the Jacobi identity. Therefore ad is a representation of g into gl(g). It is called the actjoint representation of g. The corresponding g-module is g itself where the action is given by left multiplication. The kernel of the adjoint representation is the center of g. It follows that this representation is faithful whenever g is centreless, in particular whenever g is simple. Example 2 Any graded Lie algebra can be viewed as a graded module over itself via the adjoint representation. Example 3 Recall the Heisenberg Lie algebra a as constructed in Section 1.4. At that time we “realized” a as an algebra of operators 5. This actually constitutes a faithful and irreducible representation of a. If we now view S as an a-module, the grading of S is compatible with that of a (ibid) and 5 is a graded a-module. Example 4 Let F be a vector space. Then gI(F) and §I(F ) act on V by their very definition, and we obtain the natural representations of gI(F ) and §I(F) on V, We list next some basic operations that can be performed with modules and representations of a Lie algebra g. We will intentionally switch back and forth between these two concepts in order to emphasize their equivalence. / QUOTIENT MODULES Let F be a g-module, and let F ' c F be a submodule of F. The quotient space F / F ' can be given a natural g-module structure by defining x

' V = x

- V

for all jc e g , and i; e F,

where : F ^ F / F ' is the canonical map. This module is called the quotient module of F by F'. 2 DIRECT SUMS Let iTj-: g gl(l^), ; e /, be a family of representations of a Lie algebra g. Then the space F = has a natural g-module structure by defining ^ •{L '^j£j

'

= E ‘^j (x)(vj) j ej

for all

e q ,Vj e Vj,j e J.

The representation tt of g in F obtained in this way is called the direct sum of the ir/s. We denote this by tt =

1.6

3

31

Representations

TENSOR PRODUCTS

Let TTyi g Qi(Vj), ; = 1 ,..., n, be a finite family of representations of g. Set F = ® • • • (8) and define tt: g End(F) to be the unique linear map satisfying n

tt{ x ) { v ^ (8> • • •

® ¿;„) = ^ ; =i

0 *• • 0 7Ty(A:)([;y) 0 • • * 0

for all X e g whenever Vj e l / , for all ; = We claim that tt is a representation of g in V. Indeed, if x and y e g and if 0 ••• 0 is as above, then 7r(x)7r(y)(i;i 0 • • • 0 z;„)

= u-(j:)i E Di 0 ••• 0Tr*(y)(y;t) 0 ••• 0y„ \k = l n

I k —\

E I^i 0 ••• ®Trj{x){Vj) 0 ••• 0 ir* (y )(i;* ) 0 ••• 0 y „

= L

*= 1\ ;= 1

+ Ui 0 • • • 0 ir*(j:)ir*(y)(i;*) ® +

E j=fe+i

® ••• 0

By interchanging the roles of (7r(;c)'n-(y) -

®v„

0 • • • 0 TTy(A:)(:;y) 0 • • • 0 D„|. / a:

and

17(y)l7(:i))(D i ®

we have

y,

■■■ ® V „ )

n

= E y=i

® ••• ®

-

‘^ j ( y ) ' ^ j ( x ) ) ( V j )

0 ••• 0

n

= E

® • • • ® ^;([^. y])(i^;)

®

® v„

7= 1

=

® ••• 0 y„).

and hence ir is a representation of g as claimed. This representation is called the tensor product of the iTy’s and we write ir = tti 0 • • • 0 4

TENSOR REPRESENTATION

Let it: g ^ gI(F ) be a representation of g, and let T(V) = the tensor algebra of the space V. By 3 above we obtain a family of representations ir„: g ^ g I(r"(F )) for all n e (where we take ttq: g -♦ IK

Lie Algebras

32

to be identically zero). Then itj = a representation of g in T(F), thanks to construction 2. This representation is called the tensor representa­ tion of the module V. Notice that by Proposition 1.5.1 and the definition of 7T„, we can characterize TTjixXx e g, as the unique derivation of T iV \ extending the linear map tt{ x ): V V. 5

EXTERIOR REPRESENTATION

Let K be a g-module and consider the tensor g-module T(V), Recall the exterior algebra of V A ( V ) = T ( V ) / ( v ® v\v e V). If jc e g, we have X ‘ (u

u) = X'V<S>V-\-U<S>X-U = ( x ^ V + v) <S>( x ' V

v) - X ' V ^ X ' V - V ® V ,

This, together with the fact that x acts as a deviation on T { V \ implies that the defining ideal of A(F) in T(K) is a g-module and hence that A(F) has an induced g-module structure that satisfies n

X•

f\ • • ■ f \ v ^ =

^

■ / \ x • Vi ^

• f\v^

1= 1

for all a e g and y j,. . . , ii„ e F. The g-module A(g) is called the exterior module of V. Note that each A"(F) is a submodule of A(F). 6

HO M JV, W) AND g rH O M jV , W)

Let V and W be g-modules. Define a map g X Hom^CF, W ) ^ H om ^iF, W ) by (x,f) -^x-f, where ( x - f ) ( v ) ■■=x-f(v) - f ( x ■v) for all X G g, f e Hom|,^(V, W), and y e V. This map is clearly bilinear.

1.6

Representations

33

Moreover, if y g g, we have y] * / ) ( i ’) = [ x, y] - f i v ) - f ( [ x , y ] ■v) = x - y - f { v) - y - x - f { v ) - f i x - y v ) + f ( y - X ■v) = ( x - y - f - y -X - / ) ( y ) . This shows that the map in question gives Hom^iF, W) a g-module structure. A particularly interesting case is when W = K viewed as a trivial g-module. Then K* has a g-module structure via ( x - f ) v = - f ( x • v)

for all ;c G g , / e K*,z; G K.

Next suppose that both V and W are Q-graded g-modules. Recall the subspace grH o m ^(F ,iF ) = © H o m J F ,iF ) " c H o m K (F ,iF ). If jc G g", / G Hom(|^(K, WY , and v g ( x - f ) v

= x - f ( u )

- f ( x

we have • u)

e

Thus X - / g HomQ^CK, and hence grHomu^CK, IT) is a graded gmodule. Let g be a Lie algebra, and V and V' two g-modules. A map f : V ^ V ' is called a homomorphism of g-modules if / is linear and if f ( x • l>) = x • f ( v) for all X G g and i; g K. The concepts of endomorphism, isomorphism, and so on, of g-modules are defined in the usual way (see Section 1.1). Proposition 1 (Schur^s lemma) Let 7t: g ^ oMV) be an irreducible representation o f a Lie algebra % on a space V. Then (i) Every endomorphism o f the %-module V is either trivial or an automor­ phism, (ii) Let a be an endomorphism o f the K-space V. Suppose that cr com­ mutes with all o f 7r(g). I f there exists an eigenvector o f a in V then a is a scalar. Proof If /: K F is a g-module homomorphism, then both k er(/) = {¿; e V\ f(v) = 0} and im (/) = {f(v)\v g V) are g-submodules of V. Part (i) follows from the simplicity of V. If 0-: F F is any K-linear map such that Tr(x)a = cnr(x) for all x g g, then each of the maps (o- —A • 1), A g K, is an endomorphism of the

34

Líe Algebras

g-module K Suppose there exist v and Aq e K such that aiv) = X^v. It follows that (o- - Aq ‘ 1) is not an automorphism and hence that it is trivial. Thus cr{u) = \ qU for all v ^ V, and hence (ii) holds. □ Remark 1 The existence of eigenvectors for cr in part (ii) of Schur’s lemma is ensured whenever V is finite dimensional and IK algebraically closed. Let A be an associative algebra and V a IK-space. By a representation of A on F, we will understand a homomorphism tt: A End(F). In other words, 77 is a linear map from A into End(F) satisfying for all x , y in A and V in V: (2)

iriAi'Ki') = 'rr(x)(ir(y)(u)) = (i7-(x)ir(y))(i;),

(3)

i7(l)(£ ;)

=

y.

The concept of representation of an associative algebra is analogous to that of a Lie algebra except for the (obvious) fact that we now view End(F) as an associative algebra instead of a Lie algebra. Condition (3) follows from our convention on homomorphisms of associative algebras (see Section 1.1). Similarly we define an ^-module to be a IK-space V together with a bilinear map (a,u) ^ a ‘ V from A X V into V and satisfying

( 4)

(ab) ' V = a ‘ {b • v)

for all ¿z, 6 g

i; g V.

Let F be a module for an associative algebra A, and let M be a submodule of F. A submodule of F is called a supplement of M if F = M 0 iV as an y4-module. Proposition 2

[Ja2].

Let V be a module for an associative algebra A. The following conditions are equivalent: (i) There exist simple submodules (M ,),^/ o f V such that V = (ii) There exist simple submodules (M,),=/ o f Vsuch that V = (iii) Every submodule o f V admits a supplement. A module satisfying the equivalent conditions of Proposition 2 is called semisimple, or completely reducible. One easily sees the following proposi­ tion: Proposition 3 Let V be a semisimple module o f an associative algebra A. Then every submodule of V is semisimple.

J.7

Invariant Bilinear Forms

35

Remark 2 The concept of complete reducibility also applies to g-modules. We will see later (in Section 1.8) that there exists a one-to-one correspon­ dence between g-modules and left modules of the so-called universal en­ veloping algebra U(g) of g. The algebra U(g) is associative, and hence the whole theory of modules over associative algebras can be put to work to obtain information about g-modules. We finish this section by introducing the concept of absolutely irreducible representations. We do this for modules over Lie algebras, though a similar concept exists for modules over associative algebras. Let g be a Lie algebra over K, and let M be a g-module. Let IK' be a field extension of IK. By extension of the base field from K to K' (Section 1.1), consider the K'-Lie algebra g' := IK' 0

g

and the K'-space M' = K' 0

M.

It is clear that M' has a natural g'-module structure satisfying a ^ X ' b <S > m = a b <^ X' m

for all ¿z,

e IK', x e g, m e M.

Now if M is irreducible as a g-module, then M ' need not be irreducible as a g'-module (see Example 5). If M' is irreducible for all field extensions IK' of IK, we say that M is an absolutely irreducible g-module. Example 5 Let g = IR (one-dimensional real abelian Lie algebra). Let ^

Let p: g

gI(M ) be the unique representation

satisfying p(l) = Then p is irreducible. On the other hand, the corresponding complex representation of C g = C on is not.

IJ

INVARIANT BILINEAR FORMS

The concept of a group acting as isometries on a quadratic space is a familiar one. One has a space V, a bilinear form ( I ) on F and a group G acting on V so that for all g e G, for all v,w ^ V (g • v\g • w) = (i;|w). The correspond­ ing concept for Lie algebras is as follows: Let 77: g ^ gI(F ) be a representation of g on a vector space V over IK. A bilinear form ( I ) on V is said to be g-invariant (relative to ir) if for all jc e g and for all y, w e F (1)

( 7 r { x ) v \ w ) + ( v \tt( x ) w ) = 0 .

36

Lie Algebras

In the particular case that V = q and tt is the adjoint representation, (1) reads

( 2)

([j^ ])lz ) + (y l[^z]) = 0

for all X, y, z e g, and we then say that (*|*) is an invariant bilinear form on g. There are minor variations of the preceding definition. When IK = C, hermitian forms are often more appropriate, especially in physical situations. In many cases straight invariance is too strong, so instead we have an antiautomorphism a of period 2 on g and replace (1) by

( 3)

(7t( x ) i;1vv) = (v\Tr{(r{x))w).

Rather than trying to discuss all of these variations at once, we will discuss only g-invariant bilinear forms here and bring up others as they arise. The general way in which they are used is always much the same. Likewise, although one could conceive of arbitrary g-invariant bilinear forms, in practice the only ones occurring are either symmetric or skew-symmetric, so we will restrict ourselves to these two types. Suppose that ( I ) is a g-invariant symmetric or skew-symmetric bilinear form on a g-module V. If IT is a g-submodule, then the invariance of ( I ) implies that the subspace W orthogonal to W defined by W

(i; e V\{u\w) = 0 for all w e W)

is also a g-submodule. If one knows that W is nonsingular (e.g., if (I*) is positive definite), then W O W = (0); if in addition we assume that V is finite dimensional, then V = W ^ W . This type of reasoning is standard in showing that a finite-dimensional g-module is completely reducible. In deal­ ing with infinite-dimensional g-modules, we will have to proceed with more caution. The preceding argument applied to the adjoint representation shows that if a is an ideal of g, then so is a . In particular g is an ideal of g (called the radical of the form). We conclude that if g is simple, then ( 1 ) is either trivial or nondegenerate. Example 1 Define (-I ) on gI„(IK) (or gI(K) for finite-dimensional V) by ( X\ Y ) = i r ( X Y )

( = tr(M i)).

This is symmetric and invariant: t r{[ XY] Z) = tr(ATZ - YXZ) = tr(ATZ) - ít(YXZ) = tr(yZA^) - tr(yXZ) = - t i { Y [ X Z ] ) .

1.7

Invariant Bilinear Forms

37

Since K1 is an ideal of 9l„([K), so is (IKl)-^ = and we arrive again at gI„(lK) = IKl X (Example 1.1.5). The trace form on ^I„(IK) must be nondegenerate because ^I„([K) is simple (Exercise 4.1). Let g be a finite-dimensional Lie algebra over K. The Killing form 9 X 9 9 is defined by k

(

x

,

y) = tr(ad X ad y)

k

:

for all x, y e g.

Just as in Example 1 the Killing form is symmetric and invariant. Example 2 (The Killing form on ^ I2([K)). We use the basis e , h , f of Example 1.1.6. Then the matrices of ad e, ad h, and ad / are 0 0 0

-2 0 0

0] 1 ,

oj

ad

=

/2 0

\o

0 0 0

0] 0 , ad/ = -2j

0 -1 0

0 0 2

0 0 0

and, for instance, /2 K( e, f ) = tr(ad e a d / ) = tr 0 \0 The matrix for

k

0 2 0

0\ 0 = 4. 0^

relative to the basis e , h , f is

In particular det(K) = —128 so that

k

is nondegenerate.

The Killing form is a cornerstone in the conventional treatment of finite­ dimensional Lie algebras. Traces rarely make sense for infinite-dimensional Lie algebras, and we usually have to construct invariant bilinear forms in a very explicit way. Proposition 1 Let (•!*) be an invariant bilinear form on a Lie algebra g. Then every elementary automorphism o f g is an isometry o / (• | *). Proof Let X, y e g. The invariance condition reads (ad u{x)\y) = -(x\ad(u)y) for all w e g. Now suppose that u is locally ad-nilpotent, and

Lie Algebras

38

set
= D 77 ((ad «)'x |y) y=0 J'= L ( - l ) l 7 7 (^l(adM)'y) ;=0 \J' J = (j:|e x p (-a d w)y) = (^|cr"^y). We conclude that (x|y) = (x\o-~^ay) = {(xx\cry), and hence that a is an isometry of (*| *). Since, by definition, every elementary automorphism of g is a product of automorphisms of the form cr = as above, the result now follows. □ L8

UNIVERSAL ENVELOPING ALGEBRAS

Suppose that we are given a representation tt; g gI(K)ofa Lie algebra g. Through 77 we can realize g as a Lie algebra of transformations on V. Since 7r(g) is a subspace of the associative algebra End(K), we consider the associative envelope A ^ of 77(g), that is, the (associative) subalgebra of End(K) generated by 7 7 ( g ) . The nature of the representation 77 is completely refiected in the associated representation of (g-submodules of V corre­ spond to ^^-submodules of K, etc.). The close connection between g and A ^ gives rise to the question of what we can say about associative algebras A that are related to a Lie algebra g in the following way: 1. there is a Lie algebra homomorphism 7: g ^ Lie(^), 2. y(g) generates A as an associative algebra. We call such an algebra an associative enveloping algebra of g. In this section we show that there is a universal algebra of this type—uni­ versal in the sense that every other associative enveloping algebra of g is a homomorphic image of this one. We make considerable use of these univer­ sal enveloping algebras in the sequel. Let g be a Lie algebra. By a universal enveloping algebra of g we will understand a pair (U, /) composed of an associative algebra U together with a map /: g U satisfying the following conditions. UEl The map i is a Lie algebra homomorphism from g into Lie ( U ) ; that is, i is linear, and i([^>y]) =

- i {y)i {x)

for all x , y e g.

1.8

Universal Enveloping Algebras

39

UE2 Given any associative algebra A and any Lie algebra homomorphism /: 9 ^ Lic(A), there exists a unique algebra homomorphism /: Vi ^ A such that the following diagram commutes:

In other words, f = f ' ° The standard type of argument for universal objects (e.g,, Section 1.2) shows that if g has universal enveloping algebras (U ,0 and then Vi ^V i' in the strong sense that an isomorphism / between these algebras exists such that f °i = V. As for the existence of this object we have Proposition 1 Let q be a Lie algebra. Then g admits an universal enveloping algebra. Proof. Let T = r( g) = tensor algebra of the space g. We let u be the two-sided ideal of T generated by all elements of the form X ^ y - y ® X - [x,y]. Symbolically u

<x ® y - y ® JC - [jc, yjlx, y e 9>t(9).

Let U:= r / u and denote by tt the canonical map from T into U. The algebra U is clearly associative [the multiplication in U, which will be denoted simply by juxtaposition, is associative since that is the case in T, and 7t(1) is its identity. Notice also that U # (0) since u c ©">iT"]. Define /: g U by i = ttIt’i; in other words, i is the restriction of tt to r^(g) = g. We claim that (U, i) is a universal enveloping algebra of g. To begin with, if X and y are in g, then i([x, y]) = tt([x , y]) = tt( x <8>y —y 0 x), since [x, y] = j c 0 y —y 0 x mod u and u = ker tt. On the other hand, tt( x 0 y —y 0 x) = 7r(x)7r(y) — 7r(y)'7r(jc) = /(x)/(y) —z(y)/(jc), and hence U El holds. Now let / : g ^ ^ be any linear map of g into an associative algebra A satisfying (1)

f{[x, y\)=f{x)f{y)-f{y)f{x).

By the universal nature of r(g ) (see Section 1.2) there exists a unique algebra homomorphism f . T ^ A satisfying /(1) = 1 and /( x ) = /(jc) for all X e g [we are using here the identification g = T^g)]. Because of (1), / factors through U (see Proposition 1.1). In other words, we obtain an induced

40

homomorphism f : U

Lie Algebras

A such that the diagram

commutes. Since f ( x ) = f {x) for all x e g, we obtain the desired commuta­ tive diagram (UE2). □ If 9i and 02 Lie algebras over K and /: 82 is a homomorphism, then it follows from the definitions that there is a unique homomorphism U (/): U(Qi ) 11(92) such that

9i ---------> 92 '■'1 U(/) 1'^ U(gi) ^ U(92) commutes. A direct consequence is that we can view U as a functor from the category of Lie algebras and Lie algebra homomorphisms (over K) to the category of associative algebras and their homomorphisms (over K). In the sequel we will denote the universal enveloping algebra of g constructed above by U(g), the map i being understood. Notice that U(g) is generated (as an associative algebra) by the elements i{x), e g. Let g be a Lie algebra and ir a representation of g into a IK-space V. Thus TT is a Lie algebra homomorphism from g into gI(F) = Lie(End(F)). It follows that V extends to an algebra homomorphism, also denoted by v , from U(g) into End(F) where U(g) is the universal enveloping algebra of g. In other words, V becomes a left U(g)-module with the action u ■v = tt( uX v ) for all Me U(g) and y e F. Conversely, if F is a left U(g)-module, we retrieve a representation ir of g in F by defining v i x X v ) ^ where i: g -» U. It is simple to verify that these two procedures are inverses of each other, and hence that the categories of representations of fl and of left U(g)-modules are isomorphic. ° Note that if F is a g-module and v g-submodule of F containing v.

V, then U(g)y is the smallest

1.8

41

Universal Enveloping Algebras

Our construction seems to give us very little information about U(g). When g is abelian, however, we have the following: Proposition 2

The universal enveloping algebra U(f)) o f an abelian Lie algebra to the symmetric algebra 5(1^) o f

is isomorphic

Proof Consider the tensor algebra r(l^) of the space 1^. The defining ideal u of U(]&) is then given by n = ( x ( S > y - y ( S f x\x, y e f)>7'(i)) since 'tj is abelian. But T(ij)/n is then the symmetric algebra Sfi)) (see Section 1.2). □ The next result, which is of utmost importance for all that follows, tells us how to construct a basis of U(g) from a basis of g. The injectivity of the map i: g U(g) will be an immediate consequence of it. Theorem 1

(Poincare-Birkhoff-Witt) Let q be a Lie algebra with a K-basis {xj\j e /} indexed by some totally ordered set J. Let (U, /) be the universal enveloping algebra of g. Then the family o f elements

with j\ <j'2 ^ ‘ space U.

j'ny ri ^

together with 1

form a basis of the

Proof Let U = U(g) be the universal enveloping algebra of g as constructed above. The first part of the proof shows that the displayed family spans U. The second, and considerably more difficult part, shows linear independence of these elements by constructing a suitable representation of g in which they clearly act as linearly independent operators. Let M be the set of finite ordered sequences of elements of J. Thus M=

< ••• < y „ , n e N } .

The empty sequence, assumed to belong to M, will be denoted by 0 (it corresponds to the case n = Oin the above notation). If m = (j\, . . . , ; „ ) g M, we define n to be the length of m and write /(m) = n. We also define •••

Xj^^

42

Lie Algebras

By convention = 1G

= T’®=

Notice that if J is empty so that g = (0), then our present theorem states that U = IK • 1. This statement is true, as can be seen from Proposition 2. We will henceforth restrict our attention to the case where J is not empty. We proceed in several steps: (a) The family {7r(x„)|m e M) spans U. Let U' be the span of this set. Clearly and ttCTO are in U', since in this case the elements in question are either scalars or linear combinations of the Xy’s with ; e J and both 0 and (;) are in M. We now reason by induction on n to show that ttCT") c U' for all n. Because tt is linear, it suffices to show that if jc e T" is of the form x = X: 0 • • • 0 x , , then 7t( jc) g u '. If 7i < * * < we are done. Otherwise, there exists 1 < k < n such that jj^ > Then 7t{ x ) = TT{Xj^

0

• • •

®

= tt( xj^ ® • • • ® = tt( xj^ ® ®

® (^ 4 .. ® + [^ 4 ’ ’^ h J ) ® • • • ® 1 0 X :Jk-\ 1 0 JCJk: 0 • • ®^y„) +

where x' e T^~^, By the induction assumption, 7t( jc') e U'. If the sequence in the first summand is not increasing, we repeat this procedure until it is. We conclude that ttCT") c U' for all n. Since T = and 7r(D = U, step (a) follows. We make now a technical pause to see that there is no loss of generality in assuming that the total ordering in J is actually a well ordering. From (a) we M and see that if the result fails then there exists elements mj, N nonzero scalars E: IK such that N

( 2)

E

= 0-

n= \

Now the indeces appearing on these m are finite in number, say < j 2 < **' < Jk (where N < l(m^) + • • • +/(m^)). By Zorn’s lemma there exists a well ordering ^ on J such that j\ < j'2 ^ ' ** Jk - Now (2) shows that it is sufficient to establish the Theorem for well ordered sets. We assume henceforth this to be the case for the given total ordering of J. (b) Let u = ^ ^et of symbols, and let V be the IK-space constructed with i; as a basis. We intend to give V a g-module structure and later use the universal nature of U to show the independence of the 7t( x„). We begin with some notational conventions. If m = (j\, e M and ; e J, we write ; < m in case j < j\. We also agree that j < 0 for all j e J. If j and m are as above and j < m, we write j m for the sequence ( j , j i , j 2’ -' yJn) ^ Clearly l(jm) = 1 + /(m). Finally, for all « e Kl, we let denote the subspace of V spanned by all the such that /(m) < n.

1.8

(c) There exists a bilinear map (x, for all y e / and for all m e M: (0

43

Universal Enveloping Algebras

-> x • v from g X K into V such that

if j < m,

(ii)

Xj -

-

(iii)

Xj ■v„ G Ki

if / > m, m = A:m',

We reason by induction on n to show that there exists a map

with the desired properties. If n = 0, then Vq is spanned by U0, and we define • ^0 = which is clearly as desired after linear extension to g. Let n > 0. Then has < /1} as a basis. Since we already have a bilinear map Q X V n -i^ V n ,

we define Xj • for all ; e J and m e M with /(m) = n. We do this by induction on the order of J. If j'q is the first element of J, we set X:Jo '

= U^:0™

Now let y e J be arbitrary, and suppose that k < y. If y < m, we set

• ¿;^ has been defined for all

Otherwise, m = (y^,. . . , y„) with j > j^. Set m' = (j'2, . . . , ;„), and define Xj ■

= Xj^ ■X j ■v„, + [xj,

• i;„-.

The right-hand side is already defined. Indeed, since /(m') < /(m), Xj • already defined. Moreover Xj-v^=

£

is

c„u„.

l{n)
Now is defined, since already have the map

Now by bilinear extension we get a map

as desired.

<j. Also [xy, Xy^]eg, and we

44

Lie Algebras

Before continuing we make an observation: If m = A:m' and r > k, then (3)

Jfr •

+ y

for some n with /(n) = /(m'), some h where r > h > k, and some v e Vi^^y Indeed, if r < m', set /i = r and y = 0. Otherwise, m' = hwl' where r > h > k, and we use step (c)(ii). (d) The bilinear map constructed in step c makes V into a g-module. We must verify that x • y ' v —y ' x • v = [x, y] • v for all x, y e g and V EiV.W suffices to show that the equation ( ;, k;

Xj

Xj ■

= [xj, x^] • v„.

holds for all ;, A: e J and m e M. We use induction on /(m). Assume, without loss of generality, that j > k [both sides of { j , k \ v ^ are skew-sym­ metric in j and k]. If A: < m, then (;, k; i;^) is an immediate consequence of (i) and (ii). We can therefore restrict our attention to the case where m = rm' and j > k > r. Now (j, k;Uj^) reads ( ;, k, r)

Xj - x ^ - x , -

- x^ • Xj ■x, ■v„, = [xj, x^] • x , • v^,.

Of course we do not know whether (;, A:, r) holds. But we do know that both (A:, r, j) and (r, j, k) hold. For instance, (A:, r, j) reads { k, r , j )

X^- X^- {Xj ■ v„,) - X , - X k - (Xj ■

=

[x^, X, ] ■Xj ■v^.

But by (3), Xj • + u' for some n with /(n) = /(m'), v' e and j > h > r. Thus both (A:, r; and (k, r; v') hold [the former because r < h, the latter by induction on Km)]. It follows that (k, r, j) = (k, r; v^^) + (k, r;u' ) also holds. Since the induction assumption implies that for all x , y in g, x-yv^,-yx

v„, = [ x , y ] - v ^ ,

the right-hand side of (;, A:, r) can be rewritten as follows: [ x j , x ^ ] ■X , ■

= j:, • [ X j , =

•Xj

Xk\ ■

■X,, ■

+

[[xj, x^], x,]

- x , - x y Xj ■

■ +

[ [ X p J c * ],

x, ] ■v„,,

and similarly for i k , r , j ) and (r,j,k). Now compute ( j , k , r ) + ( k , r , j ) + (r, j, k) to obtain an identity of the form 1 = 1 + Jac(j:y, x^., x^) • v^, which obviously holds. Thus, since {k, r, j) and (r, j, k) are known to be true, so is (;, k, r).

1.8

Universal Enveloping Algebras

45

(e) We now finish the proof of Theorem 1 That the elements of the form

with j\ < • • • < « e Z+ together with 1 span U over K, is an immediate consequence of step (a), since these elements are precisely the family {irix jlm e M}. To see that they are linearly independent, we view the g-module V constructed in step (d) as a left U(g)-module. Let us show that =

for all m e M.

Again use induction on /(m). If /(m) = 0, then m = 0 , = 1 and 1 • ¿;0 = i;0, so our assertion is clear. If /(m) > 0, we write m = ;m', where j < m' and Km!) = Km) - 1. Then = 7r(xj)7r(x^.) and therefore tt( x J • = Tr(Xj) • TT(x^r) • U0 = 7t(Xj) • = Uj^r = v^. Suppose now that we have a linear combination of the form L

= 0,

meM

where the and all but a finite number of these letting this element act on u^, we obtain

meM

are zero. Then by

meM

and hence all c„ = 0, since the y„’s form a basis of V.



We list below some important consequences to the Poincare-Birkhoff-Witt (PBW) theorem. Corollary 1

The images {i(xj)}j^j in U(g) of the basis {xj}j^j o f g form a linearly independent set. In particular i: g

U(g) is injective.

With this Corollary we can (and will henceforth) identify g with a subspace of U(g). If Ji e g, we write x e U(g) [instead of i{x) e U(g)]. Notice then that tt{x ^ ® • • • ®x„) = x ^ . . . x ^ for all Xj,. . . , j(:„ e g. Corollary 2

Let b be a subalgebra o f the Lie algebra g. Suppose that C {y*}*eK ^ a basis o f g such that { x j \ ^ j is a basis o f b and both J and K are totally

Lie Algebras

46

ordered. Then (i)

the injection 6 -» g -> U(g) can be lifted to an injection o f U(b) into U(9), (ii) U(g) is a free left (resp. right) U.(b)-module admitting the family {y*, • • • ^ ^ a basis. Proof From b -» g ^ U(g) we obtain a homomorphism U(b) U(g)- We totally order the set JU K (disjoint union) by declaring that j < k for all y e J and A: e K. The family { X,-Jl

. . . X,

Jn

y*. • • •

^ ■■■

...k„,n,m

is then a K-basis of the space U(g). Moreover the subfamily that does not involve the (i.e., when m = 0) corresponds to a basis of U(b). This clearly implies (i) and (ii). The statements on right U(b)-modules is proved similarly. □ Corollary 3 Let 9i , . . . , be Lie algebras, and Lie algebras). Then

s e t

Q

U(9) - U ( 9 i ) ®

=

X



X

{direct product of

® ll(9n)

as K-spaces. Proof Exercise

^

Proposition 3 Let 8 be a derivation o f a Lie algebra g. Then there exists a unique derivation Sy o f U(g) extending 8. Proof If such an extension exists, it is necessarily unique, since g generates U(g) as an algebra. As for its existence we know that 8 extends to a derivation 8r of the tensor algebra T(g) of g [Proposition 1 of Section 1.5 together with the canonical injection of g in T(g)]. Now let U be the ideal of r(g ) defining U(g). Recall that U is generated by all elements of the form p( x , y) = X ® y —y 0 X — [x, y],

^ ,y ^ 9 -

1.8

47

Universal Enveloping Algebras

By straightforward computation we verify that = ^

+ ^(-*^) ® y - y ® 5 ( x ) - 5 ( y ) ® X

- [ ^ , 5 ( y ) ] - [5(^),y] = p ( x , 5 ( y ) ) + p { 8{ x ) , y ) . Hence dj- stabilizes the linear span of the p(x, y), and therefore it also stabilizes U (use the fact that 8j is a derivation). The induced map 5u: jj(g) U(g), U(g) = T (g )/u , is then a derivation of U(g) extending 8. □ Proposition 4 l£ t % be a Lie algebra. The adjoint representation extends uniquely to a representation {denoted by adu and also called the adjoint representation) o f g on U(g) by which g acts as inner derivations on U(g). More precisely for all X e g, u e U(g), adu(x)(«) = XU - ux.

Proof Let X e g. By Proposition 3 the derivation ad x of g extends uniquely to a derivation adjjX of U(g)- Consider the inner derivation Aj.. m —>xm —ux of U(g) (see Section 1.5). Evidently 8 = ady x —A^. is a derivation of U(g), which annihilates g. Thus 8 annihilates the associative algebra generated by g that is, U(g). This proves that ad„ x = A^. The mapping x A^ is a Lie homomorphism of g into gI(U(g)), showing that ad„ affords a representa­ tion of g. ^ Remark 1 Recall that in Section 1.6 we introduced the tensor representa­ tion of a given g-module. In the case of the adjoint representation this leads to a representation ad^ of g on T(g) in which adj.(x )( yi® for all

X,

®y„) = ¿ y i ® ••• ® [^>y;]® ••• ®y« y j , . . . , y„ ^ 9-

On the other hand, in U(g) we have a d „(*)(y,...y.)- Z y i - U . y , l -

y-

........

from which we see that the mapping tt: T(g) ^ U(9) is a g-module map.

48

Lie Algebras

Remark 2 One ought to be aware that U(fl) has two natural g-module structures which are quite different. 1. The preceding adjoint representation in which n

; =i 2. The restriction to g of the natural left U(g)-module structure of U(g) as an associative algebra in which ^ • (y i •••>’/,) =

•••>'«•

Let g = © „ e c 9 “ he a graded Lie algebra. We can then find a basis e j of the space g consisting of homogeneous elements, say, Xj ^ Q ' for all y e J where aj e Q (of course the aj need not all be distinct). The tensor algebra T(g) is then naturally <2-graded by declaring that each monomial ;c ® • • • ® ;c is of degree a, + • • • + «, • The defining ideal u of U(g) is graded since ®

®

^22] ^ 9“'^ “'-

It follows (see Section 1.3) that the quotient algebra U(g) = T(g)/u inherits a (2-grading called the grading of U(g) inherited from g. Thus U(g) = © U(g)“ and U (g )“U (g)^

cU (g)

a+/3

for all a, P ^ Q-

Remark 3 The spaces U(g)“ are independent of the choice of basis [xj}j^j of g as above. Notice also that if jc e g, then the expression x is homoge­ neous of degree a ” is independent of whether we view x as an element of g or as an element of U(9> via the identification g ^ U(g). Proposition 5 Let Q be a Lie algebra. Then U(g) « « domain [i.e., the condition ah = 0 a = 0, orb = 0 holds for all a and b in U(g)J. Proof Let f x } , be a basis indexed by a totally ordered set J U t X = Proof. Let 1 ^ „ e N} be the basis of U(g) prescribed by the li "

1.9

Central Extensions

49

Poincaré-Birkhoff-Witt theorem. Define subspaces U„, n e N, of U(g) as follows: Uo = D<, Uj = IK + g,

U„ = IK + g + gg + • • • + s". In other words, U„ is the subspace of U(g) spanned by all x : X such that for all c U„ c ... and U„U„ c U„ l(x) < n. Clearly U. q C U i C n, m € N. The family (U„)„eN therefore a filtration of U(g). For each n e N, define IK-spaces U" by U" == where by con­ vention U_i = (0). Let gr(u) = e U". The map U„ x \X„ given by multiplication induces a well-defined bilinear map U" X U” ^ U"+'". We can then extend this to a multiplication in gr(U). The algebra gifU) thus obtained is called the graded algebra associated with the above filtration of U(g). be defined hy x ■= x If is If X = Xj^ . X: G X, we let X e clear that (4) The family is a basis of gi
50

Lie Algebras

contained in its centre such that e/c = g. The simplest example is e = g X c, where c is an abelian Lie algebra. Somewhat less trivial is to let c (0) be a commuting subspace of derivations of g and then give the space e = g 0 c a Lie algebra structure by defining for all c g c and x e g , [c, x] = c(x) = - [ x , c], and [c, c] = (0). The Lie algebra e is then a central extension of g; moreover g is an ideal of e and [e, e] c g. The Virasoro algebra, however, is not like this: The Witt algebra 93 is not a subalgebra of 93 and [93 , 93] = 93. We are concerned here with central extensions of this second and more subtle kind, which are called coverings. It is not obvious at this point that there is any necessity for making central extensions, and we do not try to motivate the concept any further except to say that the representation theory of a covering e of a Lie algebra g may be vastly richer than that of g itself and that in practice such objects arise completely naturally. The purpose of this section is to present the concepts of covering algebras and central extensions in a coherent way and to find necessary and sufficient conditions for the existence of universal covering algebras. Finally, as an example, we establish that the Virasoro algebra is a universal covering of the Witt algebra. The basic theory in this section is based on [Gr]. Let g and c be Lie algebras over K. By a central extension of g by c we will understand an exact sequence of Lie algebras: (CE)

0

0

such that c is in the centre of e. In other words, we have a surjective Lie algebra homomorphism tt: e g and an injective homomorphism /: c e such that c = ker(7r) is in the centre of e. Given another central extension (CE')

0

c' -U e'

0

of g, then by a morphism of the central extension (CE) to the central extension (CE') we will understand a pair (<#>, o) of Lio algebra homomorphisms such that the diagram

‘ "1

is commutative. The central extensions together with their morphisms form a category.

1.9

Central Extensions

51

A Lie algebra I is said to be perfect if I equals its derived algebra, that is, if I = [1,1]. The central extension (CE) is said to be a covering of g in case e is perfect. Proposition 1 If the central extension {CE) o f % is a covering, then there exists at most one morphism o f (CE) to a second central extension of g. Proof Let (o) and (', be morphisms from (CE) to (CE'). We then have a commutative diagram analogous to the diagram above by replacing (¡) and Q by (j)' and 'o, respectively. It follows that for all z e e , 7r'(/)(z) = 7t( z ) = Tr'(t>'(z), and therefore that 4>{z) - 4>'{z) G ker(i7') = i'(c').

(1) Now let ( -

X

and

y

belong to e. We have

y]) = H[ x > y ] )

- '([x,y])

= [4>(x),(f>{y)] - ['(x),'{y)]

= [4>(x) - '(x),(y)] + ['(x),(y) ~(f>'(y)]

= 0, where the last equality follows from (CE). We conclude that 0 and (¡>' coincide on [e, e], and therefore on e, since e is perfect by assumption. Thus (f) = and therefore
52

Líe Algebras

Beginning with a central extension 0

9

let us choose any subspace g' of e such that g' g (isomorphism of K-spaces). Such a subspace can easily be constructed: Let be a IK-basis of g, and let x'j g e be chosen so that irixj) = Xj. Then the IK-span g' of the family j is as desired. We l e t g g' be the inverse map of 77. Then for all x, y e g, 'n-{[x,y] - [x',y']) = 0, and therefore ^ ( x , y) — [x, y j - [x', y'] e c. Our choice of g' has thus led us to a bilinear map (Co)

a: g X g ^ c

satisfying the following properties for all x, y, z g g: (Col)

a ( x , x) = 0

and hence a( x , y) = - a ( y , x ) , (Co2)

a ( x , [ y , z ] ) + a ( y , [ z , x ] ) + a ( z , [ x , y ] ) = 0.

[These properties are immediate consequences of (LAI) and of the Jacobi identity.] A bilinear mapping a from g X g into a K-space c is called a 2-cocycle of g with coefficients in c if it satisfies (Col) and (Co2). We do not intend to discuss the cohomology of Lie algebras from which this terminology arises [Ja 3]. Important for us is the fact that any 2-cocycle of g with coefficients in c gives rise to a central extension 0 - » c - ^ e - > g -^ 0 of g where /: c

e is the inclusion map. This is done as follows: Let e := g 0 c

(direct sum of vector spaces).

Define a multiplication [*,*]:,« on e by [x + a, y + fe]* = [ x , y ] + a ( x , y )

f o r a l l x , y Ge ; a , f c Gc .

1.9

Central Extensions

53

Properties (Col) and (Co2) of the given 2-cocycle a guarantee that e, together with [•,•]*, is a Lie algebra. We also see that the projection tt: e ^ 9 given by X

a^ X

is then a Lie epimorphism and that its kernel c is included in the centre of c. Remark 3 The construction of our 2-cocycle a from (CE) depends upon the choice of the subspace g'. Different subspaces will in general lead to different 2-cocycles. On the other hand, different 2-cocycles may lead us to isomorphic central extensions. These questions are again in the domain of cohomology of Lie algebras and need not concern us here. Our intention is to construct universal coverings by means of “universal” 2-cocycles. For this we need to recall the second exterior power A^(g) of a vector space g. Let T\ %) = g <S) g. (This is just a tensor product of K-spaces. If we think of the tensor algebra T(g) = a noncommutative polynomial algebra, then T^(g) can be thought of as the linear span of all the monomials of degree 2.) Let J be the subspace of 7^(g) spanned by all elements of the form X 0 X, X e g, and define A^(g) = T \ q ) / J , We let r^(g ) A^(g) be the canonical map and for all x and y in g write x A y instead of x 0 y. Notice that x A x = 0 and x A y = —y A x for all x, y e g. Proposition 2 For a Lie algebra g to admit a universal covering, it is necessary and sufficient that g be perfect. Proof If g is admits a universal covering then (by definition of covering) g is the homomorphic image of a perfect algebra and hence is perfect. For the converse let I be the subspace of A^(g) spanned by all elements of the form X A [ y ,z ] + y A [ z , a:] + z A [jc,y],

x , y , z ^ g.

Define V = A^(g)/I, and for all x and y in g, let a(x, y) denote the image of X A y e A^(g) in V under the canonical map. Evidently a is a 2-cocycle of g with coefficients in V. Set e = g ® E. Define a composition law [ ,

on e by

[^ + y, y + w]j = [x, y] -I- a{x, y)

for all x, y ^ q ; v, w e V.

54

Lie Algebras

As we said earlier, this makes e into a Lie algebra. For completeness we fill in the details. The bilinearity of [ •, • \ is clear. The anticommutativity follows from the fact that for all^:, yin g,[jr,y]= - [ y , a:] anda(x, y) = - a ( y , x ) . As for the Jacobi identity consider three elements where i = 1,2,3, e g, and e K of e. Straightforward computation shows that Jac(

X 2, X^) = Jac(A:i, X2, ^^3) + («(^l»[^2»^3]) + =

+ «(^3>[^1.^2]))

0.

Indeed Jac(;ci, X2, x^) = 0 because g is a Lie algebra, and by definition the remaining term in the sum is the image in A^(g)/I of the element x^ A [ x 2 , x^] X 2 /\ [ ^ 3, ^ 1] + A [ x j , X 2 ] of A^(g), which is also zero. Now let 7t: e ^ g be the canonical surjection; that is, tt: a : + r; jc for all a : e g and v El V, Then tt is a Lie algebra epimorphism, and since V clearly lies in the centre of e, we obtain the central extension ( 2)

V-

9^0.

We intend to show that there exists a morphism of this central extension of g to any other. Suppose that

( 3) is any central extension of g. We will denote the bracket of e' by [•, • ]j-. Let us write e' as a direct sum of subspaces g' ® i'(F'), where g' is a preimage of g under tt'. Identifying g with the subspace g' of e' and V with i(F'), we write e' = g © V . Then we have a 2-cocycle f : Q X Q - * V with [x,y], . = [ x, y ] + / ( x , y ) . Since / satisfies the identities of (Co), there is an induced map /: A^(g) V' vanishing on the subspace I c A^(g) defined above. This allows us to define a linear map V ^ V' by o{a(x,y)) = f { x , y )

x,y^Q.

Recall that c = g 0 F. Consider then the linear map : c c' given by (f>(x v) = X , q) is a morphism of (2) to (3). Since o is the restriction of to F, it will suffice to

1.9

Central Extensions

55

show that (a) the diagram

9 is commutative, and (b) is a Lie algebra homomorphism. Let j:, y e g and y, w e K. Then Tr'((x + v))

= tt\ x +

o{v)) = X =

tt( x

+ v)

so that (a) is clear. Next (4)

<^([x: + y ,y + iv]e) = <^([x,y]e) = y] + a ( x , y)) = [ x, y ] + if>oa(x,y) = [^> y] + f { x , y),

(5)

([x + v ,y + wle) = [x, y]e- = [x +

^

= [(x + v),<j>{y + w )],,, and hence (b) holds [Equations (4) and (5) follow from the fact that V and V' are included on the centers of e and c', respectively.] This establishes the claim that there exists a morphism from (2) to (3). We cannot conclude that (2) is the desired universal covering of g, since c need not be perfect. This problem is corrected by defining e' = [ e , e ] , , the derived algebra of e. Since g is perfect, it is clear that 7r(e") = g, and hence that e = + F. Thus e" = [e, c] = [e^ + F, e" + F ] = [e^ , e^], since F is in the centre and therefore c" is perfect. Now let We contend that the central extension (6)

0

9^0,

= e"

n F.

Líe Algebras

56

where tt" is the restriction of tt to , is universal is surjective because, as remarked earlier, c = + V), Indeed, given any other central extension (3) of 9, we know the existence of a morphism (, <^q) from (2) to (3). If we now define and Q to and c^, respectively, it is clear that (", ) is a morphism of (6) to (3). Since e" is perfect; (6) is indeed a universal covering of g. □ Our last Proposition makes the following definition meaningful: A perfect Lie algebra e is said to be centrally closed if e is its own universal covering. We then have Proposition 3 (i) (ii) (iii)

The universal cover o f a perfect Lie algebra is centrally closed, Every central extension o f a centrally closed Lie algebra splits, I f c is centrally closed and c is a subspace o f Z(g), then 0 ->c-^e->e/c^ 0 is a universal central extension of e/c.

Proof, (i) Suppose that e is the universal cover of a perfect Lie algebra g and that the extension is given by 0

c-U e ^ g

0.

Suppose, on the other hand, that 0 - > b - *^ f A" c

0

is a covering extension of e. Let i be the kernel of tt o f ^ g. If jc e i, then fi(x) e kerirr) = /(c), so (0) = [M-i), e] = f] and [x, f] c ;(b ). But [oi, f] = [ac, [f, f]] c [[ji, f ], f ]] <= f ] = (0). We conclude that 0

i ^ / -----*Q ->■ 0

is a central extension of g. Accordingly there exist homomorphisms v: c and vq: c t such that the diagram

-i

'i

' - r f

TTofJL

f

1.9

Central Extensions

57

commutes. We then have f = [f>f] = [»'(e) + f, v(e) + i] = v[e, e] = v(e). Finally, let w := o v: e e. Since tt ° to(x) = v i x ) for all a: e e, co(x) = x + c(x), where c: e c is some linear mapping. From (a[x, y] = [&)(ac), 6>(y)] we find that c vanishes on [ e, e ] = e. Thus ¡x°v = id ^, and we have the commuting diagram 0 0

i f

Since V is surjective we see that ¡i is injective and finally that f = e and b = (0). (ii) Next let

(7)

0

b —^ f —> e

0

be any central extension of e. One sees that f - = [ f , f ] is perfect, and replacing f by f ' in (7) if necessary, we may assume that f is perfect. Then (7) is a covering of e and part (i) of the proposition gives with v : e ^ f, ¡jLop = idg. Thus (7) splits. (iii) The proof of this part is left as an exercise. □ A very important example of a central extension occurs in connection with constructing the covering algebra of the loop algebra The reader is referred to the appendix at the end of the book for a discussion of As a second example we prove the following proposition: Proposition 4 (i) The Virasoro algebra is the universal covering o f the Witt algebra. (ii) Virasoro algebras are centrally closed. Proof. Let 2B = the Witt algebra (notation of Section 1.4). Since SB is perfect, SB has a universal covering algebra e = SB 0 F (vector space sum) with corresponding 2-cocycle a. Using property (Co2), we have (8)

0 = a ( L „ [L„,, L J ) + a ( L „ , [ L „ , L j ) + a { L „ , { L „ L j ) = ( n - m ) a ( L ^ , L„+„) + (/: - n ) a{ L„, L„^*) + {m - k)a{L„,Li^^„)

for all A:, m, « e Z.

58

Lie Algebras

Setting A: = 0, we obtain (9)

0 = (n - m)a{Lo, L„+„) - na{L„, L„) + ma{L„, L„) = (« - m)a(Lo, ¿ m + J - (m + n ) a { L ^ , L„).

If /c + m + n = 0, we can eliminate n in (8) to obtain 0 = ( - * - 2m)a(L*, L_*.) + (2A: + m ) a ( L „ , L_„) + (m —k ) a [ L Setting A: = 1, this becomes (10)

(m - 1) « ( L „ + i , L - ( „ +d) = ( - 1 - 2m ) a ( L i , L _ i ) + (m + 2) a( L„, L _ ^ ) .

We now set about to “adjust” the L„’s by elements of the centre V. We have [^0?

^(-^0? ^n) •

Set for all n ¥= 0, and ^0 ~ ^0 Clearly [¿0. L„] = [ L q, L„] = nL„

for all n.

We next see that (11)

[ l „,L„] = ( n - m ) L ^ ^ „ for all m , n

In fact

0 with m + n ¥= 0,

1.10

59

Free Líe Algebras

whereas i n —m \ (n - m) L„^„ = (« -

^m+n)-

Therefore (11) now follows from (9). Now [¿m. ¿-m] = [■i'm- ^-m ] +

¿'-m) = ~ 2mLo +

¿-m )

= -2mLo - m a ( L i , L _ i ) + a ( L „ , L _ „ ) . Set P(L„, L_„) = - m a ( L i , L_,) + a(L „ , L_„) e F for all m e Z, and extend /3 bilinearly to the entire linear span of the elements L„ by defining P(L„, L„) = 0 whenever m + n # 0. Then, for all m, n e Z,

The mapping )8 is a 2-cocycle with valid for any 2-cocycle, we have (m



+

L_j ) = 0. Since equation (10) is

^ - ( m + l)) ”

By induction it is easy to see that ^(L„,L_„) =

- m )/3(L2,L_2)

for all m > 2.

Setting c = 2p ( L 2, L _ 2\ we arrive at [ l „, L„\ = ( n - m)L„+„ + We now let 33 be the K-span of the L„, n ^ Z, and c in e. Then 33 is a subalgebra of e isomorphic to the Virasoro algebra. Finally, c = [c,e] = [33 + F, 33 + F] = [33,S] = 33. This proves part (i). Part (ii) follows from Proposition 3(i). □

1.10

FREE L IE ALGEBRAS

In this section we investigate what sort of K-space a set X of symbols will generate if they are allowed to freely combine subject only to the condition that the resulting object be a Lie algebra. Consider at first a Lie algebra q and a subset X of g. Form the set 33(^) of all products of elements of X.

60

Líe Algebras

Thus 93 may be constructed recursively by (la) (lb)

A^c93(AT), if p y , p 2 ^ ‘^ { X ) ,

then

[ p i , p 2] e 93(-^)-

The set of all (finite) linear combinations of elements of 93(AT) is clearly a Lie subalgebra [X]^ of g, called the subalgebra of g generated by X. In particular g is generated by if g = [X]^. Similarly let Q(AT) be defined recursively by (2a) (2b)

X^£i(X), if Pi

e g,

^ Q(-^),

then

[pi,p2l ^

The linear span of £i(X) is called the ideal of g generated by X and is denoted by I ik(A0. Example 1 Consider the Lie algebra gj

j

of 3 X 3 matrices

a, b, c G K, IK-E12 + K jE23

^^13

where E^j denotes the matrix with 1 in the (/,;) position and 0 elsewhere. Since [£12, £23! = ^13j 91,1 is generated by £12 and £23. Since a single element in a Lie algebra can only generate the space it spans, it is clear that no fewer than two elements could generate gj j. It is immediate that [£i2, [ £ i 2> £23]] = 0 —[£23,[£ i2> £ 2311* In general, what can one say about a Lie algebra g generated by two elements x, y satisfying the “relations” [x,[x, y]] = 0 and [y,[x, y]] = 0? Since any prod­ uct involving two or more multiplications is 0, g = Kx Ky + lK[x, y], and it is easy to check that £12 x, £23 y gives rise to surjective homomor­ phism (f> (in which £13 -> [jc, y]) of gj 1 g. There is no reason why (¡> should be injective; for instance, g could have been abelian so that [x, y] = 0. However, we have established that in some sense gj 1 is a “largest” model for Lie algebras with two generators satisfying the above two relations. This observation leads us to the natural question of presentations of Lie algebras: Given a set X and a set of identities (relations) involving sums and

1.10

Free Lie Algebras

61

commutators of the elements of what sort of Lie algebras are there that can be generated by X and satisfy the given identities? Is there some “largest one” that satisfies only these identities and the Lie identities? The answer is yes, and “largest” means that every other Lie algebra generated by a set X satisfying the same relations is a homomorphic image of it. Free Lie algebras are Lie algebras on which no relations are imposed (other than those for a Lie algebra: skew-symmetry and the Jacobi identity). We will make a number of important constructions of Lie algebras by presentations in this book. Always the problem with this method is to get some understanding of what the resulting Lie algebra is really like. For instance, consider the two presentations: 9i 3: x , y : [A:,[A:,y]] = 0 = [y, [y, [y, [y, Ji]]]], 82,2: x , y : [Ai,[jc,[-»:,y]]] = 0 = [y, [y, [y, Ji]]] • It is not obvious that 3 is six dimensional and that 82,2 ¡s infinite dimensional. Clarifying such problems almost always involves ad hoc con­ struction of explicit representations of the Lie algebras. Free Lie algebras are defined by their mapping properties: Let be a set. A Lie algebra ^ is said to be free on AT if AT c g , and for any Lie algebra g and any map / from X into g there exists unique Lie algebra homomorphism / ': g g for which the following diagram com­ mutes:

Proposition 1 Let X 0 be a set. Then there is a free Lie algebra on X , and it is unique up to isomorphism. Proof. The uniqueness question is established by the usual method (see Section 1.2) and is left as an exercise. Let A ( X ) be the free associative algebra on X over K. Inside Lie(^4(AO) let g = S ( ^ ) be the Lie subalgebra [X]^ generated by X. We show that g is free on X. h&t g be any Lie algebra over K, and let /: A!' -> g be any map. Let U(g) be the universal enveloping algebra of g. Then there exists a unique homo­ morphism / : A ( X ) ^ U ( q)

62

Lie Algebras

of associative algebras extending / (we are assuming that g is embedded in U(g) in the usual way). We claim that / ' == / |g is the required Lie algebra homomorphism. First we have /'([^.y]) =f(xy - y x ) = /( x ) /( y ) - f i y ) f ( x ) = [f'ix),f'(y)\

forallx,yeg,

so / ' is a Lie homomorphism. This shows that if / ' ( x ) , / ' ( y ) s g, then also f'i[x, y]) e g. Since f ' i X ) = /(AT) c g, it now follows from the definition that /'([Afl^) c g [see (la) and (lb)]. Thus / ' makes the above diagram commutative. It is clearly unique since X generates □ Remark 1 The free Lie algebra on the set X is denoted by ^(A"). When it is convenient, we will use the model constructed above without further comment. A Lie algebra g is said to be free if it is isomorphic to §(AO for some X. Proposition 2 In the notation above, the free associative algebra A ( X ) is the universal enveloping algebra o f g(AT). Proof Let A be any associative algebra over IK, and let / : %{X) Lie(A) be any Lie homomorphism. By the definition of A(X), f \ x lifts uniquely to a homomorphism / ': A ( X ) ->A. Now f'l^^x) is a Lie homomorphism, and it extends fix'- X -» Lie(.<4). Thus, by the definition of free Lie algebras, it must coincide with /: A(X)

Since / ' is the only possible lifting of f i x , it is the only lifting of /. This proves that A ( X ) has the mapping properties of a universal enveloping algebra of g( AO. □ The free associative algebra A ( X ) (which is also the tensor algebra of the K-span V of AO is Z-graded by the total grading. Each element of AT is homogeneous of degree 1, and g(AO = [AOk- With the notation of (la) and

1.10

Free Lie Algebras

63

(lb), ©(A") consists of homogeneous elements of A(X), and hence § (A ) is the K-span of homogeneous elements. It follows that § ( A ) is graded bv 7- Jr. fact ’ " S(A)=

eg(A )", n= l

where g ( A ) " : = g ( A ) DA' ^i X) . Example 2 X = {x, y}. Bases for g"(A ), 1 < « < 5: g ^ ( A ) : X, y;

g ^ (A ) :[ ; c, y ] ; g3(A): [ji,[jc,y]],[y,[y,A:]], 3 '‘(A ): [Ji, [Ji,[ji:,y]]],[y, [y,[y,J:]]], [x,[y,[x,y]]],[y,[x,[x,y]]Y, [x,[x,[x,[x,y]]]]; [y,[:c,[x,[x,y]]]]; [y,[y,[x,[x,y]]]]; [y>[y>[^.[^»y]]]]; [[^,y],[jc,[Ai,y]]]; [[jc,y],[y,[jc,y]]]. Suppose that A = {xj,X2, . . . } (possibly finite), and let g = Z e Z ® • • • [number of factors = card(A)]. Then A ( X ) is graded by Q: For n = («i, ti2, . . . ) e (2 (all n, > 0) ^ " ( A ) is the K-span of the monomials y ^ . .. y*, where k = En„ and a:, occurs among the y,’s exactly n, times. Precisely the same argument as above shows that 5 (A ) inherits the grading S(A) = e 5"(A), where 5"(A ) ==5(A) n ^ " ( A ) . Example 3 In the example above, g^i-o^A) = K x;

5^‘’’*^(^) = Ky;

g(2.0) ( A ) = 0; 5<'’'>(A) = K[x,y]; 5 (^’i>(A) = K [ x , [ x , [ x , y ] ] ] ; g<2.2)( A ) = K[y, [x, [x, y]] + K [ x , [ y , [x, y ] ] ] ; g(3.2)(A) = lK [y ,[ x , [ x ,[ x , y ] ] ] ] + K [ [ x , y ] , [ x , [ x , y ] ] ] .

64

Lie Algebras

There is a considerable amount of literature on determining bases of free Lie algebras. The most famous of these are the Hall bases [Bo 2] and the Lyndon bases [Lth]. Let be a nonempty set, and let g = g(Ai) be the free Lie algebra on X over K, Let i? c g be any subset of elements, and let l(R) be the ideal of g generated by R. Then g == ^ / l ( R ) is called the Lie algebra defined by the generators X and the relations R. Remark 2 The terminology seems to suggest that AT is a subset of g, which it is not. Moreover it is quite common to say that ^ / l ( R ) is the algebra generated by the generators X and the relations = 0, thus both thinking of the natural image of X in as X itself (even though X need not be mapped injectively into the quotient) and anticipating that in the quotient the relations R appear equal to zero. Example 4 X = {x, y}, R = {[x,[x, y]], [y,[x, y]]}. The ideal generated by R contains all products of three or more elements of g. Let g == ^ / l ( R) . Then g = Kx + IKy + K[x, y] and g = g^^ of Example 1. Let g be a Lie algebra over K. By a presentation of g we will understand a pair (X; R) consisting of a set X and a subset R of the free Lie algebra S(AO on X such that g(A ')/I(i?) = g, where l(R) is the ideal of generated by R. Remark 3 Every Lie algebra has an infinite number of distinct presenta­ tions. For instance, we can take X to be any subset of g that generates it as a Lie algebra and take R = ker(g(AO ^ g). Evidently, if two Lie algebras have the same presentations then they are isomorphic and we may therefore speak of the Lie algebra with the presenta­ tion (X;R). Let {Qjlyej family of Lie algebras over K. For each j s. J, let {Xj-; Rj) be a presentation of g^. Let ^(uATy) be the free Lie algebra on the symbols u Xj (disjoint union), and identify ^ (Xj ) as a subalgebra of g(uA(y) in the obvious way. The Lie algebra f with the presentation ( u X j i U R j ) is called a free product of the family [with respect to the presentations (Xji Rj)l The natural mappings vf. g^ f defined by gy = %{Xj)/\{Rj) ^(uA y)/I(ui?y) = f are injective (see below) homomorphisms called the natural embeddings of gy in f. Proposition 4 {Qy}ye J ^ family o f Lie algebras over K. For each j e J, let (Xj; Rj) be a presentation of gy, and let f be the free product o f the family {gy}ye j ^dh

1.11

Campbell-Baker-Hausdorff Formula

65

respect to these presentations: (i) The natural embeddings Vj\ ^ f are injective, (ii) I f a is any Lie algebra over IK and Qj ^ d are homomorphisms, then there is a unique homomorphism tt: f a such that for all; e J 9; a f commutes. (iii) I f f' with embeddings v'j is another free product o f the family {9y}yej? then there exists an isomorphism (f>: f ^ f' such that (f>°Vj = Vj for all j. Proof (i) We maintain the previous notation. Fix any i e J. Then there is a homomorphism Qj such that 7t,( jc) = x for all x ^ TTj(Xj) = 0 for j i. Since = {0}, defines a homomorphism f g^, and evidently ° = id. Thus is injective. We leave (ii) and (iii) for the reader to check. □ In view of part (iii) of Proposition 4 we can speak of the free product of a family of Lie algebras. We denote this by j9y or simply by g^ * ♦ * g„ if J = {1,..., n} is a finite set. Example 4 The free product of a family algebras is the free Lie algebra on the set the presentations ({xy}; 0 ) of the IKxy’s.

of one-dimensional Lie j. This can be seen by using

We can use free products to combine Lie algebras together with cer­ tain relations imposed between them. We use this in a significant way in Chapter 4. Example 5 (Heisenberg algebras) Let a+, a_, and c be abelian Lie algebras with linear bases {x^\i e J}, [y.\i e J}, and {c}, respectively. Let / = a + * c * a _ , and let R be the set of relations -

dijC,[Xi,c],[yi,c]\iJ

e j}.

Then f / l ( R ) = a+ 0 c 0 a_ is a Heisenberg algebra. 1.11

CAMPBELL-BAKER-HAUSDORFF FORMULA

We begin with a nonempty set X and form the free monoid M = M{ X) on X (see Section 1.2). A typical word in M has the form W = X.

• • • JCi,

Lie Algebras

66

where . . . , X/^ ^ X, k > 0. We call k the length of w. M is finitely generated if X is finite. Let [K be a field of characteristic 0. (Much of what we say only requires that IKbe a commutative ring.) We can then form the free associative algebra A{ X) on X which has basis M and multiplication defined from that of M (see Section 1.2). ^4(J^) is graded with A ( X T spanned by the elements of M of length n. We denote by L ( X ) the free Lie algebra on X over K (see Section 1.10 where it was denoted by S(A")). According to Proposition 1.10.2, L ( X ) may be viewed as the subalgebra of Lie(^(AT)) generated by X, and then ^(A") is the universal enveloping algebra of X, The ring of formal power series (in the noncommuting variables AO over K is the set K ^ of all K-valued functions on M with algebraic operations of scalar multiplication, addition and multiplication defined by (flcr)( w) = aa{w), (c r +

t

)(

w

) = (t { x ) +

(crr)(w)

=

£

t

(

w

),

cr{ y) T( z)

for all cr, T e

w, y, z ^ M; a

yz = w

Intuitively a- G K ^ may be thought of as the infinite series We have a natural embedding of ^(AO in K ^ which realizes ^(AO as the space of functions on M with finite support (i.e., cr g K ^ such that cr{x) = 0 for almost all x ^ M). Set = (w G Af|lengthw = n) and K^ =

G K^\( t \mp = 0 if p ^ n}

for all n ^ N.

If O' G K^, we define o-„ by

( 1)

’J mp = 0 if p # n.

We will find it useful to generalize this to the case of K^ where A/" is a direct product of finitely many free monoids. The most important case is N = M X M where M is a free monoid, as above. Then K ^ ® K ^ ^ K ^ ^ ^ by identifying o- ® r with the function (cr 0 rXx, y) = o-(x)T(y). If = M 1 X • • • X Af^, then the length of jc = (x^, . . . , x ^ ) ^ N is length (^¿). Let A/' be a direct product of finitely many free monoids. A subset 5 of K^ is locally finite if for each ;c g AT, {cr g 5|o-(ji:) 0} is finite.

1.11

Campbell-Baker-Hausdorff Formula

If S is locally finite, then the sum

( E

67

defined by

= E o-(^) o-e5

^

makes sense. For example, if o- e and

then 5 •= {o-„|«

is locally finite

O’ = E o-„ = E o-„.

( 2)


n= \

Again, for each x e AT, define K, Sx(y) = ^ x . y For any choice of

e K, x e N, the set G N}

is locally finite. Using the definition of sums given above, we then have (3)

O’ = E o-( a:)5^ xsN

for all o- G

A third important example of a locally finite set is {o-ln = 0, 1, 2, . . . } , where o- g

( 4)

== { t

g

IK^|t(1)

=

0}. Thus for

a

g

IKi",

exp 0-— 1 + 0 - + - — +

and

(5)

0-2 cr^ log(l + (t ) ■■=
are well-defined sums. It is a straightforward exercise to show that exp: log: 1 + are inverses of one another.

-> 1 + (K+,

68

Lie Algebras

If O’, T e K+ and СГТ = ТСГ, then (6)

exp cr exp r = exp(o- + r ) ,

(7)

log[(l + o-)(l 4- r)] = Iog(l + O’) + log(l + r ) ,

as one sees directly by expanding both sides. Even if ат Ф та, exp a exp r = exp[log(exp a exp r ) ] . Our aim is to give some information on the nature of log(exp a exp r). Our exposition follows [Lth]. As a preliminary step we are going to establish another interesting result about free Lie algebras. Let ЛГ be a nonempty set, as before, and define (8)

Д: A ( X ) - ^ A ( X ) ^ A { X )

to be the unique homomorphism of associative algebras extending the map x»->x<8)l +

l0 jc ,

X ^

X.

We observe that Д is a graded homomorphism relative to the grading of A ( X ) <8>ЖАГ) for which (A(X)

А ( Х ) У = Ф A ( x y ® A ( X y ~ ‘. ¿=0

As mentioned above, we view L ( X ) as the subspace of A ( X ) generated by X where A ( X ) is viewed as a Lie algebra. Theorem (Friedrichs) F o r w ^ A (,X ), w G: L ( X ) «=> Ди' = 1 ^ 0 1 + 1 0 ^ . Proof. If

= w 0 l + l 0 ] v and Д 2 = г 0 1 + 1 0 г , then A[w, z] = [Aw, Дг] = [н ^ 0 1 + 1 0 н ^, z 0 l + l 0 z ] = [w, z] 0 1 + 1 0 [w, z],

which shows immediately that the elements of L ( X ) satisfy the diagonal condition. Conversely, let w satisfy the diagonal condition. We may assume that w is homogeneous of degree m > 1. Let {уДе/ be a totally ordered basis of L(J^). Then by the Poincare-Birkhoff-Witt theorem, < ¿2 < • • • < iV, r > 0, ^1, . . . is a basis of A(X).

e Z+}

1.11

Let w = Then

Campbeli-Baker-HausdorfP Formula

where each

21s above, and

69

^

’ w <8> 1 + 1 0 )v = Aiv = = L«j,k(Ay„) ‘ • • • (Ay,.J

Consider one of these summands Aw„ which, for simplicity, we write as A(y^i *• * y^"), where 5^,..., e Z+. This expands as

(yi 0 1 + 1 0 yi)*‘ ••• (y„ ® 1 + 1 = yi'yl' • • • y^» 0 1 + Siyi‘"V2" ■ • • y„" ® yi + S2yi'y|""‘ ••• y^" ® y2+ ••• + i„ y i'y !' ••• y^"“ ‘ 0 y „ + r(n ,s ), where r(n,s) e E,2.2-^(A!’)'"“' 0 A i X Y and m = Suppose that m >2. Since the expression

+ ■■■ +s„.

w 0 1 + 1 0 IV ^ A ( X ) 0 IK + IK ® A ( X ) and ( A ( X ) ® A { X ) ) " = ( A i X ) " 0 K) ® (K ^ A i X ) " ) ® { A { X ) ' ”~^ 0 v 4 ( J f ) ‘) ®

(

®A{xy]

and also {yj/e/ c : A ( x y is independent, we see that each nonzero summand W/

yp~^ •••

«>y/

must cancel with some similar summand in some other Ah^^. However, the pair (n, s) can be recovered from and hence cannot appear in any other AWj^. This shows that in fact m = 1, and hence w is in the linear span of the set {yj, e /; that is, w e L(X). □ We return to the formal power series rings where N is some finite product of free monoids. Let Ni, N 2 be finite direct products of finitely generated free monoids. An algebra homomorphism /: -> IK^2 jg continuous if whenever 5 is a locally finite set in IK^^, then /(5 ) is locally finite in and = If /: ^ IK^2 is continuous, then /(IK^O c for if cr e and /(cr) = + T, T e IK+2^ a 0, then {{a\ + r)"}„eN is not locally finite. Now, with and N2 as in the definition, let us see that any monoid homomorphism /: ^ IK^2 (^^2 being considered multiplicatively) for

70

Líe Algebras

which f ( Ni \ {1}) c IK+2 extends uniquely to a continuous algebra homomor­ phism /: ^ IK^2 If we recall that ^ requires that we identify x and 5^ and that any cr e IK^^ has the expression (3), we see that the obvious way to extend / to IK^» is by

( 9)

f{a) =

D

o-(x

) / ( a: ) .

A moment’s reflection shows that fiN^) is locally finite, and hence (9) makes sense. We leave it as an exercise to show that / is continuous and that (9) is the only way to extend / continuously to an algebra homomorphism. As an example consider the map A: M ( X ) ^ IK^® (8) IK-' ^ IK^^^

This will extend to a continuous homomorphism (10)

A : I K ^ ^ IK^^^,

which extends (8) and satisfies Ao- = £ A(T„ n= l

for all a

fM [see (2)].

Proposition (Campbell-Baker-Hausdorff) Let X be a finite set, and let x, y e M{X). Then log(exp x exp y) is a Lie element o f the form X

+ y + j[x,y]

+

•••

where the remaining terms are composed of higher (3 or more factors) commu­ tators of X and y. Proof Set M = M i x ) and consider the continuous mapping (10). We note that A ( M \ {!}) c IK^^^^. According to Friedrichs’ theorem log(exp x exp y) will be a Lie element if (11)

A log(exp X exp y) = log(exp X exp y) ® 1 + 1 0 log(exp x exp y) = log(exp X exp y 0 1) + log(l 0 exp x exp y ).

1.12

Extensions of Modules

71

Since exp x exp y ® 1 and 1 ® exp x exp y commute, and since A is continu­ ous, we can use (6) and (7) to rewrite (11) as (12)

log A(exp jc exp y) = log(exp x exp y (S>exp x exp y).

However, A(exp X exp y) = A exp x A exp y = exp Ax exp Ay = exp(x <8> 1 + 1 0 x)exp(y 0 1 + 1 0 y) = (exp X 0 exp x)(exp y 0 exp y) = exp X exp y 0 exp x exp y, from which (12) is immediate. Finally,

exp X exp y = l + x H ---- - + x\ = 1 + X + y + ^(x^ + 2xy + y^) H- terms of degree > 3 in x and y = 1 + x + y + | ( x + y ) ( x + y) + |( xy - y x ) + ••• = exp(x + y + ^ [ x , y] + ••• ). Since log(exp x exp y) is a Lie element, the higher terms are also commuta­ tors of X and y (involving at least three letters). □ In the exercises we give an explicit formula for computing further terms of the series for log(exp x exp y). We will have no need of any of these in the sequel. 1.12

EXTENSIONS OF MODULES

Let be a ring, and let be an abelian category of /^-modules. Given modules A, B in an extension of .^4 by B we understand a module E of if and morphisms a, such that we have the exact sequence (1)

72

Lie Algebras

Given another extension

( 12) oi E

0

B

E' ^ A

A hy B we say that (2) is equivalent to (1) if there is a morphism y: E' so that the diagram

B

fi'

E'

commutes. It is elementary to see that y is an isomorphism and hence that equiva­ lence is an equivalence relation on the set of extensions of A by B. We denote the set of equivalence classes by Ext(^, B). It is customary to study Ext(^, B) in the context of homology theory where Ext(^, B) is shown to be isomorphic to E x t^ ^ , B), However this theory requires that the category has “enough projectives”; that is, for every module ^ in ^ there is a projective module P in ^ and an epimorphism P ^ ^ ^ 0. Unfortunately, the category ^ of Section 2.6, for which we need to understand extensions, does not have enough projectives, so this theory is unavailable to us. Instead, we study Ext(A, B) completely in the context in which it was defined, that is, in the theory of extensions. There is in fact a complete theory of Ext in abelian categories [Str]. Our approach here is to provide the definitions and basic facts needed to prove what we need and leave the details to the exercises or to Strooker [Str] according to preference. Much of this can be found in [HS] on which our exposition is based. Our first object is to make Ext( - , - ) into a bifunctor on if, covariant in the second variable and contravariant in the first. Let a: X ^ A , p. X ^ B, be maps in if. A commutative diagram

’1

B

i‘ Y

with y in ^ is a push'Out (or fibred sum of A and B over AT) if it satisfies the universal property that for any commutative diagram

B

Y'

1.12

E xtensions o f M odules

there is a unique morphism A: y

73

Y' with

AT-----

commutative. Of course the push-out is unique up to obvious isomorphism, if it exists. Explicitly we can show that it exists by defining Y = (A e B)/K , where K = {«( a:) - P(x)\x e X ) , and by defining
+ K, ( 0 ,t ) + K .

Lemma 1 Let X .

1 B

4

be a push-out. Then (i) (p induces an isomorphism coker a Y /im ij/X (ii) if a is injective, so is i//. Furthermore, if

coker \jf {i.e. from A /im a

X /3

B is a commutative diagram and
74

Lie Algebras

By reversing all the arrows in the definition of push-out we arrive at the dual concept of pull-back. The analogous statement to Lemma 1 states that given maps a\ A X, B X, the pull-back X /3

B is characterized by the fact that


P'

E'

Since jS is injective, so is /3', and furthermore A — coker /3 = coker j8' by Lemma 1. This allows us to uniquely define a': E' ^ A so that E:

0

B

-^ E

-^ A

► 0

I ^ E '^ A

► 0

4 0

B'

One now has to check that this procedure maps equivalent extensions into equivalent extensions. Hence we have a map
E x t(^ , J3').

Furthermore (i) if B ^ B ' ^ B", then (^V) *=
1.12

75

Extensions of Modules

In precisely the same way if il/: A' ^ A is a. morphism then starting from the extension (¿ ), we can use pull-backs to get 0 ---- >B

>0 1

0 ---- - ^ E ' ^

A ’ ---------^0

and hence derive iff*:Ext{A,B)

Ext{A',B)

with

Lemma 2

Let ¿’e ExtiA, B), and let ij/: A' ^ A and
Following [Str] we prefer to write
and

Lemma 2 follows directly from the easily proved next lemma: Lemma 3

Suppose that we have the commutative diagram E:

0

E':

0 ---- » B'

A' ---- >0

B

1 >E'

Then < p ^ ( E ) = r { E ’).

*1

so that

76

Lie Algebras

Proof o f Lemma 2. Apply Lemma 3 to the top and bottom rows of 0 ---- » B

E' *A’ ---- »0 I Pull-back I

0 ---- > B

E --------- *A ---- »0 Push-out I

1

E:

1 1 0 ---- > 5 ' --------- > E"

>A ---- >0

Using this we can now define an abelian group structure on Ext(A, B), Let E:

Q --> B -^E ^A ^Q

and E^\

Q^ B

jEj

—^ A —>0

be representatives of two classes ^ and obvious maps,

of Ext(yl, B). Then, with the

E e E^: 0 ^ B e B ^ E ® E i - ^ A e A - ^ 0 is a representative of a class in Ext(^ 0^4, B 0 J?). Let V: B ® B ^ B and A: ^4 0 ^ be the maps + ¿2 a (a, a), respectively. We define ^

= V (^ 0

(see notation following the statement of Lemma 2). We leave it to the reader to prove that this is indeed an associative operation and that the split extension 0-^B ^A ® B -^A -^0 is the identity element. The inverse of the class (E ) of E:

O ^B ^E ^A -^0

is (¿ ( —id)) obtained from the morphism —id: A ^ A, a ^ —a. This can be

1.12

Extensions of Modules

77

easily shown: E + E ( - i d ) = V (£ © £ ( - id ) ) A = V{E © £ )(id , -id )A = (V (£ © £ ) ) a , where K: A ^ A ® A given by a •-» (a, —d). Now the construction of V(£ © £ ) is shown as the top two rows of E e E

B ®B

A ®A

Push-out A

B

V(£ © E):

A ®A

E2 (id,0)

0

proj

B ®A

V A

0

In the lower part of this diagram, the part that needs explaining is the map ¡jl: a - ^ ^ 2* Given a ^ A , we let e ^ E be any lift of a, and define fi(a) = X(ie, —e)). This is independent of the choice of e because V is addition of components. Now the bottom right-hand square is a pull-back because ()8, i n d u c e s an isomorphism between ker(proj) —B and ker a — B (use the dual of Lemma 1). But the pull-back of E2

A ®A Ta A

defines (V(E 0 E))K, so this extension is split. We now come to the main object of study. Consider an exact sequence of modules in ^ : B: Let A be any module in Section 3.1].

0

B ^ B' ^ B" ^ 0. Then we have the usual exact sequence [Ja 2,

0 ^ H o m (^ ,B ) ^ H o m ( ^ ,£ ')

Ho m{A,B").

From the above we have a sequence of maps E xt(yl,B ) - ! ^ E x t( ^ ,B ') ^ E x t { A , B " ) .

78

Lie Algebras

We construct a connecting homomorphism 5:

H o m (^,B ") ^ Ext(y4,B)

by 5 (/) = (Bf). (The top two rows of the diagram below illustrate this.) Proposition 4 The sequence 0 ^ H o m ( A , B ) ^ H o m (^ ,B ') ^ H om (/4,B") - ^ E x t( ^ ,B ) - i^ E x t( /l,B ') - ^ E x t ( ^ , S " ) is exact. Proof. We content ourselves with showing that the sequence of Proposition 4 is a null sequence. The rest appears in [Str] or may be taken as an exercise. First observe that = (il/(p)^ = 0. Now let / g Hom(>l, B"), and con­ sider E = 8f. The definition of 8f is given by the top two rows of the diagram. B'

B .

1

E:

0

B

hB'

y

B" Pull-back

4 E Ufj)

(id,0)

B' ® A

proj

1^ A 1 A

The bottom two rows clearly form a commutative diagram. By Lemma 1, since induces an isomorphism coker

5 = 0. In the same way let

B' — > J?" «A

1.12

Extensions of Modules

79

for some g, and let us see that 8f = 0. Looking at the diagram B'

> l>

(»>.g)| 0 ---- * B ----- *B e A (id,0)

B"

^0

i' proj

we see from the dual of Lemma 1 that the right-hand square is a pull-back. But this is the definition of 8f, and hence 3 f = 0. □ Corollary 1 Let 0 ^ B ^ B' ^ B" 0 be exact. Then Ext(A, B') = 0 if both Ext(v4, B) = 0 and Ext(^, B") = 0. □ Corollary 2 Let B = Bf^ Z) Bf^_i D • • z) Bi ^ B q = (0) be a filtration o f B. Then E x t(^,

= 0

/ = ! , . . . , / : = > Ext(y4, B) = 0.

Proof Use the exact sequences 0

B j_ ^

to prove inductively that Ext(A,

Bj B f)

B j/ B j _ ^

-> 0

= 0, ; = 1 ,2 ,... .

Along similar lines given B\

0 ^ B ^ B '^ B " -^ 0

and A as above, we have the exact sequence 0

Hom(5", A) ^ H om (5', A ) ^ Hom(B, A)

and also E x t(5 " ,^ ) ^ E x t ( B ', ^ ) - ! ^ E x t( B ,^ ) . If the connecting homomorphism 5:

H om (S, A ) ^ Ext(B", A )

80

Líe Algebras

is now defined by d( f) = (fB), then we have Proposition 4' The sequence 0 ^ Hom(B", A )

Hom(B', A )

Ext(fi", A) ^

A) ^

Hom(B, A) Ext(B, A )

is exact. Corollaries analogous to those following Proposition 4 can then be ob­ tained. EXERCISES 1.1 Let F be a finite-dimensional vector space over a field /3: F X F ^ IKbe a bilinear form. (a) Prove that

and let

9 = g(/3) — [a G End(V)\ß{ax,y) + ß ( x , a y ) = 0 for all jc, y e F} is a Lie subalgebra of gI(F). In the rest of this exercise we look at this important construction of Lie algebras more carefully. An endomorphism a e g(jß) is said to be an invariant transformation of ß. The Lie algebra g(j8) is the “linearized” version of the group Giß) of isometries of F relative to ß; that is, Giß) '= [a e GLiV)\ßiax, ay) = ßix, y) for all x , y ^ F}. Henceforth assume that ß is nondegenerate; that is, for x g F, ßix, F ) = (0) <=>X = 0 <=> ßiV, x) = (0). (b) Let p: F ^ F* be the linear map defined by {p(x),y) = ß (y ,x )

(c)

forall ac,y G F.

Show that p is an isomorphism. Show that for each a e End(F) there exists a unique element e End(F) such that piax, y) = /3(x, a*y), and show that the mapping a ^ a"^ of End(F) into itself is linear, bijective, and satisfies iab)* = Similarly define by pi*ax, y) = Pix, ay), and show that *ia*) = a = i*a)* for all a e End(F).

Exercises

81

(d) For each a e End(F) let a‘ e End(F*) be the transpose map defined by ( a ‘f , x ) = ( f , a x } .

Show that a* = p * ° a' o p

for some p e GL(V) and hence that tr a = tr a* (e)

for all a e End( F ) .

Show that for a e End(F), a e g(/3) «»a + a* = 0<=>a +*a = 0.

Conclude that g(/3) c (f) Let B be some basis of V, and relative to this basis write the vectors of V as column vectors with entries in K. Let J be the matrix of B relative to B so that B(x, y) = x^Jy

for all x , y e V.

Show that in matrix terms A* = and g(j8) = {A ^ qI„(IK)| JA = -A^J). (g) Show that the symmetric bilinear form k: Q(B) X 9(/3) ^ K k { a , b ) = tTy(ab)

is nondegenerate. 1.2 Let L be a finite-dimensional vector space over IK with basis B = (Cj,. . . , e„). (a) Define /3 to be the symmetric bilinear form on V whose matrbc relative to B is I„ in X n identity matrix). The Lie algebra g(/3) of Exercise 1.1 is called §o(n), or go(n,IK) in this case (special orthogonal Lie algebra). Show that a e §o(n) iff a is skew-sym­ metric as a matrix. Determine dim §o(n). (b) Suppose that n = 2m, and define /3 to be a skew-symmetric bilinear form whose matrix B is

82

Líe Algebras

(c)

This time g()8) is denoted by ^p(m) (symplectic Lie algebra). Determine dim §p(m). Let F be a vector space of finite dimension n over C, and let <*, • >: F x F - ^ C b e a nondegenerate hermitian form. Prove that the unitary Lie algebra U{n) := [a e qX{V)\{ax,y) + { x, a y) = 0 for all x , y e V] is a Lie algebra over R (but not over C!) and that the special unitary Lie algebra §U(n) := [a G Vi{n)\\x a = 0}

is an ideal of codimension 1 in U(«). Prove that relative to an orthonormal basis of F, a g U(n) <=> ú: is skew-hermitian. Find dim \X{n) and dim §U(n). (d) Show that the Killing form of is negative definite. Show that ^U(n) is a simple (real) Lie algebra and that its complexification (Section 1.1) is §I(n,C). 1.3 (a)

Let a and b be Lie algebras, and suppose that we are given a homomorphism of Lie algebras b ^ from b into Der(a). Define [ • , * ] : a e b x a 0 b - > a 0 b b y [a + b,

(b)

+ b'] = [a, a'] + b¿,(a') - 5^.(iz) + [b, b']

for all a,a' ^ a and b, b' g b. Show that this gives the space a 0 b a Lie algebra structure and that a is an ideal of this algebra. In particular show that for a Lie algebra a and any subalgebra b of Der a, a 0 b has the natural structure of a Lie algebra. The holomorph of a is the Lie algebra a 0 Der(a) constructed in this way.

1.4 Let ^ = 0 be an associative algebra which is graded by the abelian group Q. Show that 1 g A^. 1.5 (a)

Let A be an algebra over K, and suppose that IK is algebraically closed. Let / g Der(.^4), and suppose that for each a g IK we define :=

G y 4 l(/- a Y a = Ofor somes r

g

Z+).

Suppose that A = (this always happens if dim^^ ^ < oo). Prove that this decomposition affords a grading of A by (C, +). [Hint: ( / - (a + p)Xab) = ( / - aXd)b + a{f - /3Xb).]

(b) Find a similar statement for / e A ut(^). (c) Let g be a finite-dimensional complex Lie algebra. Let 6 e Aut(g) be of finite-order N. Set ^ and for each 0 < ; < iV define g-' = {ac e glflAc = ^^x). Show that g = ®j=o 9^ constitutes a grading of g by Z / N Z . (d) Let 0 be the automorphism of gIsiC) defined by = £,+i,y+i (indices mods) where is the ( i,;) matrix unit of gljfC). Determine explicitly the spaces g 13(C)-', j g Z /3Z for 0. 1.6 Let F be a vector space over IK with basis Show that by defining

{ v / ^l k g

Z}. Let a, /3

g

K.

= {k + a + I3{n + \))v„ +k J we obtain a representation of the Witt algebra SB on V. We denote V with this SB-module structure by F„^. Determine the conditions on a and ¡3 under which ^ is irreducible. 1.7 Let g be a finite-dimensional simple Lie algebra over K. Let g X g ^ IK be the Killing form of g. Let /B(g) be the IK-space of invariant bilinear forms on g. (a) Show that the elements of IB( q) are symmetric (use g = D(g)) and that they are either trivial or nondegenerate. (b) Let Z := {A G End,^(g)|A ad(x) = ad(x)A for all x g g} (the centroid of g). Show that Z is a field extension of IK and that g has a natural Lie algebra structure over Z (henceforth denoted 9z)(c) Show that the following are equivalent: CS 1: Z = J<. CS 2: The IK-Lie algebra IK®||^g is simple (IK = algebraic closure of IK). If g satisfies either of the two equivalent conditions CS 1 or CS 2, it is called central simple. (d) For A G Z let k^(A): g X g IK be defined by k^(A)(x, y) = K,^(x, A(y)). Show that / : A •-> K|,^(A) is a IK-linear isomorphism of Z onto IB(q). (e) Let g be a finite-dimensional simple Lie algebra over an alge­ braically closed field IK. Then I B ( q) = K k .

Líe Algebras

84

1.8 Let 1^ c g be Lie algebras. Let 3 = 3g(l^) == {x e g |[j:,^] = 0}, It = iig(]^) ■■= [x ^ g|[jc, 1^] cl^}. These are the centralizer and nonnalizer of in g, respectively. (a) Prove that 3 an n are subalgebras and that 3 is an ideal of n. (b) Show that if the representation of i) on g: p: f| ^ qK q) given by X >-» adg(jc) is semisimple, then = 1^ ® 3g('^)1.9 Let F be a IK space and A e V*. Let A: S(F) IK denote the extension of A to an algebra homomorphism. Show that kerA = Z S ( V ) { v - k ( v ) l ) . u^V 1.10 Let g be a Lie algebra and U(g) its universal enveloping algebra. Let A^: U(g) -> U(g) be given by A^^: u ^ xu - ux. Let x, / e g c U(g). For all e Z+ show that L « ; ( A ^ ) r - '( a d / y ( x ) , j=i where a,(AT) = ( - i y

N—j+\ f J.J. E k=l \ ■'

j

1.11 Let g be a Lie algebra, g ¥= (0). Show that g admits modules that are not semisimple. 1.12 Let G be a group and p: G -* GL(V) a representation of G on a K-space V. (a) Show that there exists a unique representation p I:

G

G L (F ® • • • ® F )

(n-times), « > 1,

satisfying p

U

x

) ( V

i

e> ■ ■ ■

<8>

v

„)

=

p ( x ) ( u i) ® • • • ® p (x )v „.

Let pqI G K be the trivial representation. Show that we obtain a representation pT:= Q pj;-. G G L ( r ( y ) = 0

n>0

^

n>0

r '* ( F ) ) .

'

85

Exercises

(b)

Show that determines a natural representation of G on S(F) an also on each component S"(F) so that p^(xXf x • • ‘ p(x)vi ■ p(x)v„. Show that p^ determines a natural representation p^ of G on A(F) and also on each component A"(F) so that =

(c)

• •

Л ■■■ AV„) = p ( x) { Vi ) A ■■■ A p{ x) ( v „) .

(d)

Assume that G is finite and that dim^^ F = / is ^nite. Given ^ G, let WiCac), . . . , щ(х) be its I eigenvalues in K. Verify the following identities in IK[[i]]:

X

П (1 i=l

= L ( - 1 ) " Ч р „^(д:)) г". n=0

1.13 Let a be an ideal of the Lie algebra g. Show that U(g)a = all(g) is an ideal of U(g) and U (g /a) = U(g)/U(g)a. 1.14 Let g be a finite-dimensional Lie algebra. Prove that U(g) is left (right) noetherian. [Hint: Use the associated graded algebra gr(U) and the noetherian property of 5(g).] 1.15 Let be a (not necessarily commutative) ring with no zero divisors, (a) Prove that the following conditions are equivalent ORE 1: Aa r\A b (0) for all a, b e A \ {0}. ORE 2: There exists a division ring D and a ring embedding A ^ D such that for all d e Z) \ {0} we have d = x~^y for some x ,y ^ A. ORE 3: For every left .,4-module M the set = {m e M\am = 0 for some

a e ^ \ {0}}

is a submodule of M. A ring satisfying the above equivalent conditions is called an Ore domain [see JA II]. (b)

Let {b„)„ez ^ nonnegative real numbers such that Iim sup„_Jb„)'/" < 1. If we define a„ := E"=ib„ show that lim su p „^ ia„)‘/" < 1.

Lie Algebras

86

(c)

Let A be an associative algebra with no zero divisors. Assume A admits a filtration of subspaces A = \J7=o-^i IK =. ^0 <=•••• AiAj c Ai+j for all i, j e N. dimjj Ai < 00 for all i e N.

Defineb„ == d i m S h o w that if limsup„ < 1, be the Virasoro then A is an Ore domain. Let S3 and § l2 algebra and affine —§ l2 respectively. Show that U(9S) and U(§l2(IK)) are Ore domains. (d) Prove that if g is a finite-dimensional Lie algebra, then U(g) is an Ore domain. (e) Let g = ® “=ig" be a graded Lie algebra such that dim,^ g" < oo so for all n e Z+. Suppose that limsup„_j[dim g")*/" < 1. Show that U(g) is an Ore domain. 1.16 Let R be an Ore domain, and let S c i? be a subring. (a) Show that if R is free as a right S-module, then S is an Ore domain. (b) Let a c g be Lie algebras. Show that if U(g) is an Ore domain so is t/(a). 1.17 (See J. -P. Serre, Lie Algebras and Lie Groups, Benjamin, New York, 1965.) Let Y be a nonempty set. Let A ( X ) and ^(36) denote the free associative and free Lie algebra on X. Recall the augmentation ideal A+ (X ) = ®„^ qA(X)". Define a linear map

by d( jii,. . . ,

[■^i> • • • >■^n] := a d ^ i ••• adx„_i(A:„)

for all eX Let ad: § (X ) ^ gI(g(X )) be the adjoint representation. It extends uniquely to an associative algebra homomorphism ad: A { X ) ^ E n d g (Y ). (a) (b)

Prove that for all u ^ A i X ) , v e ^ ( X ) + , d(,uv) = 2id(u)d(v). Prove that dlg(Ar) is the derivation of g (X ) for which d\^^xr is scalar multiplication by n (Dynkin’s theorem).

Exercises

(c)

87

Let X, y ^ X, X ¥=y, and let z := Iog(exp X exp y) m+1 ( - 1) = E E — m m= l P+<J>0 and let z = Ez„, where z„ g g(AT)". Prove the following explicit formula for the terms z„ of the Campbell-Baker-HausdorflF formula: ~

"

^

^P,q’>

p + q= n

where

Pl+ ••• +Pm=P

(-!)"■ +' (a d x ,r(a d y i)« ' • • • (ad x)^"-(y) m P i ' - - - q x '--“ P j

- +q^_^=q-\

Pi-^Qi>\ (ad X i/'(ad y,)^' • • • (ad y / ”- ( x ) P l + • • • + P m - l = P - ‘^

m

P l'-Q l'-

^1+ ••• +l

- --

Q m -l'-

1.18 Let Z be a set, g(AT) the free Lie algebra on X over K, and let M be an g(A!’)-module. Let d: X ^ M he. any map. Show that there exists a unique extension of d to a linear mapping d: S(A') M satisfying d{[a,b]) = ad (b ) - bd(a)

for all

In particular show that any mapping d: X a derivation of §(Ar).

a ,b ^^{X ).

g(A') extends uniquely to

1.19 Compute all automorphisms of the Witt and Virasoro algebras. 1.20 Let g be a perfect Lie algebra, and let § be its universal covering algebra. Prove that every derivation (automorphism) of g lifts uniquely to a derivation (automorphism) of §. 1.21 Prove all the results quoted without proof in Section 1.12. [Hint: See Lang, Algebra, Exercise p. 175.] 1.22 The following exercise, based on Bourbaki, covers the fundamental facts about solvable and nilpotent Lie algebras.

Lie Algebras

88

Let g be a Lie algebra over an arbitrary field IK. Recall that Dg := [g, g] is an ideal of g. Define decreasing sequence of ideals D®(g) d D^(g) D • • • and ^ T f\g ) 3 • • ♦ inductively as follows: (derived series)

D°( q) == g D"^*(9) = [D"(9)>D"(g)]

(central series)

for all n > 0

^ °(g ) = 9 ^ " ^ ‘(9) = [9, ^"(9.)]

for all n > 0.

(a)

Show that all the terms in these series are ideals of g that are stable under every derivation of g. (b) Let /: g i) be a Lie algebra epimorphism. Show that = 3% ii) and that /(-^"(g)) = Conclude that 3 g is the smallest ideal a of g making g /a abelian. Henceforth in this exercise we assume all Lie algebras to be finite dimensional. (c ) For a Lie algebra g show that the following conditions are equivalent N1: = (0) for some n ^ N2: There exists a decreasing sequence of ideals 9o ^ 9 ^ 9i ^ • ** ^ ^k = (0) such that [g, g j c g.^^ for all 0 < / < A:. N3: There exists a decreasing sequence of ideals g^ 3 • • • d g^ as in N2 and such that dim,,^ 9i/9/+i = 1 for all 0 < f < A:. N4: There exists N ^ N such that ad jCj ® ° ad = 0 for all 9. (d)

(e)

A Lie algebra satisfying the equivalent conditions of (c) is said to be nilpotent. Show that subalgebras, quotients, and central exten­ sions of nilpotent Lie algebras are nilpotent. Let K be a (K-space, and let x e Endj^(F). Consider ad x:gi(V) gl(V) by ad x : y [ x , y] — a : ° y — y © x. Show that for all A/^ e Z . a d : c ''( y ) - L ( ^ ) ( - 1)' X N —i oyoJC.i / =0 ^ ^

(f)

Conclude that if x is nilpotent so is ad x. Let V ¥= (0) be a K-space, and let g be a finite-dimensional subalgebra of gI(L) consisting of nilpotent elements of Endj^(L). Show that there exists i; e F, # 0 such that g • i; = 0. (Assume that the results holds for dimension < n '= dim g. If is a subalgebra of g of dimension m < n, use (e) and induction

Exercises

89

to conclude that some nonzero element of g/f) is annihilated by all of adf). Conclude that g has an n - 1-dimensional ideal ]^. If ;c e g \]^ , show that U •= {v ^ V\ii • u = 0} is a nonzero subspace of V that is A:-stable.) (g) (Engel’s theorem). Show that for g to be nilpotent it is necessary and sufficient that ad ;c e gl(g) be nilpotent for all x e g. [Use (f) to show that g has nontrivial center c. Now use induction on dim(g/c) and (d).] (h) For a Lie algebra g show that the following conditions are equivalent: SI: D"(g) = (0) for some n ^ S2: There exists a decreasing sequence of ideals g = go 3 g^ d • • • D g^ = (0) such that g,/g,+i is commutative for all 0 < / < A:. Such a Lie algebra is said to be solvable. Note that every nilpo­ tent Lie algebra is solvable. (i) Show that subalgebras and quotients of solvable Lie algebras are solvable. (j) If a is an ideal of g and both a and g /a are solvable (as Lie algebras), show that g is solvable. (k) Let g ¥= (0) be solvable. Show that there exists an ideal of g of codimension 1. 1.23 Let g be a finite-dimensional Lie algebra. Let ^ ( 9 ) == n

«=0

(See Exercise 1.22.) Show that for an ideal a of g, g /a is nilpotent if and only if a D T^"(g).

Chapter Two

Lie Algebras Admitting Triangular Decompositions Agathon: But it was you who proved that death doesn’t exist. Hey, listen—Fve proved a lot of things. That’s how I pay my rent. Theories and little observations. A puckish remark now and then. Occasional maxims. It beats picking olives, but let’s not get carried away... So—what else is new? A g a t h o n : Oh, I ran into Isosceles. He has a great idea for a new triangle. —Adapted from W. Allen’s “My Apology”

A lle n :

The Lie algebra gI„([K) can be decomposed in a rather obvious way into the sum of three subalgebras: the strictly upper triangular matrices, the strictly lower triangular matrices, and the diagonal matrices. This “triangular decom­ position” is a basic ansatz that appears in all the split semisimple Lie algebras, the Kac-Moody algebras, and the Virasoro algebra. A considerable amount of the basic theory of these various types of Lie algebras depends upon nothing but this triangular decomposition, and hence is common. In this chapter we develop the triangular decomposition theory. The technical definition that we adopt here in Section 2.1 was inspired by the work of Rocha-Caridi and Wallach [R-CW]. At the foundation of the representation theory of Lie algebras with a triangular decomposition are the highest weight modules, and particularly the universal highest weight mod­ ules or Verma modules of Sections 2.2 and 2.3. Section 2.4 considers the special case of the three-dimensional simple Lie algebra §I2(IK). It is hard to overemphasize the importance of the represen­ tation theory of this Lie algebra in the study of semisimple and Kac-Moody Lie algebras (also in physics!). The material of this section is used extensively in Chapters 4, 6, and 7. 90

2.1

Triangular and Weight Space Decompositions

91

A basic tool in representation theory is the notion of formal characters. These characters are essentially formal power series that assemble into a single expression all the information about the dimensions of the weight spaces of a given representation. The fact that oftentimes characters can be given by unexpected and remarkably beautiful formulas (see Section 6.4) is one of their fascinations. In Section 2.5 we introduce characters, derive the character formula for Verma modules, and relate it to the theory of parti­ tions. In Section 2.6 we introduce the module category & of Bernstein-GelfandGelfand (BGG). This category provides a natural setting for highest weight modules. All the modules in 0 have characters, and we can even make a ring out of them. There are various series, particularly a weak form of composi­ tion series, that are available for modules in 0 , and these series play an important technical role in the development. Section 2.7 deals with various notions of radical ideals for Lie algebras with triangular decompositions. Many of these ideals vanish in important cases, although there are difficult, and even unanswered, aspects to this which we will come in Section 4.5. The structure of Verma modules has turned out to be a rich and subtle subject, in both the Kac-Moody and Virasoro settings. One of the tools by which we may understand this is the Shapovalov form and Shapovalov determinant. We introduce these objects in Section 2.8 and then use them in Section 2.9 to develop the Jantzen filtration, a device that allows one to study the effect on the structure of Verma modules as the highest weight (the single characterizing parameter) is allowed to vary. The BGG duality of Section 2.10 introduces a new collection of categories of modules, and in particular a class of projective modules that allow us to see a remarkable duality between projective and Verma modules, on the one hand, and Verma and irreducible modules, on the other. This result is used in Section 2.11 to give a general result about the possible embeddings of Verma modules into Verma modules. In Section 6.7, where we specialize to the Kac-Moody case, we get definitive results on this. The results of Sections 2.9, 2.10, and 2.11 are not used until Section 6.6 and not at all in Chapter 7. For this reason they might well be skipped on first reading. 2.7

TmANGlJLAR AND WEIGHT SPACE DECOMPOSITIONS

Let ^ be an abelian Lie algebra, and let ^ qI(M ) be a representation of in a IK-space M. Let g 1^* (the dual space of 1^). A nonzero vector i; G M is called a weight vector of weight (relative to and tt) if for all A G

7r(h)v = <¡>{h)v.

Líe Algebras Admitting Triangular Decompositions

92

Recall from Section 1.8 that U(l^) may be identified with the symmetric algebra 5(^) of 1& and that any representation 17 of lifts uniquely to a representation tt of U(]^). Suppose that u is a weight vector for i) of weight . The linear mapping <^: 1^ ^ IK extends uniquely to a homomorphism : S(f|) ^ K. If hi, /12, . . . ,

are any elements of

then

••• *1*) = E «i<^(*i)‘'<^(*2)'" ••• where i = (/i, /2, . . . , ( 1)

^

tt( u) u

For each e

and a-^ e K, It follows that

= {u)v

for all w G 5(]^), i; G M.

define the -weight space

by

= {y G M \7r(h)v = (f>(h)u, for all /z e

.

Clearly is an 1^-submodule of M. Let 'f) be an abelian Lie algebra, and let ir: ij qI(M ) be a representa­ tion of We say that the 1^-module M admits a weight space decomposition if M = This sum is necessarily direct (see Proposition 1). The (f) for which ¥= (0) are called the weights of M relative to and tt. The set of all weights of M will be denoted by P(M), For each e 1^*, dim is called the multiplicity of in M and is denoted by mult^(<^). Evidently mult^( 1 if and only if is a weight. Proposition 1 Let ^ be an abelian Lie algebra, and let M be an f)-module admitting a weight space decomposition. Then (i) the sum is direct, (ii) every ^-submodule N of M admits a weight space decomposition, and moreover n N for 12// e f)*. Proof Let be a submodule of M. We have n A/^ for all e ]^* by definition. Let x ^ N and write x = where x"^ e and R is some finite set of distinct weights of M . l f R = {}, then x e O N = AT^. We show by induction on card R that each x"^ ^ Suppose that card R > 1, and let and (f>2 ^ R, (l)^ ¥= 02- Choose /z g so that i(/z) # 2(h)x =

52

s r \[4>2)

- 2Íh))x'‘‘ :N.

2.1

Triangular and Weight Space Decompositions

93

By the induction hypothesis we may assume that each component (f>2(h))x'^ e In particular so that ^ Applying the induction assumption again, it follows that each x"^ belongs to N and hence that N admits a weight space decomposition. This estab­ lishes part (ii). Now part (i) follows from the same argument when x is taken to be 0. □ Example 1 (^I„(IK)) Let Then has a basis ...,

be the set of all diagonal matrices in ^I„([K). where

0. *0 hi. '=

(1 in the ( k , A:) -position).

-1

*•0 / Let M = K", and let tt be the natural representation of (Example 1.6.4). Then

on M

0

(1 in the A:th position)

lo is a weight vector for ij with weight

< f > k { h j) =

k

0 1 [-1

given by

(

if /:

l

if k = j ,

=

+ 1,

if A: = ; + 1; j

=

Furthermore and M = weight space decomposition.

-

1.

showing that M admits a

Example 2 (The Virasoro Algebra) Let 93 = E“ = _oolKL„ 0 (Kc be the Virasoro algebra, and let = IKLq ® IKc. Think of S as an f)-module through the adjoint representation restricted by Then [L q, L„] =

94

Lie Algebras Admitting Triangular Decompositions

shows that L„ is a weight vector of weight A„, where A„ e 1^* is defined for all Me Z by An(^o) =«> A„(i) = 0. Since A„ = nAj, we have iB"'" = 93"'^' = KL„ if n # 0 and 93° = f). This shows that 93 admits a weight space decomposition relative to ^ Proposition 2

Let Q be a Lie algebra, and let ^ Der %be a representation o f an abelian Lie algebra as a Lie algebra o f derivations on g. (i) Suppose that g admits a weight space decomposition 9 = 0

9“

with respect to under the representation tt. Then (ia) for all a,l3 ^ f)*, [9“, 9^] c 9“"^^ (thus g is graded, as a Lie algebra, by the Z-span of its weights)-, (ib) U(g) admits a weight space decomposition {relative to the repre­ sentation o f on U(g) extending that o f b, on % {Proposition 1.8.3)), and for all a, /3 e U (g )“U (g)'’ c U ( g ) “ ^ ^ Thus U(g) is graded, as an associative algebra, by the Z-span of the weights o f g. Moreover this grading is the grading o f U(g) inherited from that of g in part (i) {Section 1.8, Remark 2). (ii) Suppose that g is generated as a Lie algebra {see Section 1.10) by a set of weight vectors Xj, j e J, with Tr{h)xj = 4>j{h)xj for each j and for all h e ]^. Then g admits a weight space decomposition g = ©g“ with Xj e Q'I’J and each weight a e LZj. In particular the results o f part {ia) apply to g and U(g). Proof Identify g as a Lie subalgebra of U(g) in the usual way. We know that every element of U(g) is a sum of products x^X2 . . . x ^ , where each x, e g. In view of the assumptions on g (in either part (i) or (11)), we can assume that each X; lies in a weight space, say, g“'. Then TT{h){xiX2...Xk)

=

ix^...TT{h)xj...Xk

= («1

+ak){h)x^X2...Xk.

2.1

Triangular and Weight Space Decompositions

95

Part (ii) and part (ib) clearly follow from this (for (ii) invoke Proposition 1 with g taken as an l^-submodule of U(g). Since for all x, y e g, [x, y] = - y;c we may deduce (ia) from (ib). □ Let g be a Lie algebra over a field K. A triangular decomposition of g consists of an abelian subalgebra (0) and two subalgebras g+ and g_ such that TDl: TD2:

g = g_© f| 0 g^; g+^ (0), [1^, g+] c g+, and g+ admits a weight space decomposi­ tion relative to f) (under the, adjoint representation) with weights a =5^ 0 lying in a free additive semigroup 0 + ^ ^*5 TD3: there exists an anti-involution a (i.e., antiautomorphism of period 2) on g such that
mj

The triangular decomposition is said to be regular if in addition the weight spaces of g+ in TD(2) are finite dimensional. Notice that the condition 0 ^ 0 + is equivalent to ( 2)

C + n (- ! 2 + ) = 0

and also that (3)

o-(g_) = g+.

Remark 1 We will usually refer to a triangular decomposition of a Lie algebra g as a 4-tuple (^, g+, 0+ , ir), where f),g+, 0+, and < t are as above. It will be understood that g_== cr(g+) and that g = g_0 ^ 0 g+. Sometimes we simply write g = (^, g+, 0+, c7)t o describe this situation. Let g be a Lie algebra admitting a triangular decomposition, and assume that the above notation is in effect. Let x e g+, a 0 0^_. Then [h,ax] = [crh, ax] = a[x, h] = —a{h)ax for all A 0 from which we see that a x e g l“. It follows that g_ admits a weight space decomposition relative to

96

Lie Algebras Admitting Triangular Decompositions

with weights in —0+; (4)

g_“ =
for all a e Q_^.;

and g admits a weight space decomposition relative to S+ (5)

with

if a e e + , if - a e if a = 0, otherwise.

Let Q be the group generated by We know that Q = (which is a lattice in 1^* whenever J is finite). We call Q the root lattice (regardless of whether or not J is finite). We call the a ^ Q for which g" ¥= (0) the roots of g (relative to 1^) and the corresponding spaces g“ the root spaces. We define the height function h tiQ ^Z by

ht\

^j^j] = H

This terminology, due originally to W. Killing in this work on finite­ dimensional simple Lie algebras, derives from the fact that for each h the quantities a{h) are the characteristic roots of ad h (which is obviously a diagonalizable transformation). There is some nonuniformity in whether or not 0 is to be considered as a root. Classically in the case of semisingle Lie algebras it is not, but in the more general context here it seems more natural to do so (as we have just done). For each root a, dim g“ is called the multiplicity of a and the set of all roots is called the root system of g rela­ tive to ^ ' = (t), Q^, a) and is denoted most commonly by A. Define A+= A n 0 + and A_= - A+. Then TD2 and (4) and (5) give us that A = A+u{0} U A_. We call A+ (resp. A_) the set of positive (resp. negative) roots of A. We call the diagonal subalgebra of the decomposition and g+ (resp. g_) the upper (resp. lower) triangular subalgebra of the decomposition. Remark 2 \i ^ = (1^, g+, 0+, a) is a triangular decomposition of g, then it is immediate that g _ , - 0 + , cr) is another. We call this the triangular decomposition opposite to S^. Example 3 (g = ^I„(K), n > 1). Let g+ (resp. g_) be the subalgebra of strictly upper (resp. strictly lower) triangular matrices. Let 1^" be the subalge­ bra of diagonal matrices in gI„(K), and let Ij = 1^" n §I„((K). B o th 't)" and are abelian subalgebras of gI„(IK). The triangular decomposition that we are looking for is ^I„(IK) = g_0 f) e g+.

2.1

Triangular and Weight Space Decompositions

97

Transposition X ^ serves as the anti-involution, pointwise fixing and interchanging g_ and To determine the roots, we introduce the matrix units 1 < /, j < n: Eij is the matrix with a 1 in the (i,;)-entry and O’s elsewhere. Let Cj,. . . , e be defined by

and let a^,. . . ,

Since

be defined by

+ • • • +£„ vanishes on 1^, it is easy to see that { (E « ie,)|Ja,- s K, £ a ,. = o} =

and hence that

a„_i is a basis of 1^*. For h e 1^*, [h,

= /t£,, - £,,£ = (s, - e ,)(;i)£ ,,.

For i < j this gives = (a , + ••• +aj_i)(h)Eij. Thus E^j e is a weight vector with weight a, + • • • +ay_i. Set Q+-= {Em,a,|m, e l\j} \{0}. Then 9+=

®

g: = 0

i<;

KE,j

is the required weight space decomposition. Of course Ej^ = Ejj has weight -{ai + • • • -\-aj_i) for all i < j\ and g_=

© i>j

KE¿j

is the weight space decomposition of g_. Thus ^I„(IK) admits a regular triangular decomposition. It follows that gI„(IK) also has a triangular decom­ position with the same g+ and g_ but with replaced by %. These two examples are the origin of the terminology. Example 4 (The Virasoro algebra) Referring to Example 2, set g+ = ^ ® Let Aj e 1^* be the weight of Lj. Then with Q+ = we verify TD l, TD2, and TD4 of our definition. Let a be the linear transformation defined by aLj = L_y, j ^ Z, = 0.

98

Lie Algebras Admitting Triangular Decompositions

This provides S3 with a regular triangular decomposition. Of course it is easy to modify this for the Witt algebra. Example 5 (The affine algebra ^ l2(IK) of type

See the Appendix.

Example 6 (Heisenberg algebras extended by derivations) Let a = a_ 0 Kc 0 a+ be a Heisenberg algebra so that and a_ are abelian subalge­ bras that are nondegenerately paired by the associated skew-symmetric bilinear from «/r. Suppose that there are bases {a^\ and {a}}, ; g J, of and a_ such that [ay, a\] = 5y^c (this is always possible if a is finite dimensional). Define cr by cr{aj)=a'j,

y e J,

cr(c) = c. Then axioms TDl and TD3 of the definition of triangular decompositions are fulfilled with = Kc. However, is the centre of a and hence cannot produce the root spaces required by TD2. Just as in Example 5 this problem is easily cured by enlarging 1^^. For each i e J and integer g Z+, we let d be the linear operator on a defined by ¿(a,) = d¿a¿, d{a\) = -d^a\, d\i^^ = 0. Then d is di derivation of a. We let if •= if^ ^ Kd = Kc ® Kd and make f i : = a 0 l K d = a _ 0 ] ^ 0 a + into a Lie algebra containing a as a subalgebra by defining (Exercise 1.3) [d, x] = d{x)

for all X G a ,

[d,d] = 0. Then, if we define a g 1^* by a(c) = 0, a(d) = 1, and set = E^.=^IKa„ k a we see that a has a weight space decomposition with a+= i< — ka ij = a . After extending cr to a by a(d) = d, « - = ®;t>0 a (]^, a+, Z^_a, cr) is a triangular decomposition of a with root lattice Q = Za. The problem that was raised in these last two examples, namely that of extending the algebra in order to produce more eigenspaces, is one that we will see again in our study of affine Lie algebras. Remark 3 Later on in the text (Section 2.9) we will find it useful to have the notion of triangular decomposition for Lie algebras over rings. Suppose that ^ is a commutative ring of characteristic 0 (i.e., Z is a subring of AX Let fj be an abelian Lie algebra over A that is free as an .^4-module (Remark 1 of Section 1.1). Set r

= H o m ^ (^ ,^ ).

2.1

99

Triangular and Weight Space Decompositions

Suppose that M is a free ^-module that is also an 1^-module. We define the weight space /x e 1^*, just as above: := {y e M\h • V = ii{h)v for all h

,

M has a weight space decomposition if M = The sum is necessar­ ily direct. Let g be a Lie algebra over A that is free as an ^4-module. A triangular decomposition of g consists of an abelian subalgebra f) and two subalgebras g+ and g_ of g (all free as ^4-modules) for which TD1-TD4 hold. Let g = (]^, g+, (2+, a) be a Lie algebra over A with triangular decomposi­ tion. Let jB be a commutative ring containing A, and let g == B 0^ g be the Lie algebra over B obtained by extension of the base ring from A io B (see Section 1.1). Let 'i) = B and g+= B 0^ g+. These are subalgebras of g that are free as S-modules. Every ^ induces an ^-bilinear map : i5 X by At: (6,/ï)

biJi{h),

and hence an ^-linear map (also denoted ¡lI) /1: B 0^ f) ^ 5 . One verifies that ]I is jB-linear, and hence there exists an (injective) group homomorphism "ril* ^ 5 * . Along similar lines one shows that there exists a unique antiinvolution â of g satisfying a{b

0jc)

= b

0

ot( a:).

Then is a triangular decomposition of g which is said to be obtained from (1^, g+, Q^, a) by extension of the base ring from A to B, The most obvious examples are when g is defined over the field IK and IK' is some extension field of IK. Example 7 (Complexification of a real triangular decomposition) Let g be a Lie algebra over the real numbers IR. Assume (1^, g+, Ô+, a ) is a triangular decomposition of g. Let gc '= C 0ff^ g be the complexification of g. Then evidently g^ = (gc)-® ® (9c)+ ^be obvious notation) and, with as the C-linear extension of a to g^, (^ c?(9 c)+ j Ô+? a triangular decom­ position of g^ (see the preceding remark). However, it is convenient for

100

Lie Algebras Admitting Triangular Decompositions

Other purposes to extend a to a semilinear map so that cr(ojc) = acr{x) for all e C and for all x e g. We denote this extension, which is unique, simply by cr, and we call the 4-tuple the hermitian complexifícation of(l^,g+,(2+>i^)- The real subalgebra 5 of g^ is recovered as the set of fixed points of a- in Conversely, suppose that we are given a complex Lie algebra m, an abelian subalgebra f, and a semilinear anti-involution cr on m that stabilizes f. Let be the set of fixed points of a in f. Then if is a real form of f since, for any jc e f, we have x = l/2 ( x + o-jc Kix + aix)). The 4-tuple (f, m+, Q^, a ) is called a (regular) hermitian trian­ gular decomposition if it is the complexification of a (regular) triangular decomposition (^,g+,j2+,o-)of some real form g of m. Note that Q^czi^* and ]^* can be thought of as the real subspace of f* consisting of those functions that are real valued on i). We will see in Chapter 4 that all the affine algebras, and indeed the far wider class of contragredient Lie algebras, possess regular triangular decom­ positions that are fundamental to their study. Proposition 3

Let q be a Lie algebra admitting a triangular decomposition (^, g+, Ô+, (r), and suppose that 9=

© 9"

aGA

is the corresponding root space decomposition. Let be an automorphism o f g stabilizing Then (¡) maps root spaces onto root spaces. More precisely (f|) = Í), cind if (f>*: ]^* -> Í)* is defined by *(/) = f°(f>~^ for all f ^ 1^*, then 0(g") = g"^*“ for all a ^ A. In particular * determines by restriction a bijectiue mapping o f A onto itself. Proof Let CKe A, jc e g", and H

which shows that

e g° = 1^. Thus

Then

Now

and hence (x) e Together these show that (f> maps root spaces into, and hence onto, roots spaces in the desired way. It follows that <^*A = A. □ The group of automorphisms of g that stabilize f) will be denoted by Aut(g, ij). Let Aut(A) := { e AutK(i|*)l<^(A) = A}.

2.1

Triangular and Weight Space Decompositions

101

Proposition 2.3 gives rise to an exact sequence \

K ^ A ut(g, ]^)

Aut(A).

Let 6: Q ^ be a group homomorphism (from an additive into a multi­ plicative group). There exists a unique e Aut(g, 1^) such that /elg“ = scalar multiplication by ^(a) . We define KQ ={f,\e^H om {Q ,K ^)}. Clearly K q

c

K,

Proposition 4 [B el]

Let % be a Lie algebra admitting a triangular decomposition (i), Q+,Q+,(t ). Suppose that dim < oo and dim < dim g+. Let D q c Der(g) be the deriva­ tions of g stabilizing each root space o f g. Then Der g = D q + ad g and D q n ad g = ad 1^. Proof Let 5 be any derivation of g mapping ^ into 'i). Then for any root a and any e g“ we have for all e a{h)8x'^ = which we write as (6)

(ad/i - a ( h ) l ) 8 x ^ = ~ [ 8 h , x ^ ] e g“.

If 8x°" were to have some component in g^, /3 ^ a, then with /t e such that p(h) a (h \ we have a contradiction to (6). Thus 6g“ c g“, and hence 8 e D q. It is obvious that D q n ad g = ad 1^. Let dim ^ = n, and let ..., ^ A+ be arbitrary. We can find a basis {hy, . . . , /i„) of f) such that a^ih^) = 1, i = l , . . . , n . In fact proceeding inductively, if linearly independent h^,...,hf^_^ have already been chosen so that afhi ) = l , i = 1 , k - 1, then set •= {h e ^ a f h ) = 0}. Since cannot be written as the union of two proper subspaces, we can choose X

+ •••

UH^}.

Then hi^ := x / a j f x ) is as desired. Now let basis of g+ taken so that each Xj^ lies in some root space g“^, e A+, A: e S. Let {h,^}f^^^ be a subset of such that ^k(^k) = 1

for

k ^ S.

102

Lie Algebras Admitting Triangular Decompositions

By the above we can assume that spans 1^. Evidently {crAc^l^es is a basis of g_. Let d e Der g, and define bf^j e K and h\ e by

Since dim dO)) < «>, and b/^j are zero except for a finite set of values of j (independent of k). In particular ajj and bjj are zero except for finitely many j. From o = d[h^,h^] = [dh^,h^] + [h^,dh^] we have

- b^jaj(h^) + b^¡aj(h^) = 0

for all p, q, j.

With p = j, ^ pp^ pV^p )

^qp^

^pp^pi^q)

^qp’

Let ------ E«ppO-JCp + 'LbppXp e g. P

Then for all

P

^ S, [^^>3^] “

p P

^J^pp^p{j^q)^p P

= Hagpcrxp + T^bgpXp P

P

= d h ^ ~ h',, so we have (d + a d y ) ( / i J = A ' , e ^ . Then d' •= d proposition.

ad y: if

if, since the {h^} span 1^, so d' e D q, providing the □

As an example one may easily show that every derivation of the Virasoro algebra is inner (Exercise 2.24).

2.2

Highest Weight Modules

103

2.2 HIGHEST WEIGHT MODULES Let 9 be a Lie algebra over K admitting a triangular decomposition (1^, 9+> Q+, and write g = g_0 0 g+. Let tt be a representation of g on a space M. We know from Section 1.8 that ir lifts to a representation of U(g) on M. If y is a vector in M, then 7r{n(q))v

{7t(

u

)

v

\u

is a submodule of M [since it is closed by the action of 7r(g)], and indeed it is the smallest submodule of M containing v. We call it the submodule of M generated by v, A nonzero vector z; e M is called a highest weight vector for g (relative to the triangular decomposition) if (i) z; is a weight vector relative to the action of 1^. (ii) tt{ x ) v = 0 for all X g g+. A g-module M is said to be a highest weight module if M contains a highest weight vector u that generates it. The weight A g ]^* of the highest weight vector v is called the highest weight of M. We call the pair (A, z;) a highest weight pair of M. The representation of g on M afforded by M as a g-module is called a highest weight representation. Remark I We will see shortly (Remark 2) that highest weight vectors of a highest weight module are unique up to nonzero scalar factors. In particular all highest weight vectors have the same weight. In addition all the other weights will be seen to be “lower” than A (Proposition 2.1). These two facts justify the above terminology. Highest weight modules occur very frequently in the sequel. Although in detail there are many differences between highest weight modules for differ­ ent Lie algebras and many subtleties to be understood, the broad features are quite uniform. In the physics literatures as well as in many mathematical papers, highest weight vectors are called vacuum or null vectors. Let M be a highest weight module affording the representation tt and with highest weight pair (A, z;). Using the Poincaré-Birkhoff-Witt theorem, we have U(g) = U(g_)U(]^)U(g+). Thus M = 7r(U(g))z; = 7T(U(g_))7r(U(^))7r(U(gJ)z; = 7r(U(g_))7T(U(^))z; = 7r(U(g_))z;,

Lie Algebras Admitting Triangular Decompositions

104

where the last equality is a consequence of the fact that is a simultaneous eigenvector for 7t(U(]^)) = [see 2.1(1)]. According to Proposition 2.1.2 and 2.1(4), g and U(g) admit weight space decompositions with weights in Q and are also graded by Q. All the weights of g_ lie in -Q+, and those of ll(g_) in -(2 +^(0)Let P be a subgroup of 1^*. A (2 +-fan in P is any set of the form A I 0 + - {A} U {A -/3li3 e 0+}, where A e P. We call A the source of the fan. Fans are useful objects for keeping track of the weights of representation that we will study. Note that Q-U{0} = 0 i Q ^ Proposition 1 Let q be a Lie algebra admitting a triangular decomposition (ij, Q+,Q+,cr), and let Q denote its root lattice. Let M be a highest weight module with highest weight pair (X,v) and ajfording the representation tt. Then (i)

(ii)

(iii)

M admits a weight space decomposition relative to where all the weights lie in the fan A i Q^. Furthermore = '7r(U(g_)““)i;/or all a ^ !2+^{0}. In particular = Ko. the weight space decomposition o f part (i) defines a grading o f M by ZA + Q and, for each a ^ ¡2? 9“ tind U(g)“ act as homogeneous operators o f degree a on M. if the decomposition o f q i s regular, then all o f the weight spaces o f M are finite dimensional.

Proof By the preceding remarks, M is spanned by vectors of the form v{u)v, where u e U(g_)“", a e (2+Li{0}. We have (1)

Tr{h)7r{u)v

=

\'Tr{h),'Tr{u)\v

+

=

—a { h ) 7 r { u ) v - \ - \ { h ) T r { u ) v

'Tr{u)7r{h)v

= (A —a){h)Tr{u)v, which shows that M is spanned by weight vectors and hence has a weight space decomposition. In addition it shows that = 7r(U (g_)"“)o and that all weight spaces of M are of this form. (Since modules are by definition graded only by groups, we use the group ZA + (2 for the grading even though it is clear that all the weights lie in the coset A + Q.) That U(g)“ and g“ act homogeneously is clear from (1).

2.2

105

Highest Weight Modules

Finally, suppose that the decomposition of g is regular. Now U(g_) has all its weights in O iQ ^, and except for U(g_)® (= K.l), each weight space U(g_)”^ is spanned by products x ^ .. . Xf^ of weight vectors with weights -Pi, e - Q ^ and p = • -\-p¿. Since there are only finitely many ways to decompose p ^ Q+ into parts that are also in Q+, and since dim g l" = dim g““ < oo for all a e Q_^, we see that dim U(g_)“^ < oo. Thus = 7r(U(g_)“^)¿; is also finite dimensional, and this proves part (iii). □ Remark 2 The use of the terminology highest weight is now apparent. A is a weight and all other weights are “lower” because they are of the form A - a, a e (2_^. Proposition 1 shows that A and IK¿; are unique. Indeed, if w is a highest weight vector for M of highest weight ¡jl, then \ —a = (fjL — P) — a for some a, P ^ (2 + U{0}=>a+)S = 0 => a = p = 0 => fi =A. Then dim = 1 => Kw = Ki;. Example 1 (The Natural representation of §I„([K)). We use the notation established in Examples 1 and 3 in Section 2.1 with M = K" and tt the natural representation of ^I„(IK) on M. Then M = is a weight space decomposition of M. Since E^je^ = 0 for all i < j, g+Ccj) = 0, so is a highest weight vector. Since for / = 1 ,..., n, M is generated by ej, and hence M is a highest weight module. The weights are 2 = 0i All the weight Oil, 3 = i - a 2 , . . . , (f>n = i - Oil - ' spaces are one dimensional. Remark 3 It is a fact that if K is algebraically closed, all finite-dimensional irreducible representations of ^I„(1K) are highest weight modules. Example 2 (Heisenberg algebras) We return to the Heisenberg algebras of operators described in Section 1.4. Thus a is the linear span of the operators /(xy), d/dxj, and 1 acting on 5 = Let j j be any map of J into Z+. Let a_= ElK/(jCy), a+= T.Kd/dxj. hct the degree operator D be defined on S by ...,

for all monomials in S. Thus Xj is given degree derivation of 5 (see Example 1.5.1), and [d, K ^ j ) ] f =

. . . , x "Jnk k

= («1/, + • • • + n j.

Let

= - h j f + Xjdf - Xjdf =

d

•= —D. Then d is a

-¡l(xj)f

for / e 5 shows that [d,l(xj)]= —jl(xj). Similarly [d,d/dxj] = jd/dxj. Thus d be­ haves like the extension element of Example 6 of 2.1 and fi — Kd 0 a is a Lie algebra of operators on S with triangular decomposition a _ 0 0 a+, 0 K l.

106

Líe Algebras Admitting Triangular Decompositions

Consider 1 ^ 5 . Evidently where A e 1^* is defined by

1 = 0 and h • 1 = \(h)l for all h

A(l) = 1,

X(d) = 0.

1, we see that 5 is a highest Since also <* weight module. It is quite easy to see that it is irreducible, but we leave the proof of this until Section 2.3. Let a e 1^* be defined by a ( l) = 0,

oi(d) = 1.

Then ..., is a weight vector of weight A + ••• It follows that the weights of 5 lie in A - Na. Except for = K ^ 1, the weight spaces need not be finite dimensional unless J is finite. Proposition 2 Highest weight modules are indecomposable. Proof. Let M be a highest weight module with highest weight pair (A, y). Suppose that M = ® M2, where and M2 are submodules of M. Then =

Mf e

forces either = (0) or M^ = (0). Say, M^ = (0). Then v : M^ so that M = U(g) • V c Mj, and hence M2 = (0). Remark 4 In general highest weight modules are far from being irre­ ducible. We will see this explicitly in Section 2.4. Remark 5 Analogous to highest weight modules we may define lowest weight modules M. In this case M is generated by a lowest weight vector (G_* = 0, • i; c K v ), and the weights of M lie in upward fans of the form At!2+- Lowest weight modules for g with triangular decomposition Q+, 0-) are evidently highest weight modules for g with the opposite triangular decomposition (see Section 2.1, Remark 2).

2.3

VERMA M O D U LES

In this section we show how to actually construct highest weight modules for Lie algebras with triangular decompositions. In fact the modules that we construct are universal in the sense that all other highest weight modules occur as homomorphic images of them. They carry natural (contragredient) bilinear forms (see Section 2.8), which are used later in the book to gain insight into questions of submodules and irreducibility.

2.3

Yerma Modules

107

We begin with a Lie algebra g admitting a triangular decomposition The root lattice will be denoted as usual by Q. Unless explicitly assumed, the decomposition need not be regular. Let M be a highest weight module with highest weight vector v and highest weight A. In this section we will put more emphasis on modules than representations. We will not usually specify the representation explicitly but will simply write jc • w to denote the effect of the operator defined by jc e g on an element w of M. Suppose that g_ has a basis of root vectors indexed by some totally ordered set J. For each ; e J let e —Q^ denote the root corresponding to Xj, that is, Xj e g^>. Then, by Proposition 2.2.1, each of the vectors Y^k V, (1) Z+, is a weight vector of M of where A: > 0, ‘ ’ * > h, ^ weight A + + ••• and collectively they span M. We are going to show how, starting with any A e ]^*, we can construct a highest weight module M(A), as above, for which the vectors (1) form a basis of M(A). We will also see that such a module is unique up to isomorphism. Let A e A highest weight module M(A) for g with highest weight pair (A, i;+) is called a Verma module if given any highest weight module M with highest weight pair (A, v) (the same highest weight A), there exists a g-module homomorphism r¡: M(A) ^ M such that v, A Verma module is universal in the sense that every highest weight module with the same highest weight is a homomorphic image of it. It is clear that the homomorphism rj in the above definition is unique [for the pair (A, i;)] and surjective: for if v, then for all u e U(g_), u * u • v;on the other hand, M = U(g_) *v. Also M(A) is itself unique up to isomor­ phism by the standard type of argument (see Section 1.2). The existence of M(A) will be shown in two different ways. The first is by the method of inducing modules. The second, which is more prosaic, is much more explicit and gives one a better feeling for what the module looks like. It also takes more work. Proposition 1 Let (]^, g+, ¡2+, a ) be a triangular decomposition o f g. Then, for all A e 1^*, g has a Verma module M(X) o f highest weight A. Proof 1. Let b be the subalgebra 0 g+ of g. Let Kv+ be a one-dimen­ sional vector space and make it into a b-module by defining g+* v += 0, h • Vj^= \{h)u^

for all /r e ]^.

Líe Algebras Admitting Triangular Decompositions

108

Now IKd+ is a left U(b)-module and U(b) is a subring of U(g)- Hence we may form the induced module obtained from by extension of the base ring from U(b) and U(s) (see Section 1.1, Remark 1) M(A) == U(g) ®u(6)IKt;+. Clearly, M(A) is a left U(g)-module, and hence a g-module. Consider 1® A/(A). For X e g+, X • (1 ® Ü+) = 1 ®



and for h /i • (1 ® Ü+) = 1 ® /1 • v + = 1 ® A(/i)i;+. Also U(gXl ® y+) = U(g) ®u(b)IKi’+= Af(A). Combining these, we see that M (\) is a highest weight module with highest weight vector 1 ® of weight A. Let M' be any highest weight module with highest weight vector v' and highest weight A. The mapping / : U(g) X f ( u , av^) = au ■v', is bilinear and U(b)-balanced: Namely for w s 11(b), f(uw,av+) = au • w • v' = f { u , w ■av^). Hence there exists an induced linear mapping /: U ( 9 )

+

satisfying u (S> au • v'. This is a U(Q)-niodule map, and it satisfies 1 0 i; + L?' as desired (see [BA2] for more on tensor products). □ Before starting on the second proof we isolate the following fact which we will use several times in the sequel. Lemma 2 Let A e 1^*. Then (2)

U(g) = U (g _ ) e |u ( g ) g + + £ U(9)((* "

2.3

Verma Modules

109

The reader may wonder about the notation ~ which the sum is incredibly redundant. Evidently the sum may be replaced by a sum over any basis of f). Proof. The mapping A:

IK extends uniquely to a homomorphism A: 5 (^ )

whose kernel is

IK

~ A(/z)l) (Exercise 1.9). Thus 5 (i|) = K 0

L 5 (^)(/г - A (/i)l).

Let b_!= b ® 9_, and recall that (PBW theorem. Corollary 2), U(b_) is a free U(g_)-module admitting any IK-basis of U(b) as a U(g_)-basis. Now the triangular decomposition and the Poincaré-Birkhoff-Witt theorem gives us U(g) = U (g _ ) U ( b )U ( g J = U (g _ )U (b )(K l® U (g J g + ) = U (g_)U (b) ® U (g)g^ = U (g_)(K ® E U ( i ) ( A - A ( / i ) l ) ) ® U (g)g^ (because U(b) = 5 (b )) = U (9_) ® E U (b_)(/i - A (/i)l) ® U (g)g^ Asf) (because U(b_) is a free U (g_) module). Now 9+(/i —A(/i)l) c U(g)g^ since g^. is an b-module under the adjoint representation, and thus U (g)(/i - A (/i)l) c U (b_)(/i - A (/i)l) + U (g)g^.



We now give the second proof of Proposition 1. Proof 2. Let p :U (g ) ^ U ( g _ ) be the projection determined by the direct sum decomposition (2) of U(g).

lio

Lie Algebras Admitting Triangular Decompositions

The kernel of p is clearly a left ideal of U(9>- Define an action of U(9) U(g_) by y-u= p(yu)

for all Me U (g_), y e U (g).

This makes U(g_) into a U(g)-module: Let y', y e U(g), u e U(g_), and write yu = piyu) + r, where p(.r) = 0. Then y' • (y • m) =p{ y'p {yu )) = p {y '{ yu - r)) = p(y'yu) = (y 'y ) • u, since y'r is in the kernel of p. For u', u e U(g_), u' ' u = p{u'u) = m' m, and therefor the action of 11(9_) on itself is left multiplication. Thus U(9-) is generated by 1 as a U(g)-module. For all y G U(g+), y • 1 = p ( y ) = 0, and for all

e ]^, /z • 1 = p{h) = p(A (/i)l + h - A(/z)l) = A(/z)l.

This shows that U(g_) has been made into a highest weight module with highest weight vector 1 and highest weight A. If M' is any highest weight module with highest weight pair (A, v ' \ then the kernel of p annihilates v'. Thus the mapping U(g_) ^ M', u• a g-module map showing that U(g_) (as a g-module) is a Verma module.

□ Remark 1 It is clear from Proposition 1 (especially the second proof) that, as U(g_)-modules, M(A) = U(g_) and M(A)^”“ = U(g_)““, where the ac­ tion on U(g_) is left multiplication. We see that as U(g_)-modules, all the M(A)’s look the same, namely like U(g_). It is the actions of and U(g+) that are different. Since U(g_) is an domain (Proposition 1.8.5), we have the important fact that a Verma module M = M(A) is a torsion-free U(g_)-module; that is, for u e U(g_), m ^ M, (3)

w • m = 0 <=> M= 0 or

m = 0.

Any homomorphism of M(A) that is not injective annihilates some nontrivial

2.3

Yerma Modules

111

element u • v, u ^ U(g_) \ {0}. Therefore we arrive at the following impor­ tant conclusion: Proposition 3 Let M be a highest weight ^.-module. For M to be a Verma module it is necessary and sufficient that M be torsion free as a \liQ_)-module [i.e., (3) holds], O Remark 2 If M is a Verma module, then as a U(g_)-module it is monogenic ( = cyclic) and torsion free, and hence free. Corollary Any submodule of a Verma module that is itself a highest weight module is a Verma module. From the left U(g)-module mapping U(g) ^ M ( A ) , u ^ u • u ,. we conclude that M(A) = U ( g ) //( A ) ,

(4)

where /(A) is the annihilator of in U(g). From (3) and the second proof, we see that (5)

/(A)

=U(9)g^+ ElI(s)(^-A(/i)l).

Often (4) and (5) are used to define Verma modules. The next result shows us that irreducible highest weight modules exist and are unique. Proposition 4 Let (^,g+,!2+jOr)

^ triangular decomposition o f g, and fei A e 1^*.

(i) I f M ( \ ) is the Verma module o f highest weight A, then (ia) every proper submodule N o f M ( \ ) has a weight space decomposi­ tion relative to and the weights lie in A —0+j (ib) M(A) has a unique maximal proper submodule MA); (ic) L(A) := M(A)/MA) is irreducible, and up to isomorphism, L(A) is the unique irreducible highest weight module o f g with highest weight A. (ii) Any highest weight module M with highest weight A contains a unique maximal proper submodule N. Furthermore M /N = L(A).

112

Lie Algebras Admitting Triangular Decompositions

Proof, (ia) If A/" is a submodule of M then in particular N is an 1^-submodule of M. By Proposition 2.1.1, N has a weight space decomposition with weight spaces n M If A is a weight of N, then = «1;+ and then N = M, since generates Af as a g-module. Thus, if N is proper, all the weights of lie in A — (ib) Using (ia), we see that the sum A^(A) of all the proper submodules of M is still proper (since none of them can contribute to M^). This establishes (ib). (ic) L(A) = M(X)/N(X) is clearly a highest weight module with highest weight A, and since A^(A) is maximal, it is irreducible. Let L' be any irreducible highest weight module with highest weight A. Then, since M(A) is a Verma module, there is a nonzero homomorphism 77: M(A) with M{XY for all weights (j) of M(A). We have already seen that rj is surjective, and therefore its kernel is a maximal proper submodule of M(A). Thus ri(N(\)) = 0 by part (ii), and M(A)/iV(A) = L '. (ii) From the universal property of M(A), there is a surjective homomor­ phism M(A) M. This takes weight spaces to weight spaces from which it is clear that N ( \) maps to a proper submodule N of M. Then N is maximal, and M / N = M{k)/N{k) = L(A). □ Example 1 (Verma modules for Heisenberg algebras) Following Example 2.1.6, assume that a = a _ 0 lK c 0 a + is a Heisenberg algebra with an anti-involution a and bases {fly}, (cr(fly)} (; e J) of and a_ such that [fly, cr(fl^)] = 8jj^c j, A: e J. We extend a to & = a _ 0 0 a^_, where = IKc 0 Kd and where [ d , fly] = fly, [d,a(aj)] = —o -(fly ) so that fi acquires a triangular decomposition with root lattice Q = Za(a e 1^* given by a(c) = 0 and a(d) = 1). Let A G ]^*, and let M(A) be the Verma module for fi with highest weight pair (A, ¿;+). Then M(A) = is the corresponding weight space decomposition of M(A). We have M(A) = U(a_) ♦v^A = U(a) • and the annihilator .^4 of v, in U(fi) is U (a )a ^ + Vi{a){c - A(c)) + Vi{á)(d - k ( d ) ) . This is the content of (5) for this example. Thus M(A) = Vi(&)/A.

2.3

Yerma Modules

113

If we restrict the representation to a, then the annihilator ^ of U(a) is quite easily seen to be

in

U (a)a^+U (a)(c-A (c)), and M(A) = U(a)//4. Since we end up with the same representation space [i.e., M(A)], whether or not we adjoin d to a, it is worthwhile to comment on its role. The element c e is central in a (and in a) and consequently acts as scalar multiplication by A(c) on all of M(A). Indeed for u e U(a), c -( m - i;+) = w *c *i; += A(c)w • i;+. Thus c is unable to decompose M(A) into its characteristic form as a one-dimensional “highest” weight space and a sum of weight spaces of lower weights. The element d does not have this defect, and as we saw already, leads to the decomposition 0M(A)^“'*'^. It is primarily because we want these kinds of weight space decompositions that we have formulated the definition of triangular decomposition as we did. Of course û = û _ 0 lK c 0 û + is not a triangular decomposition [it violates axiom TD2]. We return to our discussion of M(A) as an d-module. We propose now to show the following: (7)

If

A(c) # 0,

then

M(A)

is irreducible.

We introduce some terminology: A multi-index is an element n e i^l'^of finite support. If , «i j are the nonzero values of n. A: > 0, . . . , ^ J, then we write

a" |n|

for the operator <2"^* • • * for the operator for and n! for

on M(A); on M(A);

In this notation a basis for M(A)^“ '^“ is the set of elements +, |n| = r. We have the following inductive calculations in U(a): (8)

[a,.,o-(a^)”] =

V,

n e Z+,

m

(9)

=5,7«

m ,n r=l

114

Lie Algebras Admitting Triangular Decompositions

Thus, if m > « > 0, flX fly )" •

[a^,(r(aj)"]v^ = 8¡jncaf’-^a(ajY~^ • v+ =

• Ü+

_ j 8¿jn\c'^ • \0

by (9)

by induction

if m = «, in m > n .

It follows that for multi-indices m and n with |m| = |n|, ( 10)

if m

0 \ n!c'"‘ •

n (then for at least one j, nij > rij)

if m = n.

It is now easy to see that M(A) is irreducible. Let r e Z+, and let X = Ze^a'!. ■

e„ e K .

Then for any multi-index m with |m| = /*,

ÍZ™ •X =

•v ^ = m!e^A(c)*^ •v + G: N ( X ) ^ = (0).

Thus each ^„ = 0 [if A(c) # 0], and hence x = 0. As for M(0), (10) shows that • u += 0 whenever |m| = |n| > 1, and hence is a submodule of M(0). Obviously this submodule is maximal, and hence is MO). We conclude that L(A) =

(M(A) ([

i f A ( c ) ^ 0, if A(c) = 0.

Example 2 (The Virasoro algebra of Example 2.1.4). The diagonal subalge­ bra of the Virasoro algebra is two-dimensional with basis L q and 0. Thus any linear functional A on is determined by the two values /i :=A(L q)

and

c — A(0).

We denote the corresponding Verma module by M = M{h, c) and a highest weight vector by Since 0 is in the centre of S3, we have 0 * x * i ; + = x * 0* u^= cx ‘ for all X e U(S3). Thus 0 acts as scalar multiplication by c on

2.3

115

Yerma Modules

M. With Ai e ]^* defined by A^CLo) = 1 and A^Cc) = 0, we have M = Using the Remark 1 the Poincare-Birkhoff-Witt theorem applied to the ordered basis L _ i , L _ 2, . . . of SS_ we find that a basis of is the set and

V^\n^
= n |.

The problem of determining the maximal submodule N{h, c) of M(/i, c) is quite complex (see the references in Section 2.8). Remark 3 There is obviously a lowest weight analogue of Verma modules. Verma modules for g with the triangular decomposition are lowest weight Verma modules for g with the triangular decomposition and vice versa. Proposition 5 Let g have triangular decomposition (f), g+, o-) and let = be its opposite triangular decomposition {see Remark 2.1.2). Let ( tt, M ) be any representation o f g. We define a pair ( tt^, M^) consisting of a K-space and a mapping g ^ gl(M ^) as follows: • as a vector space, • for X ^ V Ei

= M, 7t ' ^ ( x )

v

=

-7 r(a (x ))v .

Then (i) (tt®", M^) is a representation o f g; (ii) ((7r^)^(M -)-) = (7r,M); (iii) = M~^ for all /1 e ]^* Furthermore M is an ^-weight module if and only if is an ^-weight module’, (iv) N (zM is a (¿-submodule relative to ir if and only if •= N

=

(p,h)v,

—Tr{o’h)v = ( p , h } v , <=>

7r(h)v

=

(



p,h}v.

e 1^, for all

e M

116

Lie Algebras Admitting Triangular Decompositions

Again (iv) is trivial, and for (v), (A, y+) is a highest weight pair for Af(A) <=> U+ G M^, v + ¥= 0, Tr(Q^)v + = 0,

M = ir(U (g))i;+ , « D+e

0

tt'^{Q-) v +=

0,

M‘^ = 7T(U(g))£;^, <=><—A,i; + >

a highest weight pair for M.



Now (vi) follows from (iv) and (v).

2.4

^l2(K)-THEORY

We recall the Lie algebra ^I2(1K) consisting of 2 x 2 matrices of trace 0 with entries in K. The representation theory of this Lie algebra is of the utmost importance for the theory of semisimple Lie algebra. A basis {E, H, F} of §I2(IK) satisfying the relations [H ,E ]= 2E ,

[H ,F ]= -2F ,

[E,F]= H ,

is called an § 12-triplet. We recall that ^I2(IK) = K f 0 Kh 0 Ke, where

/=(;

2 ).

- ( i

-M '

«=(2

D-

As we saw earlier, {e, h , f ) is an § 12-triplet. Evidently if we set §_;= [K/,

:= Kh,

§ += Ke,

and define an anti-involution a on ^l2([K) by transposition, then we have a regular triangular decomposition ^I2(1K) = ^_0

0 ^+

with Q+= Z+a, where a(h) = 2 (Section 2.1, Example 3). Let A 0 f)*, and consider the ^I2(1K)-Verma module M(A) of highest weight A. Fix a highest weight vector of M(A). Then by Propositions 2.2.1

2.4

117

ёКСЮ-ТЬеогу

and 2.3.3. = K /" • +^ (0),

for all

n ^ N.

It follows from Proposition 2.1.1 that any submodule R of M(A) is either (0) or has the form for some Hq > 0. In the latter case e -/"0 • y + = 0.

(1)

Conversely, if Hq is a positive integer for which (1) holds, then we see that /'^0 • is a highest weight vector and U(g) *u += U(^_)/''o • +c M(A) is a proper submodule of M(A). We conclude that the (unique) maximal proper submodule MA) of Af(A) is generated by the highest weight vector /"0 • ¿;+, where is the least positive integer satisfying (1). Lemma 1 Let \(h) = a e K. Then for all n ^ N, (i) /z • /" • u^= (a - 2n)f^ • (ii) e • /" • z; + = n{a — n + 1 )/" “ ^ *z;+, where we make the convention that f~^ ‘ v += 0. Proof (i) follows from the fact that / " • +e M(A)'^“"". We prove (ii) by induction on n, it being clear if n = 0. For n > 1 we have e

• ü+= [ e , / ] • / " ^ - v ^ + f - e - f n - l • V, = (a — 2(n — 1) ) / " ^ • y + + (/i — 1)(л — n

2) / " ^



= n(a —n + 1) / ” ^ v +. Proposition 2

Let M(A) be the Verma module for §12(Ю with highest weight pair (A,z;+). Then (i) M(A) is irreducible if and only if \(h) ^ 141; (ii) if A(A) e 141, then N ( \ ) is a Verma module with generator and highest weight A —(A(/z) + l)a. The irreducible module L(A) is of finite dimension X(h) H- 1 and is the only nontrivial quotient module of M(A). Proof Let a = A(/z). After the preparatory remarks and Lemma 1, we see that M(A) is reducible if and only if По(л —«0 + 1) = 0

for some n^ e Z^_.

118

Lie Algebras Admitting Triangular Decompositions

This is possible if and only if a e I4j and п^ = a This shows (i) and also shows that equation (1) has precisely one solution whenever a e N. In that case M(A) has only one nontrivial submodule, namely ЖА), and MA) is generated as a highest weight module by ' v Thus MA) has highest weight A —(a + l)a. Since (A —(я + \)aXh) = —л —2 e Z _ , it follows from (i) that the Verma module M(A —(a + l)a ) is irreducible, and so MA) is a Verma module, namely MA) = M(A - (a H- l)a) (Proposition 2.3.3). If M(A) ^ L(A) is the natural homomorphism [with kernel MA)], then {/^ • Ü+10 < 7 < й} is a basis for L(A). □ The finite-dimensional irreducible highest weight modules L(A) are pre­ cisely those for which A(A) = a e N. We sometimes denote L(A) by L(a) if \(h) = a. In the physics literature these modules are often denoted simply (a) or (a) [and also unfortunately by their dimensions (a + 1)]. If v+ denotes a highest weight vector of L(A), then we have the basis (2)

v^,f ■

and corresponding weights A,A —a,A —2 a , . . . , A — aa = —A. The values of the weights at h form the symmetric string (3)

a,a - 2,a - 4 , . , , , - a .

Trivial though it may seem, this symmetry will eventually lead us (in Chapters 4, 5, and 6) to a complete theory of symmetry in root and weight systems of Kac-Moody algebras. If we set у _=/"* • i;+, then, up to scalar multiples, the vectors in (2) can be written e"* '

'v

v_,

which displays L(A) from the point of view of a lowest weight module. Another way to look at the symmetry is to interchange the roles of e and / in the triangular decomposition (and then to replace й = [e,/ ] by —h = [/, e]). Then L(A) is a highest weight module with highest weight vector v_ and highest weight -A ( - A (- A ) = д). One of the central results of the classical theory of semisimple Lie algebras is Weyl’s theorem, which states that their finite-dimensional repre­ sentation are completely reducible. Eventually we will prove a version of this theorem (set in a much wider context). However, we will find it useful to have the result for §12(Ю much earlier. The proof that we present here is in essence the same as the more general one that will appear in Chapter 6. We will make use of the concept of primitive vectors, a subject that is more fully developed in Section 2.6.

2.4

SljOlO-Theory

119

Let M be an §l2(lK)-module admitting a weight space decomposition relative to IK/z. A weight vector v e is called a primitive vector if there is an §l2(lK)-submodule N oi M such that u ^ N and such that e • v ^ N, For instance, highest weight vectors are primitive [with N taken as (0)]. Proposition 3 Let K / 0 K/z 0 Ke be the triangular decomposition o f §I2(1K) described above, and let M be a finite-dimensional ^l2(K)-module admitting a weight space decomposition M = 0M ^ (p 0 1^*) relative to f). Then M= © L„ ¿=1 where each is an irreducible ^i2(K)-module isomorphic to L(A^) for some = /¿a, I f e N. The decomposition is unique to the extent that the collection (Aj,... , \jf) of highest weights is unique up to rearrangement. To prove this result, we introduce the element (4)

C = |/z2 + e/ + /e

of U = U(§l2(IK)). The next lemma says that this element lies in the center 3(U) of U. In general, elements of 3(U) for semisimple g are called Casimir operators. However, there is always a quadratic Casimir operator like (4) which is essentially unique and is usually called the Casimir operator. We will never have occasion to use any other. (In Section 4.5 we will introduce quadratic Casimir operators in a far wider context.) Lemma 4 C lies in the center of U. Proof It suffices to show that [e, C] = [/, C] = 0, since e and / generate §I2(IK) and hence U. We have [e,^h^ + ef + fe] = \{ [e ,h ]h + h{e,h]} + e { e , f ] + [ e , f ] e = —eh — he The case of / is similar

eh

he = 0. □

Suppose that F is a highest weight module for §I2(1K) (relative to a given triangular decomposition), and let be a highest vector of weight A. Let

120

Líe Algebras Admitting Triangular Decompositions

a = A(/z) e IK. Then C •f

f

++ e •/ • +

=

+ /e ) • f +

= { W + «)í'+Also for all MG U, C • M•

u ' C ' v^= [\a?’ +

• v^.

Since i;+ generates F, (5)

C V=

+ a)v

for all f g F.

Proof (of Proposition 3). For some algebraic extension IK' of IK all the eigenvalues of C acting on M lie in IK' [if IK is algebraically closed, then IK' = IK]. Let M' = IK' M. Then M' is a module for the Lie algebra IK' ^ ^I2(1K) = §I2(IK'), and C can be interpreted as an element of 301'), where U' == U(§l2(IK')). From M = we have M' = 0(IK' ^ M ^ \ Each space M'^ •= IK' 0^^ is a weight space for 1^' — IK' % 1^, from which it follows that we have produced a weight space decomposition of M' relative to f)'. Let t be an eigenvalue of C with corresponding generalized eigenspace M' := {i; G M '|(C - i)^ • = 0 for some A: > 0} (see Section 7.1). Then Af' is an §l2(lK')-submodule for M' since C g 301')- In particular it is 1^'invariant and hence decomposes into weight spaces M[^ '= M[ n M'^. If VG then e ' V E: (where we are identifying §I2(W inside §I2(IK') via X 1 0 x). In view of the finite dimensionality of M' over IK', there can only be finitely many nontrivial weight spaces, and hence there is a weight ¡i and a weight vector u g \ {0} such that e • ¿; = 0. Now is a highest weight vector, and in particular a primitive vector of M'f. Let us show that for any primitive vector w of weight v in Af/, we have ( 6)

K/t)

and

j v { h f + v(h) = t.

Let AT be a submodule of M'„ with w ^ N, e ■w ^ N. Then on w + N ^ M't/N, C acts as multiplication by \v(,hY + v{h), and hence C • w = (\v{h)^ + v{h)^w mod N. Since (C —i)* • *v = 0 for some A: > 0, we obtain \ v i h y + vih) = t. Since v

2.4

121

gl2(IK)-Theory

is a highest weight for the finite-dimensional quotient module M¡/N, v{h) by Proposition 2. This establishes (6). Now (6) shows that there is only one primitive weight in M/, namely above, and that a — e N. In particular t e K. Thus all the eigenvalues of C lie in K, and the extension of K to K' is unnecessary. Let u \ , . . . , be a basis for M^. If e • 0, then + /:a is a highest weight for some A: > 0, contradicting our observation above about primitive weights. Thus for each i, L,(/¿) == U • is an irreducible ^l2(IK)-module isomorphic to Liix). It follows that n (Ey^,U • = (0) (since iv{) and that R = ® L j ( f i ) CM,. ; =i Consider the quotient module M^/R. It is a finite-dimensional §l2(W-module with a weight space decomposition on which C acts as multiplication by t. The argument above shows that if it is not (0), then it has a highest weight v. Then V is 2i primitive weight of M ,, and hence it is equal to ¡ by (6). But { M J R Y = M>t/R^ = (0). Thus R = M„ and jl

(V)

© Lj(jx).

y=l

From M = (the sum taken over all the eigenvalues of C) and (7), we have the decomposition of M into irreducible submodules, as required. For the uniqueness property we consider the composition series k

k

M = © Ly D © Ly D y=l y= 2

э L ^ э (0)

(i.e., each submodule is a maximal submodule of the previous one). By the Jordan-Holder theorem (which is a very general fact whose scope lies far beyond Lie theory) the factors

j=i + \

are unique (including repetitions) up to the order in which they appear. [Ja2, 3.3]. □ Remark 1 It is quite impossible to expect any stronger uniqueness in the decomposition of a module into irreducible submodules. For example, the module M — L 0 L also decomposes nicely as L + 0 L_, where L = =

122

Lie Algebras Admitting Triangular Decompositions

{(i^, ± ^ L). However, one does have uniqueness of the isotypical com­ ponents (the Af, in the preceding proof) [Ja2, Thm. 3.11]. CoroUary 1 Under the hypotheses of Proposition 3, the Casimir operator C acts as a semisimple transformation on M with eigenvalues of the form \a^ + a, a The eigenspace of M is the sum o f all the irreducible submodules isomorphic to L{a) [the L(a)-isotypical component]. Example 1 Consider ^I2(1K) c gl2(lK). The adjoint representation, adgi^^^^^, restricted to ^I2(1K) determines a representation of ^Í2([K) on gl2(IK). We do not need to invoke Proposition 3 to conclude that gÍ2(W is completely reducible: clearly gl2(lK) = IKl e ^I2(1K). As a preview of what is to follow below, we explicitly describe the corresponding representation of 5L2(IK). Let A" g gl2(IK). Then ad = L x — R x ’>where L x and R x are, respectively, left and right matrix multipli­ cation by X. If X is nilpotent, then exp ad A" = exp(L;^ —R x) = exp L;^(exp — R x) = exp L ; ^ ( e x p s i n c e L x and R x commute [in End(gÍ2(IK))]. In other words, for all Y e gl2(IK), (exp ad X \ Y ) = exp(AOexp(y)exp(AT)“ ^ As we will see, this shows that the representation of SL2QÍ) on gl2(W is p i - X ) : Y ^ x Y x - ^ for all x e SL2(K). The Lie group associated with the Lie algebra ^l2(K) is the special linear group SL2ÍK)

ad-bc = 1 .

-{l(:

Any of the finite-dimensional §l2(IK)-modules that we have been discussing above carries a natural compatible 5L2(lK)-module structure. We begin with a noteworthy fact about the representations of §I2(1K). Let denote the space of 2 X 1 column vectors with coefficients in K, and let ir be the natural representation of §I2(IK) on it (i.e., acting as matrix multiplication). Then in and let fact K ^ s L(l) in our notation above. Let M= ^ j j , i ; = | ^ j i rm Then S is graded by 5 = 5([K^) be the symmetric algebra on the space Z, 5 = following Section 1.2, 5'^ =

© Ku^vL i +j = n

Each X e §I2(IK) lifts to a derivation on S, say, X (Proposition 1.1.5), and it is immediately clear that [X,Y] = [X,Y] [both are derivations extending [AT,y] e §I2(IK)] showing that we obtain a representation on S. Since X(S") c 5", we obtain a representation of §I2(IK) on each 5", n = 0,1,2,... .

2.4

§ 12(1K) -Theory

123

Proposition 5 Let n ^

Then ( tt^, 5 ”) is an irreducible ^l2ÍK)-module isomorphic to L{n).

Proof. The case « = 0 being obvious, we can assume that n > 0. Let {e, h, /} be the standard basis for §I2(IK). Then for all X e §I2(1K), = nu^ ^tt{ X ) u . Since

(s

m^i i )

and

we have 7T„(e)w" = 0, 7T^{h)u’^ = nw". Thus is a highest weight vector of weight n for §I2(1K), and the result follows from part ii of Proposition 2 and the fact that dim 5" = « + 1.

□ Now we extend the action of SL2(K) to 5(IK^) in an analogous fashion. Again, let 77 denote the natural representation of 5L2([K) on Each X e SL2(K) determines a linear mapping on ® ••• 0 (« factors) by i;j 0 • • • 0 7r(jc)i;i 0 • • • 0 v(x)u^, and hence on the tensor algebra T(IK^) by linear extension [where on T([K^)° = K, the action is trivial]. Thus 5L2(IK) acts as a group of automorphisms of r([K^) (as an associative algebra). Since it stabilizes the ideal J generated by the set of vectors y 0 w - w 0 y , y,w e we have a group action 77 of SL2(K) on 5(1K^) = T(K^)/J (see Section 1.2) with tt( x )( v ^ • • • v^) = irix)v^ • • * 77(jc)i;„. Let ^ Then 7T^ is our desired representation of SL2(K). Using the isomorphism 5" —L(n), we have an action of 5L2(IK) on L(n). Next we study in what sense t7„ is compatible with t7„ [see (8) below]. Let X e §I2(IK) be a nilpotent matrix; that is, X ^ = 0 for some /: > 0. In fact = 0, fc > 0 => (K^ d ATIK^ d AT^IK^ = (0) the containments being strict, so X ^ = 0. Relative to some basis {u^, U2) of IK^, A", as a linear transformation, has the matrix form ( ^ ^ |, whence exp AT = 1 + X + ( : : ) ' ATV2! + • • • is similar to “j, which shows that exp X ' 5L,

124

Líe Algebras Admitting Triangular Decompositions

Lemma 6 For all nilpotent X e §I2([K) and for all n ^ N, and

( 8)

is nilpotent on L(n),

expir„(A') = ■j7„exp(X).

Proof. We may take S" as our model of L(n). For Mj, . . . , m„ e ATe SI^OK),

and

n

^ n ( ^ ) ( “ i • • • « « ) = L «1 • • • ATwy • • • u„, J=i

and one sees inductively that 7T„(Xf(u, ■■■ U„)=

E . , *,+ ••• +*„=* '^1---- '^n-

•••

It follows at once that if X is nilpotent, so is tt„(X), and that

expv „(X )(u i • • • « „ ) = E — k _

— ( “ i ••• u„) _

X ’^^

X^-

k A:i+ • • +A:„=A: ^1* = exp X{u f) • • • exp X(u^) = 'n-„{expX)(ui ■■■ u„).



We say that an §l2(K)-moduIe (p, F ) is integrable relative to the basis {e,h, f ) if V is decomposable as a direct sum of IK/i-weight spaces and pe and p f are locally nilpotent on V, Proposition 7 An integrable ^l2(K)-module (p, F ) can be written as a direct sum o f finitedimensional irreducible ^l2(K)-submodules, In particular (p, F ) is completely reducible. For every nilpotent element X e §I2(IK), p{X) is locally nilpotent. The space V admits a unique SL2(K)-representation p with the compatibility condition (8)

exp p { X ) = p(exp X )

for all nilpotent X e §I2([K).

2.4

êl2(K)-Theory

125

Proof. If f e K is a [K/z-weight vector, then the êl2(lK)-submodule generated by V is ¿,;>0

(by the PBW theorem), and this is finite dimensional because of the local nilpotence of pe and p /. Thus W is completely reducible by Proposition 3 and it follows that F is a sum, hence direct sum, of finite-dimensional irreducible submodules of êl2(K) (Proposition 1.6.2). Using Lemma 6, every nilpotent X e êl2(lK) is locally nilpotent in its action on V. Furthermore the Lie algebra action êl2(IK) on each irreducible submodule W of F “integrates” to an SL2(K) action, as we described above, and the compatibility condition (8) holds on W. Piecing the representations together in the direct sum, we have a representation p of 5L2(IK) on F which is compatible with p. The uniqueness of p follows from the fact to be shown immediately below that

{(i

o)L ““ ((!

2)},.K

form a set of generators of the group SL2(IK).



We now gather together some useful facts about SL2(IK). Define B ==

a 0

b a-*

H -=

t 0

0

\b ^ K

0 - t -1

AT:=//U

t e

It is easy to see that each of these is a subgroup of 5L2(IK), that H
(o

!)(-!-■

?)(o

;)■ (-?-'

shows that the set i(A - { ( i

#\/l

n\

;)■!(:

Î)

te K

o)

126

Líe Algebras Admitting Triangular Decompositions

generates the element n{t) and hence also the matrices

( 10 )

h( t) ■■=n ( t ) n ( l ) ' = 1^

t^K ^.

j

Given an arbitrary matrix A =

* e 5L2(IK), we want to reduce it to 1

by left multiplications by elements of U. Applying n(l) if necessary, we can assume that a 0. After applying

1 —ca~^

0 1

we can assume that A =

a 0

b a-^

Then /i(a-i)y4 = | j

and

= 1.

We have proved the first part of Proposition 8 (i) U generates 5L2(IK). (ii) SL2(K) is generated by B KJ N\ and H = B C\ N, (iii) 5L2(1K) =

^

(Bruhat decomposition).

Proof. It remains to prove parts (ii) and (iii). From (9) we see that U lies in the subgroup of 5L2(IK) generated by B and N, whence the first part of (ii). Obviously B n N H. Set

=(-?

i)-

Notice that s is a representative for the nontrivial coset of H in N. After part (ii) we will prove part (iii) if we show that B U BsB is closed by right

2.4

SijiW -Theory

127

multiplications by elements of N. Since N = H U Hs, this reduces to showing that sBs (Z B U BsB. In showing this, we may replace each occurrence of 5 by any element that we wish from the coset Hs = sH of H in N. Using (9), we see that

1 -r-i

0 G BsB 1

for all t e

Thus for all t e Let a typical element of B be written as

[l

/-)(J

S i G K.

!)•

Then

^( o

which is what we wanted.



Parts (ii) and (iii) of Proposition 8 express a basic ansatz, which we will see fully developed in Section 6.3. An interesting application of Proposition 8 is to use it to prove the following. Proposition 9 The only proper normal subgroups o f SL2(K) are

( ( i ;)}

-

(

m

:

:)}■

The same proof {due to J. Tits) may be used to prove that many other groups are ''essentially"’ simple [773]. Proof Suppose that K # 5L2(K) and that AT is a normal subgroup of SL2(K). Consider the subgroup BK. Since it is a union of .B-double cosets, BK = B, or BK = SL2{K). The latter implies that SL2(K)/K = B K / K = B/B n K, However, is a solvable group; hence also B / B OK , whereas 5L2(IK) is its own derived group, and the same goes for SL2(K)/K. These are

128

Lie Algebras Admitting Triangular Decompositions

contradictory, so we have BK = B\ that is, B Z) K. However. /

0 1

l\la 0 /\0

feW

0

-1 \ 0/

\ —b

0 a

. A trivial calculation with shows - ( : : ) □ that fl = +1. Thus K has the required form. and hence K c

( : ; - )

Corollary The action of 5L2(1K) on 5" is faithful if n is odd and has kernel {±1) if n is even. Proof By Proposition 9 the kernel is either trivial or is {± 1}. Since

the result is clear.



2.5 CHARACTERS Suppose that M is a vector space which is graded by an abelian group P and for which the degree subspaces are finite dimensional. In many situations we can, or would like to, make useful numerical statements about all of these subspaces at once. For instance, we might like to know the dimensions {dim or we might have a homogeneous linear operator T of degree 0, and we might be interested in the traces (tr(r|A/a)}^gp (of which the dimensions are the special case for T = id^). As a simple example consider 5(K), F = K x 0 lKy, asa Z-graded module under the total grading. Then 5(K) == IK[x, y], and the degree subspace S%V) of elements of degree n admits the monomials

as a basis. Thus dim S%V) = n + 1. This information is neatly stored in the formal power series (1)

E (« +1)9"/1 = 0

This series goes by various names: the Poincare series of (the Z-graded module) 5(K) or the generating function (for the dimensions of the degree

2.5

129

Characters

subspaces) of 5(K). We often call it the character of 5(K), for reasons to be explained later. The use of the word “function” in this context is not to be interpreted to mean that (1) is some real or complex valued function of q. Of course such an interpretation might be useful (in which case questions of convergence appear), but our only intention at the moment is to consider (1) as an element of the formal power series ring K[[^]]. Part of this section is devoted to a basic introduction to power series. For the moment it suffices to say that (1) is an invertible element in the ring K[[q]] and that its inverse is (1 - qY. The ring structure of K[[q]] is manifestly useful when we go on to consider the graded algebra K[x, y, z]. Regarding [K[x:, y] and K[z] as subalgebras of K[x, y, z], the space K[x, y, z T of elements of degree n in K[x, y, z] is E K [x ,y M zr"^ / =0 and (2)

dim(IK[x, y, z ] ”) = ^ dim(lK[x, y]')dim(lK[z]" i= 0

Clearly the generating function of K[z] is E7=o^' = (1 —^) \ and hence by (1) and (2), the generating function of K[x, y, z] is -3

n=0

n=0

Induction on dim V quickly shows that the generating function of SiV ) for dim F = m is (3)

(1

It is not hard to expand this as

(!-«)■” -

£ j" '

We now establish a suitable generalization of this for treating jP-graded spaces. Let P be an additive abelian group. We let e{P) = [e(a)\a e P}

130

Lie Algebras Admitting Triangular Decompositions

be a multiplicative copy of P; that is, we define e(a)e(P) '■=e{a + P ) ,

a,P ^P .

The elements e(a) are called formal exponentials. Given a commutative ring R, we define P[P] = Re(a) to be the free module over R with basis e(P). Then R[P] becomes an associative i?-algebra with 1 — e(0) as the identity element if we define a multiplica­ tion by (4)

H

a^P

a„e(a) • E /3e/>

= E ( E a +^ =y

'

R[P] is called the group algebra of P with coefficients in R. If M is a finite-dimensional P-graded space, then M has only finitely many nontrivial degree spaces, and we can define the generating function or character of M by ch(M ) = i ; dim M“e (a ) e Z [P ]. Unfortunately, most of our graded spaces are not so simple, and we have to extend Z[P] to express their characters. To this effect let us assume the following. (5) There exists a nonempty family {yy}y of elements of P indexed by a set J such that the group Q •= Ey^jZyy is freely generated (as an abelian group, by the {yy}yej* Under this assumption we let denote the semigroup of Q generated by the 7y’s. A typical example of this situation is Q+= \ {0} in Q = Z^. Assuming (5) is in effect, we define sl Q +- fan in P to be a set of the form U {A - ^ 1^ e (2 +}, where A e P (Section 2.2). We call A the source of the fan. We introduce a partial ordering < on P by setting / x
2.5

Characters

131

we define the support of / by su p p (/) == {a e Pla„

0}.

Notice that R[P] = { / ^ R[PT\supp(f) is finite}. We cannot supply R[PT with a composition law by simply extending (4) because meaningless infinite sums of elements of R will arise on the right-hand side. Consider, however, R [ P i Q ^ ] ■■= { /=

a ) e jR[P]"^|supp(/)lies in a finite number of ¡2+-fans|,

and J.0+] == { / = £ a „ e ( a ) |s u p p ( / ) lies in A J. g + j , where A is an arbitrary element of P. Both R[PIQ+] and i?[0i<2+] become associative algebras under (4). Indeed let / = La^eia), and g = Lb^eip) lie in R[P j Q+] with supp(/) c (J (a, i(2 + ), 1=1

supp(g) c U j=i

Let 5 ^ P, and consider writing 8 = a p, a e supp(/), p e supp(g). Then 8 = pj - e ^ (a^ + Pj)i Q^, where s is the sum of two elements of C+U{0}. By the assumption on <2+ we see that there are only finitely many ways of writing 8 in such a manner. Thus

a +(B=8 is a well-defined sum and (4) makes sense. Clearly R[0i Q+l is a subalgebra of R [ P i Q j . For each A e F we define ^[■Pi!2 + ] ( A ) ~ { E « a ^ ( “ ) ^ R[P i Q +] \ ^a = Ofor all a rel="nofollow"> a). Let { /J/ei

^ family of elements of R[P iQ+], and write fi=

£ « « ,« (« )•

a^P

132

Líe Algebras Admitting Triangular Decompositions

We say that the above family is summable if the following two conditions hold. (51) There exist , A„ in P such that supp(/,) c (J J=i(Ay i Q_^,) for all i e I. (52) For all A in F there exists only a finite number of i in I for which /; i R[P i Q ^ \,y Proposition 1 Let R[P I Q

be as above.

(i) Two elements x and y o f R[P iQ ^ ] are equal if and only if x = y mod R[P i !2+](a) ^ (ii) If (//)/ei ^ ^ summable family o f elements o f R[P IQ+] with f = there exists a unique element f = of >10 +] that a^ = ^i^ts sum has only finitely many nonzero terms). Proof (i) is straightforward. (ii) Let a ^ P. Then =>f^ ^ R[P>IQ+](«). Axiom S2 then shows that the sum E^ei^a, ¡s finite. Consider / == e R[PT • By SI we see that supp(/) lies inside the union of a finite number of fans. Thus f^R [P iQ ^l □ The element f ^ R[P i Q+] defined in Part (ii) of Proposition 1 is de­ noted by E, ei//Now suppose that M is a P-graded vector space with finite-dimensional degree subspaces such that all nontrivial degrees [degrees a for which M“ (0)] lie in a finite union of 0+-fans. Then we define the character of M by (6)

ch(M) = £ dimM“e( a ) e Z [ P i 0 + ] . a^P

All important case of this is the situation where M is a highest weight module of highest weight A for a Lie algebra g admitting a regular triangular decomposition (f), g+, Q+, a). Then M is graded by the group P = ZA + 0, where 0 is the root lattice, so that (5) holds for this choice of 0 , and all nontrivial weights of this weight space decomposition lie in the 0+-fan A i 0+. Also by Proposition 2.2.1 all the weight spaces are finite dimensional because of the regularity of the triangular decomposition. The character (6) is

2.5

Characters

133

thus defined. Likewise we may define (7)

ch(g_) =

Y.

dim g “e ( - a ) e Z[Oi g +]-

It is primarily because of this type of example that it is more convenient to base fans and the definition of IK[0i (2+1 on - Q + rather than Q+. The use of the word character in this connection has its origin in the complex representation theory of compact Lie groups. In this situation is a finite-dimensional abelian Lie algebra over R, and there is associated with each h ^ if an operator on the complex space M whose action on the weight space M" is multiplication by [whereas h acts as multiplication by a(h)]. The operators form a compact abelian group T, If M has finite dimension then tr^ = E d i m M “e^“^^\ The mapping tr^(e^) is a character : T ^ C (in the sense of group theory). We have a formal version of this with e(a) replacing the function e" : -> We can try to define ch(M) as a function on i) through h

Y dim

cc(h)

This of course raises very interesting questions of convergence and the rate of growth of the dimensions of the weight spaces, which we do not treat in this book. The ring R[0i 2+] is easily identified as a ring of formal power series. Let the basis of Q+ given in (5). Each a ^ Q+ has a unique coordinate representation in terms of the y/s: ( 8)

ri:y: + JrJi

Jk'Jk'

The coordinates n = (itj) are elements of (mappings of J into [^) for which ftj = 0 for all but a finite subset of J. Let Xj •= e(-yj). Then for a with coordinates n as in (8) e { - a ) =x;/i... which we denote simply as x". Then

where the sums run over all coordinates of elements of 2 +u{0}. As we have already mentioned, these are formal sums involving (in general) infinitely many nonzero coefficients. The most common situation is with J = {1,..., m} in which case each monomial x" and /?[0J,2+] is the well-known ring of formal power series in m commuting variables, R[[xi,. . . , x^]]. We will also have

134

Líe Algebras Admitting Triangular Decompositions

occasion to use the case J = In both cases the exponential and monomial notations are useful, and we work with them interchangeably. Generally, when we are using the monomial notation, we will denote R[0i Q+]hy i?[[jc]] or The first question that we settle is which elements of R[[x]] are units (i.e., have multiplicative inverses). For m = (rrij) ^ (2 +*-^{0} we define k l := Recall the partial ordering < defined earlier. For m, n ^ ¡2 +^(0}? m < n if and only if

for all i.

Let R[[;c]]" be the R-span of the elements X*" for which In particular

lm| = n.

= R.\.

Proposition 2 For / = ^ ^[[^]] to be a unit, it is necessary and sufficient that üfi a(0, . . . , 0) be a unit o f R, I f f is a unit, then its inverse g = Ebm*™ ^ recursively defined through

(9)

L

aA-

r + s = m, s < m

Proof Writing fg = l leads directly to (9). If a^ is a unit, these equations admit a unique solution which is found inductively on |m|. If a^ is not a unit, then there is no solution to a^bQ = 1, and hence / is not invertible. □ A particularly important instance of this is the well-known (10)

(1 - x ) ~ ^ = l + x + x ^ +

.

We have already pointed out the expansion {i-x)

- £ (



)* ’ .

We will have a number of occasions to write down product expansions (11)

n (i+ /,).

2.5

Characters

135

where /¿^R[[x]\ and / / = (i.e., = 0). These products make sense if we assume that for each n e Q + there is a finite subset D(n) of J such that = 0

whenever j ^ D(n)

and

m < n.

Indeed in that case only finitely many /, can contribute to the coefficient of a given monomial x". More precisely the coefficient of x" in n (1 +//)

is independent of S provided that S d D(n). This coefficient is then the coefficient of x" in (11). Consider the rather natural looking product ( 12 )

n ( i + « 0 ^ »<[[«]]•' y=l

This has an expansion L Poin)q", n= 0

and Po(n) has a simple and beautiful combinatorial interpretation. The coefficient Po(n) of was already established by the time we expanded

fl(i +^0-

y=l

Since expanding this product amounts to forming simple products by choos­ ing either the 1 or the from each factor, we see that p^in) is the number of sequences 1 < 7i < 72 < **• < Jr

such that E-=i 7/ = n, that is, the number of partitions of n into distinct parts. In the same way if m^, m2, . . . belong to N and we write (13)

n ( i + «0 ^= L r ( n ) g " , ;=i

then r(n) can be interpreted as being the number of partitions of n into ^The use of q rather than x^, or simply x, is to conform with the standard notation used for partition functions in the literature and elsewhere in the book.

136

Lie Algebras Admitting Triangular Decompositions

distinct parts where the number j may be considered available in different colours. For example,

y=l

generates the partitions of n into distinct parts where the odd numbers are of two colours but then even numbers of just one colour. Suppose that we distinguish the two types of odd numbers by plain and bold fonts. Then, for instance, the coefficient of is 6, with the actual partitions being 4,31,31,31,31,211. The above partitions are restricted; this means that we can use each part only a limited number of times. The product (14)

0(1-90 ; =i

= E p («)9"

enumerates the unrestricted partition function: p(n) is the number of se­ quences j\ <J 2 < • • • <Jr,

with

= n. To see why, expand each factor of (14) using (10) to get

{l + g + q^ + ■■■)[! + q^- + ( q ^ f +

+q^ + { q ^ f +

Now interpret the /cth factor (1 +
1

1 part of size k 2 parts of size k <->

2

Then any given monomial

is interpreted as the partition 1 . . . 1 2 . . . 2 . ..A:...A: Si

$2

Sf^

ofn =

,

2.5

137

Characters

and the entire expansion has the interpretation as the generating function of the unrestricted partition function. To interpret (15)

n ( i -« 0 ; =i

>

m,

we imagine that each integer j is available in rrij “colours.” This is the generating function for the number of partitions of n into parts where we may use each positive integer any number of times and also with any combination of colours. If rrij = 0, then j cannot be used in any partition (i.e., j is not available in any colour). For more on partitions, see [HW] and [An]. We come now to the main results of this section. Proposition 3

Let n be a Lie algebra graded by an abelian group P for which the following conditions hold, (i) All the nontrivial degrees lie in —Q+ where Q+ is a semigroup o f P satisfying (5); GO For all a e •= dim n ““ is finite. Let U(n) be the universal enveloping algebra o f n with the inherited P-grading {Section 1.8). Then ch(U(n))=

n

(1

Proof. Let [yj}jej be the given basis for <2+- Let i;*., A: e K, be an ordered basis of n consisting of homogeneous elements, say, g n “**, 8 ^ ^ Q+Then according to the Poincare-Birkhoff-Witt theorem, the products (16)

ki< ...< k„

form a basis for U(n). On the other hand, the expansion of (17)

r i ( l - e ( - 8, ) )

-1

A:eK

enumerates all the products (18)

e ( - 8 , y “' . . . e { - 8 , y \

k,< ...
138

Lie Algebras Admitting Triangular Decompositions

The coefficient of e ( - 8 ) in (17) is thus the number of products (18), with

which in turn is the number of products (16) that lie in U(n)“^. Since every a appears times among the 5y’s, the proposition follows. □ Example 1 (Abelian Lie algebras) As a simple example we take a finite­ dimensional vector space a with a basis and consider it as an abelian Lie algebra. By Proposition 1.8.1 U(a) is naturally isomorphic to the symmetric algebra 5(a). If we set Q = Z, Q+= Z+, a~^ = a (all elements have degree —1), and q = e( —1), then Proposition 3 gives ch (5 (a))= (l-« )

-N

which is precisely what we had deduced before in (3). If instead we set Q = Z", ¡2+= \ {0}, = (0,..., 1,.. ., 0) (1 in the ith place), and = KXi, then we have a completely different grading, and

ch(5(a)) =¿=n(l-K-a,))“‘. 1 An immediate consequence of Proposition 3 and Remark 1 of Section 2.2 is the character formula for Verma modules: Proposition 4 Let q be a Lie algebra admitting a regular triangular decomposition. Write 9= ^ ® 9+, and let Q denote the root lattice. Let ch(g_) =

L " !« « (-« ) ^ Z[04, e + ] . a^Q^.

Then (i) ch(U(g.)) = - K -a))-"*« e Z[01 (ii) for each A e 1^* the character o f the corresponding Verma module M(A) is given by ch(M(A)) = e(A) n where P = Z \

Q,

( l - e ( - a ) ) " ' ”“ e Z [ P i < 2 j

2.5

139

Characters

Just as with (15) we can give the product in Part (i) of Proposition 4 a combinatorial interpretation: ch(U(g_))=

E K{ p ) e { - I 3 ) , j8eQ+u{0}

where K(p) is the number of partitions of ¡3 into parts a ^ Q+ and 1. each a ^ Q+ occurs in different colours, 2. each a ^ Q+ of each colour may be used any number of times. This gives rise to a function K:Q (defined to be 0 outside Q ^) which is called the Kostant partition function [Kol]. Example 2 (§I2(K)) We have §I2(IK) = IK/ 0 Kh © Ke graded by Q = l a c ]^* with / of degree —a. For A © 1^*, M(A) = 'L n > o ^ f * where u+ is 3. highest weight vector, and by Proposition 4, ch(M(A)) = e(A)(l - e ( —a))~^ =

^ ( A ) + ^ ( A — Of) + ^ ( A — 2o f ) + * * * .

Example 3 (The Virasoro algebra) We use the triangular decomposition of S3 given in Example 2.2.4 with SS_= ^ ® where Ai(L q) = 1 and A/c) = 0. Let q = e(-Ai). Then 1KL„ = and ch(SS_) = n= \

Let (19)

e ]^*. Then

ch(M(/x)) = e(/i,) n (1 /2

=1

\

and we see from (14) that dimAf(/i,)'^ ' ' ^ = p { n ) , where p{n) is the partition function. This agrees with the explicit basis constructed in Example 2.3.2.

140

Líe Algebras Admitting Triangular Decompositions

The final example is an application to the theory of free Lie algebras. Suppose that card X = m < oo. According to the discussion in Section 1.10, there are two natural gradings of S (^ ), one by Z in which every element of X has degree 1 and one by ß = 2 '”- The next result gives formulas for the dimensions of the degree subspaces with respect to each of these two gradings. We do not need these formulas in the sequel, and they can safely be omitted. Proposition 5 [Witt] Let X be a set o fm elements^ and let S(AT) be the free Lie algebra on X over K. Let pi be the Mobius inversion function. Then (i) for all n

^ r\n

(ii) for all m-tuples, n = (n^,. . . , n^) of nonnegative integers

where r|n means that there exists a positive integer k such that nj = krj for all j = 1, . . . , m, and in that case n / r — k. Proof Both parts are proved in essentially the same way using a result from the exercises. We give the proof of the second one. We refer readers unfamiliar with the Mobius function to [Jal] and [Bo2, Appendix]. For each m-tuple n let = dim^^ By Proposition 3 the character of the universal enveloping algebra of ^ ( X ) is n ( l - x " ) ~ ‘' " e K [ [ x ] ] , n

where x = {xj,. . . , x^}. (Do not confuse the commuting variables Xj,. . . , x„ with the elements of X ) On the other hand, we know that the free associative algebra A ( X ) is the universal enveloping algebra of S(X ), and its generating function is easily seen to be (1 - (x i + ••• +x„,)) \ Thus ( 20)

n ( l - x " ) " " = l - ( X i +

--+xJ.

2.6

141

The Category 0

By Exercise 2.16, the dimensions d„ are given in terms of the set 5(r) of partitions of r into other m-tuples and certain multinomials C(p) for each partition p. Since the only coefficients on the right-hand side of (20) are limited to terms of degree 0 or 1, the multinomials C(p) are 0 unless p is the partition r = r i ( l , 0 , . . . , 0 ) -I-r2(0, l , . . . , 0) 4- • •• -t-r„(0,0,...,l) in which case it is (/•i + ••• \

1• ***' m•

1 ''i +



Formula (ii) follows immediately. Example 4 ( ^ ( ^ ) , card(Ji) = 2) n 1

2 3 4 5

dim /x(l)2^ = 2 (1/2){ m(1)2" (1/3){ m(1)2^ (l/4){/x(l)2^ (l/5){/x(l)2^

dim

+ m(2)2'} = 1/2(4 - 2) = 1 + m(3)2'} = 1/3(8 - 2) = 2 + m(2)22 + jtx(4)2'} = (1/4)(16 - 4) = 3 + A^(5)2'} = (1/5X32 - 2) = 6

= (1 /6){m(1)6!/3!3!+ m(3)2!/1!1!} = 3

Note There is a procedure due to P. Hall [see Bo2] that produces an explicit basis for each degree subspace of a free Lie algebra. 2.6 THE CATEGORY & Throughout this section g will denote a Lie algebra admitting a triangular decomposition (1^, 0+? which we fix once and for all. Our aim is to introduce a category <^(g, [BGGl] whose objects might loosely be described as consisting of those g-modules whose characters lie in Z[f)* iQ+]. In fact the last part of this section is devoted to putting a ring structure on the isomorphism classes of modules in ^ to form the representation ring of which is then related to Z[f)* J, ¡2+] via the character map. Unfortunately, g itself, under the adjoint representation, does not appear in & in general. With this exception ^ and its a opposite category contain all the representations of g that we will need in this book, including in particular highest weight representations. The first half of this section introduces the (local) concept of composition series of modules in the

142

Lie Algebras Admitting Triangular Decompositions

notion of the multiplicity of an irreducible submodule of a module M in category and more on primitive vectors which were briefly used in Sec­ tion 2.4. The category is deflned as follows: (i) Objects of 3^). Those g-modules M having the following prop­ erties (ia) M admits a weight space decomposition M=

©

with respect to the action of f); (ib) the set P(M) of weights of M, that is,

is included inside a finite number of fans of ij* iQ+; (ic) for all e P(M), dim^^iM^) < oo. (ii) Morphisms of S^). All g-module homomorphisms between the modules in Obj(<^). We often write M e «^) to mean that M is an object of The category of g-modules is the category <^(g, We are already familiar with highest weight modules. Provided that its weight spaces are finite dimensional, such a module lies in For instance, if the triangular decomposition is regular, then for all A e 1^* the Verma module M(A) and the irreducible module L(A) are in Remark 1 (i) It is useful to note that if 0 + is countable, then every module in & is of countable dimension. (ii) We recall (from Section 2.5) that a partial ordering > was defined in by declaring that for all A, /u, e 1^*, A > / t < = > ^ t e A i ¡2 +* We also introduce for each A e 1^* the depth function

defined for all /8 e ¡2 _^u{0} by ¿ , ( A - / 3 ) := ht(/3).

2.6

The Category 0

143

Lemma 1 Let F = U i 0+) union o f a finite number o f fans in 1^*. Let S be a nonempty subset o f F, Then (i) if p ^ S, the set {A e 5|A > p) is finite; (ii) 5 admits maximal elements. Proof (i) Let p ^ S and ; e {1, . . . , n}. By definition of <2+-fans, it is immediate that if p ^ Ay i Q+, then there is no element ^ e Ay i with ^ > P, and if /1 e Ay I Q+, then there is only a finite number of elements i e A; I (2 +, with ^ > p . It is clear therefore that the set in question is finite. Part (ii) follows from Part (i). □ Let M e ^ (g , and let M = sition. We recall the formal character of M ch(M) =

be its weight space decompo­

E dim M^ e( p) ^ Z [ V iQ+]^ /Ltei)*

If M = M', then the isomorphism must map weight spaces isomorphically onto weight spaces so ch(M) = ch(M'). Proposition 2 Let M and N e ^ (g , ^ ) , and let P{M) and P{N) be their corresponding sets of weights. (i) I f both A and B belong to

is an exact sequence o f ^-modules, then Moreover, for a// e

0^

->

^ 0

is an exact sequence o f K-spaces and ch(M) = c h ( ^ ) + ch(B). (ii) Every submodule and every homomorphic image o f M belongs to ^ (g , ^ ) . (iii) The direct sum M 0 AT belongs to ^ (g , Moreover P{M ^ N ) = P(M) U P( N) and ch(M ® N) = ch(M) + ch(A^). (iv) The tensor product M ^ N belongs to ^ (g , Moreover P{M 0 N ) c P{M) + P{N) and ch(M ® N ) = ch(M)ch(iV).

144

Lie Algebras Admitting Triangular Decompositions

Proof. Let M = Identify A with a submodule of M to conclude (Proposition 2.1.1) that A admits a weight space decomposition A = where

e

A'",

= M'^ n A. It is clear then that A e B = M/A=

© M V 0 A -'s usi,* Ae6*

3^). Also 0

M>^/A>^,

and hence B=

® B>^,

where B'^ = M'^/A'^ for all fi e i)*. This shows that B of (i) follows easily. (ii) The proof is obvious from Part (i). (iii) For every ju. e 1^*,

,

The rest

(M ® AT)'‘ = M'" ® JV**, and thus M®N=

0

Evidently P( M ® N ) = P(M) u P(N), and the weight spaces are finite dimensional. Thus M ® AT e (^, and Part (iii) follows. (iv) Let {y,}, g j and ek basis of M and N, respectively, consisting of weight vectors, say, e M^ ‘ and e M*'* for all i e I and it e K. The set {d, ® Wfcl/ei, *eK is a basis of the space M ® AT and these are weight vectors: Indeed for h /i • ( y,- ® H'fc) = h ■Vi ® =

iJLi(h)Vi ®

+ Vi (8) h • +

Vi ® A * ( h ) w ^

= {Pi + ^k)(h)Vi ® w ^ . . This shows that M ® N admits a basis consisting of weight vectors and hence a weight space decomposition. Moreover, if y e 1^*, then (M ® AT)'*' has as a basis the set {y, ® consisting of those i and k such that /r, + A;t = y. In other words. (1)

( M <8>N y =

© (M>^(8i N^). fl+\=y

2.6

The Categoiy 0

145

Thus F(M <S) c P(M ) + P(A/^), and this is contained inside the union of finitely many fans. Finally, from (1) we get ch(M (S>N) = ch(M)ch(N). □ Let M be a g-module. An element v ^ M is called a primitive vector if 1 y is a weight vector relative to 1^; 2. there exists a submodule N of M such that u ^ N and

- i; c N.

If this situation arises and A the weight of v then we also say that A above is a primitive weight of M {relative to N). Every highest weight vector of a g-module is a primitive vector. Lemma 3 L e t M ^ & {% ,Sr\ (i) For a weight vector v o f M o f weight /x, the following are equivalent: (ia) V is primitive, Gb) V ^ U(g) • V, (ic) there exists a submodule N o f M such that N c U(g) *v and U(g) • v/N = L{p), (ii) For a primitive weight vector o f weight ¡jl to exist in M, it is necessary and sufficient that L{ jjl) be a subquotient o f M [i.e., that there exist submodules X and Y o f M such that X :d Y and X / Y = Lip)]. Proof (ia) => (ib) Let v g be primitive. Then there exists a submodule M' of M such that v ^ M' but g^* i; c Af'. We have v ^ M ' = Vi{%) - M ' D U ( g ) -g^-i; proving Part (ib). (ib) => (ic) Suppose that v ^ U(g) • g+* == M'. Then M' is a submodule of M and g+* v c M'. This shows that v is primitive. Let M *= U( q) *v/M' , M is a highest weight module generated by the coset v + M'. According to PartjGO of Proposition 2.3.4, M Ims a unique maximal submodule N and M/ N = L{p). The preimage N of N in U(g) *v gives us U(g) • v / N = L{p), proving Part (ic). (ic) => (ia) The submodule N of Part (ic) serves to show that v is primitive. (ii) After Part (i) it remains only to show that if M has a subquotient X / Y = L{p), then M has a primitive vector of weight p. But any preimage ¿;+ in of a generator D+e L { p Y of L{p) under the map X X/Y Lip) is primitive: T, g+* + c y. LI

Líe Algebras Admitting Triangular Decompositions

Proposition 4 Let M and N be objects of ^ ( 9, ^ ) , and let f : M -^ N be an epimorphism. Suppose that v ^ M is a highest weight vector o f weight A and that w ^ N is a primitive vector of weight p. Then (i) there exists a primitive vector x ^ M o f weight p such that f ( x ) = w; 00 if f(v) ^ 0, then f (v) is a highest weight vector o f N o f weight A. Proof 0) Let N ' be a submodule of N with w ^ N ' but w c N', Since / maps onto N^, we can find x ^ with f ( x ) = w. Set M' = f ~ \ N ' l Then X ^ M' and g+- jc c A/'. (ii) The proof is straightforward. □ Remark 2 It is generally not true that the homomorphic image of a primitive vector is a primitive vector. Proposition 5 Let M e ^ ( 9, Then

be a nonzero module, and let P(M) be its set o f weights.

(i) every maximal element o f P(M) (with respect to > ) is a highest weight', in particular highest weight vectors, and hence primitive vec­ tors, for M exist. (ii) The set of primitive vectors o f M generate M as a q_-module (and a fortiori as a q-module). Proof (i) Since M ¥= (0), we have P(M) # 0 , and hence P(M) admits maximal elements by Lemma 1. Let p be such an element, and let v e M^, V ¥= 0. Then 9+* V c ^ which shows that i; is a highest weight vector. (ii) To see the primitive vectors generate M as a 9 .-module, we consider the space

L

v= V

U(g_)i;cM .

primitive

Clearly V is an 1^-module and hence admits a weight space decomposition (being included in M). Suppose M ^ V , and choose p e P(M) maximal such that (tV .lix^ \ V, then x is not primitive, and hence X e U(9) • 9+- ;c by Lemma 3. Now U(9+) • 9^- X c c K by the maximality of p. But then x e U ( 9 _ ) - U ( ^ ) *1 1 (9 ^ - 9 ^;c

c

U ( 9 . ) - U( f t ) - K c F

contrary to the choice of x. This shows that V = M.



2.6

The Category 0

147

Our next two results characterize irreducible and completely reducible objects of Proposition 6 Let M ^

^ ) , (M ^ (0)). Then the following conditions are equivalent

(i) M is irreducible, (ii) M = L(A) for some A e 1^*. Proof Assume that M is irreducible. Let v e be a highest weight vector (Proposition 5). Then M = U(g)i;, so M is a highest weight module and hence a homomorphic image of M(A). Since M is irreducible, the kernel of this map is a maximal submodule of M(A) and it equals MA) (Proposition 2.3.4). Thus M = L(A) as desired. □ Proposition 7 Let M Ei ^ (g , ^ ) , (M =5^ (0)). The following conditions are equivalent, (i) M is completely reducible [in ^ (g , (ii) M is generated by its highest weight vectors, and every highest weight submodule of M is irreducible. Proof, (i) =►(ii) Suppose that M is the direct sum of a family of irreducible modules of <^(g, *^). By our last result M = © L( A ,) ¿el for some family {Aj^gj c Evidently M is generated by its highest weight vectors. Let be a highest weight vector of weight A, and write t; = E i;, where v¡ e L(A,) for all i e I. Then g^.- ü = 0 =» g^.- v¡ = 0 for all i => v¡ L(.X¡y‘ for each i. Now for all /t e we have E a(/ i ) ü, = \ { h ) v = h • V = /e l

/e l

148

Lie Algebras Admitting Triangular Decompositions

which shows that f = E A, = A

It is easy to see then that the submodule U(g)i; generated by v is isomorphic to L(A) and hence is irreducible. (ii) => (i) By assumption M is a sum of irreducible submodules. Then M is the direct sum of irreducible modules by Proposition 1.4.2. □ Corollary 1 Let M ^ be a module with the following property: I f A and p are primitive weights o f M, then \ > p ^ k = p. Then M is completely reducible. Proof Let be a highest weight vector of M, say, of weight A. If U(g)i; is not irreducible, then any primitive weight /a of a proper submodule of U(g)i; (such p exists by Proposition 5) will satisfy k > p, which is not possible. Thus U(g)¿; is irreducible. Let M' := with the sum being taken over all highest weight vectors of M. If M / M ' (0), we can consider a primitive vectors of M, say, x e M^, such that x ^ M' (Proposition 4 applied to the canonical map M M/M' ), Now g+- a : # (0) (for otherwise x e M'), and hence the space U(g+)g+* x contains some highest weight vector, say, of weight A'. Then X > p, contrary to our hypothesis. □ We now introduce composition series. It admits a composition following local version

the concept of local, highest weight, and Verma can be shown that not every module in ^ (g , series (see Exercise 2.13). We have, however, the of composition series.

Proposition 8 Let M e ^ (g , and A e if*. Then there exists a finite sequence M q, , ,.,Mf^ of modules in ^ (g , S^) and a subset I c {1,..., A:} with the following properties, (LCSl) (LCS2)

M = M¡^z> D • • • D Mo = (0). I f i G I, then there exists A¿ e 1^* such that A¿ > A and M,/ M, _i= L( A, )

(LCS3)

I f i ^ I, then (M ,/M ,_i)^ = (0) for all p > k.

2.6

The Category 0

149

In words, all weight spaces o f M for weights equal or above A are involved in irreducible quotients o f the series. Proof Define á(M, A) = dim(M^). (This sum is finite by Lemma 1). We reason by induction on d{M, A). If d{M, A) = 0, we simply set = M, Mq = (0), and 1 = 0 . Assume that d(M, A) > 0 and that the result holds for all modules N e <^(g, 5") for which d(N, A) < d(M, A). Let fi e P(M) be a maximal element satisfying p > \ ( jjl exists by Lemma 1), and let v e y ¥= 0. Then i; is a highest weight vector (part (i) of Proposition 5). The highest weight module V = U(g)i; contains a (unique) maximal proper submodule U (Proposition 2.3.4) and V / U = Lip). We observe that d{M/V,X)
since dim(F^) = 1,

and that d(U, A) < d{M, A),

since dim([/^) = 0.

By induction hypothesis both M / V and U have sequences of submodules with the desired properties. We now consider the inverse image in M of the sequence of M / V under the canonical map M M / V , say, M = M^z> ♦ D Mq = F, and the sequence of U, say, U = U^z:> • • • ^ Uq = (0). Since Mo/Up = Lifi) (see above), it then follows that the sequence M = M _D

••• z^ M o ^ U ^ z>

••• D i / o = ( 0 )

is as desired. A sequence of the type appearing in Proposition 8 is called a local composition series of M at A. The factors for some /x > A are called proper. The remaining ones are called extraneous. Remark 3 We make the simple observation that if we insert a submodule N between Mj and Mj_i, in the local composition series M = Mf^^

• •• d Mo ={0}

relative to A, then the resulting series M

= M f,:D

••• M y

D

••• d M o = {0 }

is also a local composition series at A and has the same proper factors, including multiplicities, as the original series. Indeed there are only two

Líe Algebras Admitting Triangular Decompositions

150

cases: 1.

is proper, in which case N = Mj or N = Mj_^, and one of N/Mj_^ and Mj / N is proper and one extraneous [actually (0)]. 2. is extraneous, in which case both Mj / N and N/Mj_-^ are extraneous. Two local composition series for M, say, M = d • • • =) Mq = (0) and M = Ni ^ • • • z>N q = (0) are equivalent if k = I, and there is a permutation i ^ i' of {1, . . . , k) such that for all i, Proposition 9 Let M e (^(g, and fei A, /x e 1^*. Any two local composition seríes {M¿} and {M/} o f M at A and /x, respectively, have common refinements that are equivalent to a series {M") that is local at both A and jjl. Furthermore for ^ > A {resp. ^ > /x) the number proper factors of type L ( 0 in {M¿} and [M¡'} (resp. {M/} and {M"}) are the same. Proof Using the Schreier refinement theorem [Ja2] find a refinement {M-} equivalent to refinements of both {M¿} and {M/} (as modules). According to the last remark, this series will be local at both A and p and the number of proper factors will not change. □ Let M e ^ (g , 5^) and p e 1^*. Let A g f)* be arbitrary with p > X, and let {M¡\ be any local composition series of M at A. We claim that the number of proper factors of type L(/x) in this series is independent of the choice of A and the particular series {Mj that we have chosen. Indeed if {M/} is a local composition series at some A' with p > A', then {MJ and {M/} have a common refinement (M/'} as in Proposition 9. Then the number of proper factors of type L(p) is the same in (MJ and (M"} and also in (M/} and (M/'}, hence in (M j and (M/}. □ Thus we can make the following definition. For M e (^(g, and for /x e we define the multiplicity of L(p) in M, denoted by [M : L(p)] to be the number of proper factors of type L(/x) in any local composition series of M at /x. We will see another interpretation of these numbers in Proposition 12. Let M e ^ (g, filtration

A highest weight series (HWS) for M is an increasing

(0) = Mo c Ml c M2

The Category 0

2.6

151

of submodules of M so that (HWSl).

U M =M;

i=0

(HWS2). If M,_i M¡, then with highest weight /i.,.

is a highest weight module, say,

Let {A/,} be a HWS for M. If 9 e 1^* is any weight, then dim M ’’ < 00, and the sequence {dim is increasing to dim M ’’. Thus (HWS3). For each e f)* there is a A: e Z+ such that for all i > k, M f = M ‘< ‘. If the highest weight series satisfies •••

•••>

we say that it is a finite highest weight series of length equal to n. Proposition 10 [G L, DGK]

Suppose that the root lattice Q is finitely generated (.equivalently the index set J of the triangular decomposition S ' is finite). Let M e Then M has a HWS, (M,}7=o- Furthermore the series can be constructed so that (HWS4).

> fij => i < j, where

Proof Since M e

there exist P { M) c Ai i

is the highest weight of e

such that

• • • U A^ i e +-

If A^ i (2+n Ay i (2 + =5^ 0 then there exists A with A i A¿ i <2+^ Ay i ¡2+- Thus we can assume that the union of the fans is disjoint. Then for any e P ( M \ ¡JL = - p for some unique / e {1,..., A:} and /3 e (2 +’^{0}Let d()L¿) := = ht(p) (Remark 2.6.1(ii)). Clearly from the assumption on QAP' ^ P(M)\d(/jL) = N} is finite for each N ^ N. Let fi^ G P(M) be chosen with d(fji^) minimal. Then is a maximal weight of M relative to > . Thus, if ¿;i e \ {0}, is a highest weight vector, and generates a highest weight module M^. Now repeat the argument with M/M^ to get a submodule M2 of M, M2 ^ Mj for which M2/ M 1 is a highest weight module. In this way we obtain a filtration (0) := M q (zMi d M2 c • • • . Since the value of d(fi¿) is increasing and can only remain at one value for finitely many i, we see that for any weight

152

Lie Algebras Admitting Triangular Decompositions


= • • • . Thus UM, = M. The con­ □

For each M e O bji^iq, y ) ) we have its associated character ch(M) e i Q A s we have pointed out before, M = M' => ch M = ch M'. Let S = S( q, be the set whose elements are the isomorphism classes of g-modules in We denote the equivalence class of M by M. Evidently ch determines a mapping, also denoted ch ch: satisfying ch(M), where M ^ M. We let R = R(q, denote the free abelian group on the set 5. A typical element of R has the form

(finite sum). R can be made into a commutative ring by defining multiplica­ tion by bilinear extension of M-N= This is evidently well defined. The character map extends to a homomor­ phism ch : R ^ i Q+], We denote its kernel by K, and set R = R(ij, ^ )8 } :R /K , We call R the representation ring of g relative to Factoring ch through K, we have the character map ch:R(q,^)

iG+].

For M e O bj(^) we denote its image in R( q, y ) by 0^ A B ^ C 0 is an exact sequence of modules then ch(B —^ —C) = 0 by Proposi­ tion 2 and hence [B] = [A] + [C] in R. In particular for modules M and N in [M © AT] = [M] + [TV]. We also have [A/® TV] = [TV/][TV] by the definition of the multiplication in R.

2.6

The Category t

153

Remark 4 It is useful to note that any element Z oi R can be written in the form [Z+] - [Z_], where Z+ and Z _ e For if Z = then we simply set Z^_==

0

(Af 0 • • * © Af)

(^[Af] summands),

Z_:=

0

(M ®

(-Crjv^j summands).

®M)

Proposition 11 Let {c;^}^ e 6* t>e a family o f elements o f Z. (0 The family ch ¿(A));^eE)* o f Z[if* | <2+1 is summable if and only if there exists a finite union F o f fans in Z[k*iQ^] such that [X e 0) c F . (ii) For every element f if Z['i)* IQ+] there exists a unique family o f integers {C;^}Aefi* such that the family {c^ o f zli)* J, 0 +] is summable, and f = ch(L(A)). Proof (i) For each ju. e h* let = c^ch

L { f i)

=

c J

Y .

-

a)].

If the family (/^)^ ^ f,* is summable, then by definition (see (SI) of Section 2.5) {supp/^lju e h*} c F , where F is a finite union of fans. Now since supp 0, and hence {p, e f)*|c^ Conversely, assume that {/x e holds, since

= 1, we see that ¡x e

0} c F . # 0} c F. Then clearly condition (SI)

{supp 4 I m e

c

F.

Fix A e ]^*. Then for /x e 1^* we have ffjL ^ Z[]^* i 2

+ ] ( a)

^

^ 0 and

=> jjL ^ F

and

for some ¡jl — a > \ jJL > \ fJL > \

154

Líe Algebras Admitting Triangular Decompositions

and this set is finite by Lemma 1. This establishes (S2) of Section 2.5 and hence the summability of the family in question by Proposition 2.5.1. (ii) Suppose that / = La^eifi) e Z[l^* i Q+], We wish to write / in the form Ec^ ch(L(^t)) as in Part (i). We may assume, as in Proposition 10, that all the weights in supp(/) lie inside a finite disjoint union of fans. Then there is no loss in assuming that all the weights appearing in supp(/) lie in one fan be the depth of fi (see A i G + . For each ¡x ^ A i Q + let difx) == Remark 1). We compute the coefficients by induction on the depth. Suppose that / has been written in the form /=

L c^ch(L(M)) + / . dilxXd

for some d > 0, where contain nontrivial terms only for weights v with d{v) > d (we begin at / = / q). Let denote the set of weights of depth d in A i (2+, and for each i e I let denote the coefficient of c()ll^) in /¿. By part (i) the set {c^. ch L(/x^)}^^/ is summable. Setting /¿+1 ■■=fa - E,^,c^.ch(L(/u,,)), we have / = E d if j¿ )< d- ¥ 1 c c h L ( ^ ) +/ d+i. where contains nontrivial terms only for weights v with d{v) > d + 1. The entire family {c^ ch L(^t)} is easily seen to be summable, proving the existence of part (ii). Finally, if the uniqueness were to fail, then E^ g f ^a L(A) = 0 for some union F of finitely many fans. Let 5 — {A e Flc;^ = 0}. If S 0, then it has a maximal element Aq and

CA„chL(Ao)-----E C;^chL(A) A # Aq

gives a contradiction. Indeed the coefficient of e(Ao) is on the right.

on the left and 0 □

Remark 5 In Proposition 11 we have used the characters of the irreducible modules in as a “Z-basis” for Z[l^* i 0+]. However, the only facts that we have used about ch(L(A)) are 1. ch L(A) involves e(/¿) only if /a e A J, 2. the coefficient of e(A) is 1. Thus Proposition 11 holds, for instance, if we replace each ch(L(A)) by the character ch(M(A)) of the corresponding Verma module.

2.6

155

The Category &

Proposition 12 Let M e

5^). Then chM=

12 [ M : L(iJi)]ch L(ix), /xei)*

and this is the unique way o f writing ch M as an integral combination o f the characters o f irreducible modules from Proof The uniqueness follows from part (ii) of Proposition 11. We prove that for each A e 1^* chM =

L [ M :L ( /i ) ] ch L ( /x ) fji>\

mod Z [ ^ i !2 +](a)

(see Proposition 2.5.1). For if {M¡)¡^o „ is a local composition series of M at A, then for each /a > A, [M : L(/i)] is the number of proper factors of type L(/i) in {M,}. We have c h M = ¿ ch ¿= 0

^

[ M :L ( M ) ] c h L ( M ) m o d K [ n e + ] ( A ) -



/11 ^ A

Let F e A Verma composition series (VCS) (of length r) for M is a descending sequence of modules of V F = M o = ) M i3 •••

DM, = (0)

so that M¿_i/M^ is a Verma module, / = 1,2,..., r. Such an object need not exist for a given module V. However, if it does, then c h F = E chM¿_i/M¿, and hence by Remark 5 the Verma factors M^_i/M^ are, up to permutation, uniquely determined by V and are independent of the particular VCS chosen. The number of times that M(/x) occurs in a VCS of M is denoted by [M:M(p)l Proposition 13 Let p

be fixed. There exists a unique group homomorphism

156

Lie Algebras Admitting Triangular Decompositions

satisfying

Proof Let

: R(g,

-» Z be the unique group homomorphism satisfying

We show that this maps factors through the defining kernel K
x = E c ,M „ 1= 1

where N

E c,ch(M ,.) = 0. ¿=1 Thus in Z[]^* i 2+] we have by Proposition 12, N

0=

E [ M, : L ( n ) ] c h L ( f i )

¿=1

= E ÍE^,[M,:L(M)]]chL(M), ^ e f ) * \/ = l

and hence for all

/

e 1^* we obtain N

£ c, [ M , : L ( m)] = 0 ¿=1 by Proposition 11. Thus N

¿= 1 =

L

c

, [ M , : L (

m

)]

= 0 .

/=1 We have therefore an induced group homomorphism

as desired.

2.6

The Category ^

157

Corollary 1 (i)

If 0 ^ I,

^ M ^ M /N -» 0 is an exact sequence o f modules from then for each ¡jl e 1^*, [ M : L ( m )] = [AT:L( m )] +

(ii) For M j, . . . ,

[ M / N : L { t i ) \ .

e i^(g, [Ml Ф

0 M , : L ( m)] = Е [ М : Ц м ) ] . k =\

Proposition 14 ch: i?(g,

-» Z[if* 1 0+] ^ an isomorphism o f rings.

Proof ch is injective by the definition of i?. Let / e I[i>* j, g+l. By Proposi­ tion 11 we can write / = Ec^ ch(L(A)). Let M+:= 0 c^L(A), «A>0 M _ ~

Both of these lie in

© c*<0

— c ^ L ( X ) .

and ch([M j-[M _ ])= /.



Let M e ^ (g , ^ ) . Then M has a weight space decomposition M=

© M^.

Recall that we have defined the restricted dual space M^es of M by Mres == { / ^ M*K/, M^> = (0)

for all but a finite number of

Proposition 15 Let

:= M^es

a K-space. The map g X M^ -> M^

e 1^*}.

Lie Algebras Admitting Triangular Decompositions

158

denoted by {x,f) ^ x - f , and given by {x ' f , m ) = gives

for all jc e g, / g

m ^ M,

a Q-module structure.

Proof. The map in question is clearly bilinear. Moreover, if jc, y g g and m ^ M ,^ e have i [ x , y ] ■f , m } = < /, [o-(y),
■a { x ) ■m) - ( f , a { x ) ■

= { x - y • f , m ) - ( y ■X ■f , m ) , so [^>y] - f = x ■y ■f - y ■X ■f . That AC• / e

is clear.

The g-module



is called the restricted dual module of M.

Proposition 16 Let M G ^ (g , (i)

and let

be its restricted dual. Then

admits a weight space decomposition relative to

=e with

(ii) e ^ (g , ^ y , (iii) ch = ch M; (iv) (v) M is an exact contravariant functor o f i^(g, (vi) L(A)^ = L(A) for all A e 1^*.

into itself;

Proof (i) Given / € we can define the map =/ ° ^ is the natural projection M that annihilates Af** for all ju.

where A. By the

2.6

159

The Category <

definition of M^, f ■= where 5 is some finite set (depending on /) . Let us see that each is a weight vector of weight A. Indeed, given m ^ M and writing m =

£

m ^,

e M>^,

we have, for all /i g f), {h ■f^ ,m ) = {f¡^,a{h) ■m) = {f ^ , h • m> =

< /

a>

= k{h){f)^,m) = k{h){f)^,m).

This shows that f¡^ g Now part (i) follows. Evidently - (M^)* as K-spaces, and hence dim,^ M'^ = dimi^ M^, since all the spaces in question are finite dimensional. This establishes parts (ii) and (iii). (iv) Write = M for convenience. If m g M, let m g M be de­ fined by ñi{f) = { f , m)

ioxdWf^Mg.

The resulting linear map ~ :M ^M is clearly injective. Moreover c

for all A G f)*

so that ~ is surjective because of the finite dimensionality of the weight spaces and part (iii). Finally, ~ is a g-module map. Indeed, if a: g g, w G M, and / G Mg, we have X ■m ( f ) = { f , x ■m) =
, F : AT*

Given a g-module homomorphism M*

160

Lie Algebras Admitting Triangular Decompositions

by

for all / e N* and m ^ M (thus is the transpose of F). It is clear that if / vanishes on N^, then F^f vanishes on M^. We therefore get an induced map F 'N

M

We verify that this is a g-module homomorphism F :N

M .

In fact for all x ^ q, {F„{x ■f ) , m) = ( x ■f , F{ m) ) = ( f , cr {x) ■F ( m ) ) = ( f , F { a { x ) ■m)> = ( F^ f , a ( x ) ■m) = {x • F„f , m). If G : AT ^ P is another morphism in

then

( G oF) ^ = F„ oG^, showing that

is a contravariant functor of ^ (g , into itself. The exactness is left as an exercise. (vi) Let ¿;+ be a highest weight vector of L(A), and let v% be the linear functional = 1, = 0 if ^ X. Then by part (i), u% e (L(A)^)^, and for all x e g" , jc • y* e (L(A)^)'^'^“ = (0). This shows that i;* generates a highest weight module with highest weight A. Since ch L(A)^ = ch L(A), we conclude from Proposition 12 that L(A)^ —L(A). □ Caution

is not the same thing as 2.7

defined in Proposition 2.3.5.

THE RADICAL

In this section we introduce four different ideals of a Lie algebra g with a triangular decomposition (i), g+, Q+, a). Each of them has a right to be

2.7

The Radical

161

called a radical of g. However, in general they are not all equal. They are 1. t y ( g ) == the set of all elements of g that annihilate every irreducible module in 2. m ^(g) == the largest ideal of g intersecting trivially; 3. n(g) == the sum of all the residually nilpotent ideals of g; 4. rad(g) := n the intersection being over all triangular decom­ positions of g. We discuss these in turn. We find that always r ^ = m ^ , and in the case of primary interest to us, that is when E , e j 9~“' + h + E , e j 9“' generates g as a Lie algebra, r^ ( g ) = m ^ (g ) = rad(g) and Z(g) ffi rad(g) = n(gX We make use of these results in Chapter 4. Throughout this section g will denote a Lie algebra over IK admitting a triangular decomposition, and we will let ■^= (i),Q+,Q+,o’) denote one such decomposition. To describe this situation, we will henceforth say that (g, is a triangular pair. Proposition 1 Let (g, y ) be as above, and write g = g _ ® ® g+. Let Z(g) and D(g) denote the centre and derived algebra o f g respectively. Then (0 Every ideal o f q is graded by Q; (ii) Z(g) = {A e l^|a(/i) = 0 for all a e A}; (iii) D(g) = g_®([g, g] n fi) ® g+. Proof (i) Let a c g be an ideal. Then [1^, a] c a and therefore a is a submodule of g under the adjoint action of 1^. Now part (i) follows from Proposition 2.1.1. (ii) By part (i) and element belongs to the centre of g if and only if all of its homogeneous components do. If x e g“, a e then a(,h) # 0 for some h Thus [h, x] = a(h)x # 0, and hence x i Z(g). Similarly g_n Z(g) = (0). It follows that Z(g) c fi, and part (ii) is then clear. (iii) As in part (ii) we see that g_® g+c D(g) and hence that part (iii) holds.

□ Let (m,), s i be any family of ideals of g such that m, n = (0). Then the ideal Em, of g, being graded, satisfies (Em,) n = (0). We conclude that there exists a unique largest ideal of g intersecting t) trivially. Thus m ^(g) exists.

Lie Algebras Admitting Triangular Decompositions

162

Proposition 2 Let (g,

be a triangular pair as above. Then r

= m ^(g).

Proof. Let L be an irreducible module in ^ (g , ^ ) . Then L s L(A) for some A e 1^* (Proposition 2.6.2). The annihilator of L is clearly an ideal of g, and hence also is an ideal of g. Suppose e r ^ n ]&. Then for any A for which A(/i) # 0, we have h • L(A) # (0) contradicting the fact that h e r ^ . Thus r ^ c xn^. Conversely, let L(A) be an irreducible module of (s, "^X and let i )+ g be a generator forit. Let V ~ v^. Since m ^ n = (0) and since is graded, we have V=

ti+c g_- v^+ g+- v^= g_- v+
Now g+- V = 9+-

Ü+C ( m ^ + m ^g + ) • v^= V.

Thus U(g)-FcU(g_)U(^)-Fc

E L(A)^
which shows that U(g) • F is a proper submodule of L(A) and hence (0). This proves that m^* u^= (0). Let N '= {u Ei L(A)|m^* v = (0)}. Then N is a submodule of L(A) since (9 •

^

g] • N + 9 •

N = (0),

Since v +E N, it follows that N = L(A) and hence that m ^ annihilates L(A). Since Awas arbitrary, this shows that m ^ c as desired. □ The ideal r^ ( g ) (or simply if g is understood from the context) described in the last proposition is called the (Wedderburn-Jacobson) radical of g with respect to We will see in Proposition 5 that for a large class of Lie algebras admitting triangular decomposition, the radical does not depend upon the choice of triangular decomposition Define r 5r : = r ^ n g + Then

and

r^:= r^ng_.

2.7

The Radical

Since cr(r^r) is an ideal of g intersecting

163

trivially it is easy to conclude that

= r^ and that

Example 1 (Extended Heisenberg algebra a) The notation is that of Example 2.6, where we extended a Heisenberg algebra by a derivation in order to obtain a triangular decomposition. Recall that S = IK[^y]ye j can be made into a highest weight module of type (1, A) for any A e ]^* where if = Kc ^ Kd. Moreover these modules are irreducible whenever A(c) 0. (Example 2.3.2). Now Kxj^) ■■ ^ 0 so that r^ (fi)_ = (0). It follows that r^(a)^.= cr(r^(a)_) = (Ó) and hence that a is radical free with respect to the triangular decomposition in question. Example 2 Let g = Ka © Kh © Kb be a three-dimensional Lie algebra with bracket defined by [A, a] = —2a, [h, b] = 2b, and [a, b] = 0. It is easy to see that g admits a triangular decomposition with root lattice Q = Za where a e (K/z)* is defined by a(h) = 2. The two-dimensional space r = Ka © Kb is an ideal of g intersecting Kh trivially, and hence r is the radical of g relative to the triangular decomposition in question. Proposition 3 Let g and ^ be as above, and suppose that r ^ ( g ) = 0. Then for g_ we have

g+ and

[ z+ ,s _ ] = (0) <»z+= 0, [z_, g+] = (0) « z_= 0. Proof Suppose that [z+, g_] = (0), g+. Without loss of generality we may assume that z+ is homogeneous. By assumption U(g_) z+= Kz+, where the action is given by restriction of the adjoint representation. Then U(g) • z^ = U(g J U ( ^ ) U ( g _ ) • z , c g^, which gives an ideal of g (i.e., the one generated by z+) intersecting trivially. Thus z+= 0. The second assertion follows by applying a to the first. □ Our next result deals with the problem of how Lie algebras with triangular decomposition behave under extension of the base field. (For Lie algebras obtained by extension of the base field see Remark 1.1.1).

164

Lie Algebras Admitting Triangular Decompositions

Proposition 4 Let q be a Lie algebra over IK admitting a triangular decomposition (^5 9+ rel="nofollow"> ¡2+? ^)* Let IK' be a field containing IK. Let g' = IK' the Lie algebra over IK' obtained from g by extension o f the base field from IK to IK', and let = (IK' IK' ®(k9+, Q+> I ® cr) be the corresponding triangular decomposition of g' {see Remark 3, Section 2.1). Then

Proof. For convenience let us set i)' = IK' and g'^. = IK' <S>|,^g+. It is immediate that IK' c To establish the reverse inclusion, it suffices to show that r^ ,(g ')‘^c IK' (for we can then apply 1 ® a). Let be a basis of IK' over IK. Let a e g+j and consider a nonzero element z e r^ /(g ')“. Write z = T, k^<8>x^, A eA

where x “ e g“. Suppose that e g^',. . . , y, e g^' is a sequence of ele­ ments where /Sj • • • -1-/3, = —a. Then ad(l ® y , ) . . . ad(l ® y,Xz) e r^Xg') n £)' = (0), and 0=

® adyi...ady,(ji:J'). AeA

We conclude that ad ... ad = 0. It follows that for each A e A , the ideal generated by in g intersects trivially and hence that each x “ er ^ ( g ) '^ . Thus z e IK'<8>j^r^(g)‘^ as desired. □ Remark 1 Let g, y , r ^ , and

be as above. Define 9 == 9 / r ^ ,

and let : g ^ g be the canonical map. Then g = g_e fi e g+, where g+— 9+ A 5r and §_== g _ A 5^ (we are identifying with a subalge­ bra of both g and g). It is clear that a induces an antiinvolution of g since o-(r^) = r ^ , as we just saw. As long as 5+=?^= (0), we obtain an induced

2.7

165

The Radical

triangular decom position

of g with root spaces given by 9“ =

g“

for all a e g .

Finally, observe that if a is an ideal of g such that d n = (0), then the preimage a of d in g also intersects ij trivially (because the restriction of “ to if is injective). Thus a c r We conclude that = (0).

( 1)

We next consider the problem of the independence of r^r from We begin with some general facts about Lie algebras. If A is an ideal of an arbitrary Lie algebra I, we inductively define a decreasing series A =A^ A^ ^ • • • of ideals of I as follows: A^ :=A, A'^^^ := [ A, A^ ] . The ideal A above is said to be residually nilpotent if n ^ " = (o). n>l

We define n(I) to be the sum of all residually nilpotent ideals of I. Observe that n(I) itself need not be residually nilpotent. Returning now to our Lie algebra g we define the (Wedderburn-Jacobson) radical rad(g) of g by rad(g) = the intersection being taken over all triangular decompositions of g. We say that g is radical free if rad(g) = (0). Notice that g/rad(g) is always radical free (see Exercise 2.18). Proposition 5 Let (g, ^ ) be a triangular pair as above. Assume that (CTl) The subspace algebra.

5

^ 9 generates % as a Lie

166

Lie Algebras Admitting Triangular Decompositions

Then (0 r ^ , r Jr, and are residually nilpotent ideals o f n (ii) r ^ c for any other triangular decomposition o f g, in particular = ^ 5^(9) = rad(g); (iii) n(g) n Í) = Z(g); (iv) ^ induces a natural triangular decomposition on g/Z(g), and we have rad(g/Z(g)) = it (g/Z(g)), Z(g) e rad(g) = it(g); (v) n(g) is residually nilpotent] (vi) I f S ci)* spans f)*, then rad(g) = fl a s 5 ann L(A). Proof (i) Let U(g) • r j- be the ideal of g generated by r j- (here U(g) acts by the adjoint action). We must show that U (9) • r ; ^ c r ^ . Suppose not. Then, since U(g) • r j- c r ^ , there exists some element z e r ^ n g“, a e Q+, such that [ x i [ x2,...)[-'"A;>-2] ' ’ ' ] ] ^

{0}

for some elements Xj,. . . , g g. From condition (CTl) we can assume that e g * “ >. for some g J. If we choose k above minimal, then X j g g “ “ A, and

Xi

w ■■= [x2,

[ x 3 , . . . , [ x * , z ] ]

G

But w is an element of n = (0), contradicting the fact that [xj, w] # 0. It follows that r jr is an ideal of g. Moreover ( 2)

(rj.)

c

©

g“,

ht(a)>n

which shows that r J- is residually nilpotent. The analogous results for follow by applying a. To show that is residually nilpotent, first observe that [t;^, rjr] c = (0) and that hence r ^ c ( r » " + (rj-)".

2.7

The Radical

167

Combining this with (2), it follows that r^ c

e aeA

g“.

\ht{a)\ >n

Thus 0 = (0), and is residually nilpotent. (ii) Let 3^' = be any triangular decomposition of g. We claim that c that is, Pi 1^' = (0). For suppose not. Let h 0 belong to this intersection. If a'(h) = 0 for all roots a' of (g, then h e Z(g), and hence ^ripart (i) of Proposition 1). Thus h e r ^ n = (0), a contradiction. Therefore let a' be a root of (g, such that a'(h) 0, and let X ^ X ¥= 0. Since (ad h ^ x = a ' ( h y x , we conclude that x e for all contradicting the fact that is residusually nilpotent. Thus x ^ c z x ^ r , and the rest of (ii) follows from Proposi­ tion 2 and the definition of rad(g). (iii) Let a be a residually nilpotent ideal of g. If e a n and a(h) ¥= 0 for some a e A, then (ad/l)"g- = g ^ and hence g" c a ” for all n, which contradicts the fact that a is residually nilpotent. It follows that a n c Z(g). Let a^,. . . , be residually nilpotent ideals of g. (Uj + • • • + a^) n ]^ - (Ui + • • • +a^)^ = a? + • • • +a^ (3)

£ a , ni)cZ(g) /=1

by the above. Now let h e n(g) Pi 1^. Then by definition h belongs to a finite sum of residually nilpotent ideals of g, so e Z(g) by (3). This shows that n(g) Pi c Z(g). The reverse inclusion is obvious. (iv) We can assume that for each i e J, g“' ¥= ( 0 ) . Then from part (ii) of Proposition 1 , o : ,lz (g ) = 0 for each i e J, so we have a natural interpretation of j2 as a set of linear functions on íi/ Z ( q). Furthermore {«/l.ej remains linearly independent in this setting. Let tt : g 9/Z (g) denote the natural mapping. Then 'Tr(g) = '7r(g_) 0 7t(]^) 0 7r(g+) [note that 7r(g+) ¥= ( 0 ) ] ad­ mits a weight space decomposition relative to 7r(fi), and a factors through tt. Thus we have an induced triangular decomposition Evidently Z(7r(g)) = (0 ), and (CTl) holds for 7r(g).

168

Lie Algebras Admitting Triangular Decompositions

By Part (i), tyÍTTÍg)) c nCirCg)). To establish the reverse inclusion notice that Tr(ii) n n(Tr(g)) = (0) by Part (iii). Thus rad(g/Z(g)) = n(g/Z(g)). Let a be a residually nilpotent ideal of g. For notational convenience let denote the map v . W contend that 5 is a residually nilpotent ideal of g. (Note that this is not “obviously” the case.) Set 21 = Write 21 = ®2l“ relative to the induced triangular decomposition ^ of g/Z (g) (see Proposition 5). Suppose that ic g 21“ \ {0} for some a 9^ 0. For each n = 1,2,... there exists x„ G (a")“ such that x„ = x. Since ~ restricted to g“ is injective, x„= x„=- X ^ g“ for all m, n. Then x g = (0). Since any ideal of g lying in 5 must be (0), 21“ = (0) and 21 = 21 n ^ c Z(g/Z(g)) = (0). This finishes the proof of our claim. Thus, if a is any residually nilpotent ideal of g, then 3 c n(g/Z(g)) = rad(g/Z(g)). Combining this with the fact that the preimage of rad(g/Z(g)) in g is (clearly) rad(g) ® Z(g), it follows that a c rad(g) ® Z(g). Thus n(g) c rad(g) ® Z(g). The reverse inclusion fol­ lows from (ii) and (iii). This fibnishes the proof of Part (iv). Finally, n(g) is a residually nilpotent ideal. Indeed n(g)" = ( r ( g ) ® Z ( g ) ) " = r(g)", and r(g) is residually nilpotent. (vi) ann(L(A) := [x G q\x • L(A)) = (0)}, so by definition rad g c n as5 L(A) =' I. As for the reverse inclusion, note that / is an ideal of g; hence if I
THE SHAPOVALOV FORM

The problem of describing the submodules of a Verma module is in general very difficult. For instance, it is not at all obvious whether M(A) is irreducible and how irreducibility might depend on A. In this regard the construction of the Shapovalov form is extremely useful. This is a so-called contragredient bilinear form on U(g) with values in 5(1^) which is then transferred to Verma modules M(A). In principle it provides information about the weight spaces MA)'^"“ of the maximal submodule N( \ ) of M(A), although in practice a lot more work is required before any specific information is forthcoming (see Sections 6.6 and 6.7). We assume that we have a Lie algebra g admitting a triangular decompo­ sition g_ 0 0 g+, root lattice Q, and anti-involution cr. This is the first time the anti-involution is going to play a significant role.

2.8

The Shapovalov Form

Using the Poincare-Birkhoif-Witt theorem, we may write

(1)

U (g)

= U(^) e {g_U(9) + U(9)9+}.

Note that which interchanges 9_H(g) and U(g)9+ and pointwise fixes UO^). Both components on the right-hand side of (1) are fi-modules under the adjoint representation. We let q : U % ) ^ U(^) be the projection defined by (1) (so that q annihilates the summand in braces). It is convenient to use Proposi­ tion 1.8.2 to identify U(fi) with the symmetric algebra S(^) so that q: U(g) S(l^). We define the Shapovalov form f : U ( g ) x U (9 ) by F { x , y ) = q{
(i) (ii) (iii) (iv)

F is symmetric. For all u , x , y ^ 11(9), F(ux, y) = Fix, a(u)y). For a , P ^ Q and a ¥=p, U(g)“ ± U(9)^ relative to F. H I, 1) = 1.

Proof, ii) Let X, y e U(g). Writing 9+, and applying
X

M

V

of a g-module M into some space V is called contr^redient (relative to tr) if

170

Lie Algebras Admitting Triangular Decompositions

for all x , y Ei M and for all w e g B{ux, y) = B{x,(T{u)y). The Shapovalov form F is contragredient relative to the anti-involution of the triangular decomposition. Remark 1 More common in physical applications are the hermitian contra­ gredient forms. For these we need a complex Lie algebra g with a semilinear anti-involution cr. Then, if M is a g-module, a hermitian contragredient form on M is a mapping

which is linear in the second variable and antilinear in the first—that is, {ax + y\z) = a{x\z) + and {z\ax + y> = a{z\x) + —such that {u jc|y> = <jc|o-(m), y> for all x, y e M and for all w e g. If the hermitian contragredient from < • | • > is positive definite, then we call it a unitary contragredient form and say that the representation of g on M is unitary (relative to < • I * » . We will usually construct hermitian contragredient forms by beginning with a real form f of g with an anti-involution a and a f-module M with a contragredient form ( | •) on M. Then the complexification of g acts on the complexification of M. Furthermore a extends uniquely to a semilin­ ear anti-involution cr on gc» (*!*) extends uniquely to a hermitian contragredient form < • | • > on M^. We have {x

iy\u + iv) = {x\u)

i{x\v) — i(y\u) +

for x, y, m, y e M.

One checks immediately that {g • x\y) = for all g e f and for all jc, y e M^. Then for g, e I and x , y ^ M^, we have ( ( g + ih) *jr|y> = - i(h -xly) = {x\(Tg *y> - i{x\ah *y> = {x\{(Tg - iah) *y) = { x \a { g + ih) *y), which shows the contragredient. Also < • | • ) is unitary if and only if (*| •) is positive definite. Let us return to the discussion of the Shapovalov form. Any A e 1^* extends uniquely to a homomorphism /- > /( A ) of S(ij) into K. Since in particular the Shapovalov form takes values in we may define, for each Ae a [K-valued symmetric bilinear form f (A) on U(g) by F (A )(x ,y ) = ( F (x ,y ))(A ). Now if y e U(g)g+, then for all x e U(g), F(x, y) = q((r(x)y) = 0 (since

2.8

171

The Shapovalov Form

cr(jc)y e 11(9)9+) and in particular F(A)(x, y) = 0 for all x e U(9)- Also if y G Xli^Xh — A(]^)X then it is a straightforward exercise to show that F(x, y) = f(h —A(/i)) for some / e 5(1^) and hence again F(A)(x, y) = 0. It follows that the left ideal 1(A) [see (2.3(5))] of U(9) is in the radical of F(A). If we recall that M(A) == U(g)/I(A) and use 1 e U(9) to determine the highest weight vector ¿;+ of M(A), then we obtain an induced blinear form F^: M(A) XM(A)

K

satisfying F;,(x • i; + ,y • u^) = F (A )(x ,y )

for all x ,y e U (g).

Remark 2 The symmetry between + and - in (1) is deceptive. The definition of the Shapovalov form given here is appropriate for highest but not lowest weight modules. Proposition 2 (0 (ii) (iii) (iv)

F^ is symmetric and contragredient. Relative to F^, unless a = /3. The maximal submodule is the radical o f F^. Writing M(A) = lKi; ++ have for all x, y e U(9) that F^(x • v^, y • v^) is the component of o-(x) *y • i^+ in

Proof Parts (i) and (ii) are straightforward. To move part (iii), let R be the radical of F;^. F is a submodule by the contragredience of F and is proper since F^(i^+, 1;+) = 1. Thus R c MA). Conversely, let w e MA). Then for all jc e U(9), Fj ,(x -v^ ,w ) =F^(v +,o-(x) -w ) = 0 by part (ii), since cr(x)w e N(Á) c This shows that MA) c R. To move part (iv), write a-(x)y = F(x, y) + r as in the proof of Proposi­ tion 1, and apply it to i > □ We have established that M(A) is irreducible if and only if is nonde­ generate. However, we can be more precise than this. Let y ^ Q+ U{0}, and define FL as the restriction of F to U(q_)"'’': F |^ :U ( g _ ) " ^ x U ( g _ ) '

S (^).

172

Lie Algebras Admitting Triangular Decompositions

Proposition 3

F|y(A) is singular if and only if N ( \Y Proof, We have

# (0). by

u

U ' V.

and F|y(A)(Mi,«2) = F ( « i ,M2)(A)

- v + , U 2 - v ^) .

For «2 e U (g_)' «2 is in the radical of

( 2)

F|,y(A)

<=> U2 *v ^ ±

relative to Fj^,

<=> «2 *^ + -*- ^ (A )

relative to

<=> «2 *^ + ^



Now suppose that g admits a regular triangular decomposition. Then for any y G ¡2+ U{0} we may find a basis, say, « i,. . . , u„, of U(g_)~'^ (See the proof of part Proposition 2.2.1 (iii)). Consider the n X n matrix (3)

Sh^(A) =

From (2) we have the following: Corollary

I f g admits a regular triangular decomposition and Sh^ is defined by (3), then (i)

the dimension of N(XY~^ equals the dimension o f the null space of Sh/A ), (ii) M(A) is irreducible if and only if det(Sh^(A)) ^ 0 for all y ^ U{0}. Amazingly det(Sh^) can be explicitly computed for some of the algebras that are most interesting to us, for instance, affine algebras and Virasoro algebras (see Section 6.6 for the invariant Kac-Moody case). The result is that det(Sh^) factors into linear factors in 5(1^). The knowledge of these factors obviously provides direct information about MA).

2.8

173

The Shapovalov Form

Example 1 (Heisenberg algebras) We continue directly from Example 2.3.1. In the notation established there, for |m| = |nl > 1 we have (4)

F ^{a 'lv^,a 'iv^) = F j^v^,a'la'Lv^)

=

„m!A(c)'"’'

[see equation 2.3(8)].

If A(c) ^ 0, we see that the basis of M(A) is an orthogo­ nal basis. If A(c) = 0, then every basis element |m| > 1 is in the radical of Thus we see once again that M(A) is irreducible if and only if A(c) ^ 0 and MA) = if A(c) = 0. If is finite dimensional, then so is M(A)^“^“ for each r > 0 and det(Sh,_,„(A)) = n

m!A(c)^

|m| = r

If IK = R and A(c) > 0, then (4) shows that the form is positive definite. If we complexify a and M(A), then according to Remark 1 above, the resulting representation is unitary. Example 2 (The Virasoro algebra) We use the notation of Example 2.3.2. The diagonal algebra is spanned by L q and c, and M = M{h, c) denotes the Verma module with highest weight A: A(Lq) = /z, A(c) = c. Let denote a highest weight vector of M. The subspace M" has as a basis the set of elements • K+, where < • • • < rij^ and «j + • • • = n. We compute out the value of F^ on this basis for the values n = 0,1,2. This requires some simple calculations: L iL _i • V

(

2L q + L _ iL i) •

= —Ihv^ _\ F _j *

“ 3 L jL _j

F _1^ 2.^ —\ *^ +

= 6hu^ F^F^F_2 •

6hv^

L iL iL _ iL _ i • v += (8/z^ —4h)u + L2L_2 ■u+= { - 4 h + (i)c)ü + .

174

Lie Algebras Admitting Triangular Decompositions

The resulting matrices for « = 0,1,2 with respect to the bases {v^}, {L_ • i; +}, and {L _2 *u+, • z;+} are

(1),

i-2h),

—Ah + (^)c

6h

6h

8h^ - Ah

In the case that K = R, we may, as before, produce a hermitian form on the complexification of M(A). The problem of deciding for which pairs h,c the resulting representation M(A)c is unitary is much more involved and inter­ esting than first appears. (See [GO] for more on this.). Example 3 ( ê l2(IK)) For A e and a highest weight vector of the Verma module M(A), a basis for M(A)^“"“ is / " • The computation

^ a( / " •

■i'+) = «! n

k= l

((A + p)(h) - k ) ,

is left as an exercise (Exercise 2.19). We have written this using the function p e p(h) = 1, because it appears this way in the generalization (Section 6.6). We observe that the formula shows us in another way that is singular (hence M(A) is reducible) if and only if \(h) g I^. Proposition 4 [Ka] Let q be a Lie algebra over C with triangular decomposition ^ = (^j 9+j Q+j cr). Suppose that the basis Yi o f Q is finite, and let a 0 for all a e n . Then any unitary q-module M in category 0 is completely reducible as an a-module. Proof Let M be a unitary module. Define F: R>o by ♦= ^o)- For each c e C let (resp. g^) be the sum of the a-eigenspaces of /iq on M (resp. ad /iq s) for which F(a) = c. Since the weights of M lie in a finite number of fans and F takes a discrete set of positive real values on ¡2+, it is clear that for all c e C, dim < oo. Note that g^ = ^ and g^ • c for all c, d e C.

2.9

Jantzen Filtrations

175

Decompose a into ad/iQ-^ig^nspaces: a = Define (resp. a_, resp. Oq) as Ea^^ summed over all c such that /(c ) > 0 (resp. /(c ) < 0, resp. /(c) = 0). Let a := a + C/iq. Then a = a_ + (ao + C/iq) + a+

and

dg := Qq + C/iq c ]^.

Let < • I • > be the contragredient form relative to which M is unitary. We begin by showing that M is completely reducible as an á-module. Indeed, if N is an d-submodule, then N = where C\ N. Since < • | • > is positive definite on M"" and dim < oo, has an orthogonal supplement in M^: = N"" ± P"". Thus N M = N ® ^ , and N ^ is an d-submodule because < ♦| • > is contragredient. This shows the complete reducibility. Now suppose that AT c M is an irreducible fi-module. We prove that it is an irreducible a-module. For if not, then N ¥= (0), and we let x = Ex^, be a vector chosen with the following properties: 1. x e N \ { 0 ) , U(a) - jc #iV, 2. cdLiá{c\x^ # 0} is minimal among all vectors x satisfying property 1. Note that the weights of M lie in finitely many fans and hence the values of /«A ,/zo» form a discrete set bounded above as A runs through the weights of M. Thus among the vectors jc = E jc^' satisfying properties 1 and 2 we may choose one for which 3. m3x{ f(c)\x^ ¥= 0} is maximal among all vectors x satisfying properties 1 and 2. Let X satisfy properties 1, 2, and 3, and let x = Ex^, with x^ satisfying the maximizing condition of property 3. Now from the choice of x, - x^ = 0 for all d > 0; that is, a+= 0 and hence a +* = 0 for all c. Thus for each c with x^ ¥= 0, N = U(a) • ^ 0. This can only be true = U(a_) • U(ao) • U(a^) • c E ^ ^,.A^^, for one value of c, and hence x = for some c. Therefore x is a /zro-eigenvector, It follows that U(a) • x = U(a) X = N, contradicting the choice □ of X . 2.9 JAN TZEN FILTRATIONS Jantzen filtrations provide a technical tool for deeper study of Verma modules. The results that we establish here are not used until we discuss the Shapovalov determinant formula in Section 6.5, and the reader can (and probably should) omit this paragraph until it is needed. This section is a natural continuation of Section 2.8, and we use the notation established there without further comment.

176

Líe Algebras Admitting Triangular Decompositions

Let A e 1^*, and let M(A) be the corresponding Verma module. Let ze and imagine that we make a “small perturbation” A^ = A + iz, i e K, in A. Presumably M(A^) is closely related to M(A). Indeed, if we identify M(A^) as a subspace of U(q_), these Verma modules can all be compared directly. In doing this, we find that for w e U(g_), the Shapovalov bilinear form F^(v,w) is a polynomial function in t. Loosely speaking is defined to be the subset of vectors u of M(A) for which F^lu, M(A)) c t^K[t] where t is now a variable. This gives rise to a filtration M( A) = Mq ^

D M2 D *• •

of g-submodules of M(A), a Jantzen filtration [see [Jz], Chapter 5]. We use this filtration to give us a detailed view of the way in which the singularities of arise, the main result being Theorem 4. Preliminary to even writing down the statement of Theorem 4, we require an algebraic apparatus to formalize the heuristic discussion above. Let g have a regular triangular decomposition (1^, g+2+,o-), and let K[i] be the polynomial ring in one indeterminate over K. Set 9 == IK[i] ®k 9Then g is a free (K[i]-module of rank equal to dim^^g. There exists a unique IK[i]-bilinear mapping [*, •]: 9 X g ^ g extending the Lie multiplication of g: [ p ( i) ® x , q ( t ) ®y] = p ( t ) q ( t ) ® [j;,y ] for all p ( t) ; q{t) e IK[r]; x, y e g. This makes g into a Lie algebra over K[t], It is also a Lie algebra over IKwith g as a subalgebra through x 1 ® jc. (See Section 1.1 for Lie algebras over rings. We will use the full generality of the Poincaré-Birkhoff-Witt theorem (see Remark 4 in Section 1.8) in the arguments to follow.) Now g has a triangular decomposition as a lK[i]-algebra in an obvious way, as we saw in Remark 2.1.3. We define §

H[t]

Í)

and 9+== ^ [t]

9,

2.9

Jantzen Filtrations

We identify 1^* with a subset of

177

— Honi|,^[,j(§, K[t]) by linear extension of

A(p ( t ) (S>h) = p ( t ) \ { h )

for all p ( t ) e K[t]; /i e 1^; A e f)*.

We make this identification without comment hereafter. Extend cr to <7 on § by linear extension: a(p(t)

= p ( i ) ®
Then our triangular decomposition is

where Q+<^

5*. For a e Q, r == K [i] ® 9“.

We set about constructing a suitable “Verma module” for g. Let U(§) be the universal enveloping algebra of g [viewed as IK[r]-module (Remark 4 Section 1.8)], and let A, z e 1^* be fixed in our discussion. Set A = A + rz e 5*. Define /(A) to be the left ideal of U(g) generated by g^. and all elements of the form h — Ae i { k ) = { U , h - \{h)\h

i/(g )-le ff

Then M = M(A) := U ( § ) / / is a §-module and is our desired Verma module (see 2.3(5)). For each /1 e let

M4 :=

! ^ v ^ M \ h - v = p ,(h )v

for all ft e §}.

Using Remark 3 of Section 2.1 and the arguments at the beginning of Section 2.2 we see that M=

© aeG+U{0}

178

Lie Algebras Admitting Triangular Decompositions

and that = IK[í]í)^.,

where i+== 1 + /,

M‘' ““ = U (g_) “

via M• (1 + / ) <-^ M-

This uses the Poincaré-Birkhoíf-Witt theorem (over IK[f]). In addition we will need the Verma modules (over g), A/(A + az), for various a e IK, which are defined as U(g)//(A + az), where /(A + az) = (g+, /z — (A + azXh) \h G ^>u(3)-ieft [see 2.3(5)]. Let a G K, and let £^;K [t] ^ K, p ( t ) *^p(«)> be the evaluation map. Since U(§) = »<[^1 «k « (s )’ ^ e have a K-linear homomorphism of associative algebras e„:U (g) - ^ U (9 ) defined by £a- P ( 0 ® ^ We evidently have e j9 = idg

(9 identified inside g ),

^0( 9 +) = 9±>

kei£a = (t - n)U (9)We recall the decomposition of 2.8(1): (1)

U(g) = U(^) ® (9 -fi(9 ) + ^ ( 9) 9+)

and the projection map ^ :U (g )-.U (^ )-W determined by this decomposition. In the same way we have (2)

U(g) = U ( § ) ® (9-U (§)

2.9

Jantzen Filtrations

179

and a projection i':U ( § ) ^ U ( § ) = 5 ( § ) . These projections will enter the picture in a little while when we consider the Shapavalov form. We next assemble the properties of that we need. Given / e 5(1^) and A e 1^*, we sometimes use the notation /[A] to refer to its value /(A) at A. We use similar notation for / e 5(§). This may avoid some confusion in the thicket of brackets that occasionally appears. Lemma 1 (i) ë ^ ° â = <7° s^. (ii) For all Ü G U(§), (iii) éa(/(Â)) c /(A + az).

= (qej^idxx + az],

Proof. (i) The proof is obvious. (ii) Write M= «1 + «2, where ii, lies in the ith direct summand in (2). Then q(ii) = Mj, qs^,(u) = ^(e^(iJi)). It is therefore enough to prove the result for u = Ui, where has the simple form p(t) ® f, pU) e IK[i], / G 5(f|). Then e<,(«(“ i)[-^]) =

+ tz])

= p ( ^ ) f [ ^ + «z], while (i?M “ i))[A + (iii) Since

= ( « ( P ( « ) / ) ) [ ^ + «2 ] = p ( a ) /[ A + az].

is a homomorphism, it suffices to check that 8+) ^ 9+j

which we already know, and that e^{h - A(A)) = e^(h) - (A + az)(e^(A )). It suffices to check the latter for h = p(t) ® h, p(t) e K[t], h

180

Lie Algebras Admitting Triangular Decompositions

Then ^a{pi0 =

i { p { t ) ® h)) - e ^ (p (0 ((A + tz){h)))

= e^(h) - p { a ) { \ + az)(h) = B^(h) - (A + az)s^{h) as required.



After part (iii) of Lemma 1 we have from

a natural mapping

= U ( g ) //( A ) ^ U ( g ) / / ( A + az) =M (A + a z) . In the sequel M(A) and M(A + az) are denoted by M and M, respectively. Lemma 2 (i)

i/i is a (U(§), U(g))-m<2/7 in the sense that for all v ^ M and for all X e U (§ ), • v) =

(ii) ker

= it — a)M.

Proof, (i) This is clear since (ii) M

M

is a homomorphism.

=

U (g )//(A )

=

\. U (g )//(A )

The result now follows from ker £„ - it

-

U (g_) i^a

^ a)U(§).

« (9 -) □

Now recall that the Shapovalov form on M(A + az) is obtained by defining F-. U(g) X U(9) ^ through F iu, v) = q i a iu ) y \ evaluating

2.9

181

Jantzen Filtrations

F(u, i;) at A + az and observing that the ideal /(A + az) is in the radical of this form. Thus we have an induced form on U(g)//(A + az) — M. Similarly we define F: U(g) X U(§) ^ S(§) through F(u, u) = q(a(u)v) and, after evaluation at A, we induce a lK[i]-valued bilinear form on M = U(§)//(A). Lemma 3 For all a ^ K and all x, y ^ M,

Proof. Let u,v ^ U(g_) correspond to x and y. Then £aFx{x,y) = e^(i((r(M )i;)[A]) =

+ az] A+ a z

by parts (i) and (ii) of Lemma 1.



We now make an important hypothesis (NDG)

F^ is nondegenerate i.e.

M(A)) = 0 <=>jc = 0.

For instance, suppose that to e 1^* can be chosen so that F^ in M(o)) is nondegenerate. Then for any A e f)* setting z = co - A, we have F^+z nondegenerate. Now let A = A + tz, and suppose that F^ (x, M) = 0 for some X Ei M. If X ¥= 0, then we can suppose that (t — 1) does not divide x [otherwise, divide out (t - 1)]. But then il/^ix) ¥= 0, and this contradicts Lemma 3. Thus, in this case (NDG) holds for A. For each A: = 0 ,1 ,2 ... define M,:= { i e M |( i - a ) * |F x ( i , M ) } . In other words, i e <=> Fj^x, y) is a multiple of (t - a)* for all y ^ M. Since is contragredient, it is obvious that is a §-submodule of M. Thus we have the filtration (JFl)

M = Mq ^

z>M2 ^ ■■■

of M. Since F^ is nondegenerate, n “ =o^* = (0)- We define M* =

A: = 0,1,2, • • • .

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Líe Algebras Admitting Triangular Decompositions

By Lemma 2, M* is a g-module, so we have the Jantzen filtration (JF2)

M(A + az) = Mo =) Ml D M2 3 • • •

of M(A + az). Furthermore This last result is not entirely obvious. We prove it in Theorem 4. The case a = 0 gives us a filtration of M(A). This completes the formalization of the heuristic discussion that opened this paragraph. If y e <2+ U{0}, then we have corresponding filtrations of weight spaces M^ where Mf-^ = M* nM^-^ = {jc eM^-T'|(i -a)*lFj;(jc,M^-^)} which is mapped by

onto

This last sequence stabilizes at (0) after a finite number of steps because M^^az-y ¡5 a finite-dimensional K-space for each y. Let y e <2+^{0}- We know that M^~'^ is a free IK[i]-module of finite rank (since U(g_) is a free lK[i]-module by PBW and K[t] is a principal ideal domain). Let {x^,. . . , be a basis for it. We are interested in the Shapo­ valov determinant det(Sh,,) = det(fx(x,,ii),. .) e K [i]. This is unique up to nonzero factors from IK. Let f i t ) e IK[i]\(0). The number o rd ,_ ^ /(0 is defined as the unique nonnegative integer k so that (i - a)^\f(tX but (t does not divide fit). Theorem 4 [Jan] Suppose that Fj^ is nondegenerate. Then (0 For all y ^ Q + n{0}, ord,_„(det Sh^(A)) = E^=i dim (ii) ch M^. = E^eQ^n,o, ord,_^(detSh.^(A)c(A + az - y); (iii) Mj is the maximal submodule N(X + az) o f M = M(A + az); (iv) n “ =o^* = (0).

< oo;

2.9

183

Jantzen Filtrations

The theorem is a direct consequence of the following general result that is also due to Jantzen. Proposition 5 Let A be a principal ideal domain and let p be a prime ideal o f A. Let (K be the field A / p . Suppose that X is a free A-module o f finite type, and set X •= X / p X with natural mapping ijj: X ^ X. Suppose that F: X X X A is a nondegen­ erate symmetric bilinear form, and let det(F) be the determinant o f the matrix {F{Xi, Xj)) for some basis {Jcj of X over A (note that det(F) is unique up to a unit of A). Let X^ = { x ^ X \ F { x , X ) and set

Then ordp(det(F)) = Y.

X*

k= l

(where ordp has the obvious meaning). Proof B. Let X ^ = Hom^(X, A) he the -.4-dual of X. Each x ^ X induces an element F ( jc, • ) of Let Y (zX^ be the submodule of all functionals induced by X in this way. Since the mapping x F(x, • ) is injective, ranky = rank X = rank X^. Using the well-known basis theorem [Jal] for modules over principal ideal domains, we can find a basis {e?,. . . , of X^ so that {a^e^,. . . , a^e^ is a basis for Y for some suitable elements a ^ ^ A \ {0}. Choose fi e X with F(f^, • ) = a^e^, and let {e^,. . . , be the basis of X dual to the basis {e^,. . . , We have

Since {/)), is a basis for X (because {a,e,}, is a basis of Y), there is a matrix S = (Sij) e GL„(A) with /, = £y_iS,yey, i = Thus d e tF = d e t ( F ( / ,,/,) ) = d e t|F (i;s ,.;C p /* jj = ( a ^... a^)Aet S.

184

Lie Algebras Admitting Triangular Decompositions

Since det 5 is a unit of ^4, we conclude that n

ordp(det F) = Y j ^rdp k=l

Let X = T.bjfj e X, Then Jc e

<=> ordp F[ej, x) > k <=> ordp ajbj > k

for ; = 1 ,..., n, for y = 1 ,..., n,

<=> ordp bj > k - ordp aj. Now feyCmod p) = 0 unless ordp bj = 0. Thus X¡^ = € A / p ) = Eord„a )•/'(/;)> where J(,k) ■■={j e { 1 ,..., n}\k - ord„ a. < 0}. Thus ' diniK Xk = card(/ lordp aj > A:}, and hence L dim^ k=l

= L ordp ÜJ = ordp(det F ). j=l

Proof o f Theorem 4. (i) This follows from Proposition 5 with ^ = IK[r], X = M ^~f, p = U - a)IK[r], and so on (ii) This is an immediate consequence of part (i) (iii) Let X e M, and let jc e M be any preimage of x. Then using Proposition 2.8.2 and Lemma 3, X e AT(A + az) <=i>

M) = 0

<=>Jc e Ml jc e Mj. (iv) From part i, fl

= (0) for all y e Q+ U{0}.



2.10 BERNSTEIN-GEUFAND-GELTAND DUALITY The origin of this section is a paper by Bernstein, GelTand, and GelTand [BGG2]. Their theory was worked out for finite-dimensional split semisimple

2.10

Bernstein-Gerfand-Gerfand Duality

185

Lie algebras. The generalization to the infinite-dimensional case was carried out by Rocha-Caridi and Wallach [R-CW], and this section follows their paper. The motivation for [BGG2] was a certain duality principle that had appeared in the category of finite-dimensional ^-modules for certain finite-dimensional associative algebras A over a field IK. Suppose that {Lj,. .. , L„} are the irreducible ^-modules (up to isomorphism). For each L, there is a unique indecomposable projective module for which Hom^(/^, L^) ^ 0. Let = [¡¿: Lj] be the number of occurrences of Lj in a composition series of The matrix C = is called the Cartan matrix of A (no relation to the Cartan matrices that appear in Chapter 3 and play such a fundamental role in all of the rest of the book!). For certain A,C = D^D for some integral matrix D (not necessarily square). In particu­ lar C is symmetric and positive semidefinite. One natural way to interpret this would be to find a collection . . . , M„} of “intermediate” modules that occurs as the factors in certain descending series for each /¿. If we denote by [/^: M^] the number of occurrences of in li in such a series and by [M^ : Lj] the number of occurrences Lj in then c^y = [li : L y ] = : L y ] . Thus, if it were true that the “duality principle” [/^: M^] = held, then C = D^D for D = (d^tyX where == : L y ]. In this section we construct various subcategories of the category for which just such a duality principle holds, the and Ly being the Verma modules and irreducible modules in this subcategory, respectively. Our main task is to construct the indecomposable projective modules for which the Verma modules are to play the intermediate role. In Section 2.11 we will use this duality principle to prove a basic result about embeddings of Verma modules into Verma modules. Let g be a Lie algebra over IK with regular triangular decomposition (f), g+, Q+, cr). Fix A e ]^* once and for all. We define if(A) to be the full subcategory of <^(g, T) whose objects are those modules M of ^ for which M=

© tei)*

and = (0) if fjL ^ A i Q^. We define Fif(A) to be the full subcategory of if(A) whose modules are finitely generated g-modules. Note that if M is a module of F-^iA) with the finite set of generators Xi = E x f, i = 1 ,..., AT, where x f g then {xf'l/ = 1 ,..., n, e 1^*} is also a finite set of generators. Thus modules in F-^ have finite homogeneous generating sets.

186

Lie Algebras Admitting Triangular Decompositions

Proposition 1 (i)

T^(A) is closed under taking submodules, forming finite direct sums, and forming quotient modules. In particular i^(A) is an abelian category. (ii) Fif(A) is closed under forming finite direct sums and forming quotient modules. (iii) For all fjL E: M(fji) and L(fi) are objects in Fif{A) and -é'(A) and the modules L(/i), At g A J, ¡2+? precisely, up to isomorphism, the irreducible modules in if{A). Proof. The only part that is not immediately obvious is the statement about the irreducibles in A), and for that we use Proposition 2.6.6. □ Since A is fixed, we will feel free to abbreviate if(A) and F ^(A ) to F-é" respectively.

and

Lemma 2 Let M be a module in F€. Then any proper submodule N o f M in -é" lies in a maximal proper submodule o f M in -é. Proof Let jCj,. . . , be a set of generators of M, and let N be any proper submodule of M in Choose k as large as possible so that the module generated by {N, . . . , x¡^} is not all of M. Let ^ be the set of all submodules K oí M ijm -é") such that Nj^
¡ jl

and P^, P2 as defined above,

P^ is finite, a G P , P^Q+\J{0}=>a+P 2

G P2 .

2.10

Bernstein-Gerfand-Gerfand Duality

187

Proof, (i) See Lemma 2.6.1. (ii) If on the contrary a + /3 e then /x + o :H -)S e A l(2 + , and hence also /i + a e A l Q ^ . This contradicts a e P2^ Consider the decomposition 1 1 ( 9 © U ( 9 j “ e © U(gj". a^Pi ol^P2 Then from Lemma 3 we obtain Lemma 4

is an ideal o f U(g+).



For /1 e A 1 ¡2+ we provide U(g+) with the unique g+0 1^-moduIe struc­ ture satisfying (jc + /z) • M= for all

e

+ a , h )u + XU /z e ]^, w e U (g+)“ ; a e (2+U{0}.

(This can be thought as the restriction to g+0 with lowest weight ^t). Let

of the Verma module of g

IV= W ( pl) : = U ( g J / © U ( g j \ a^Pz Now from the fact that 0^eP2^^^+^'' U(9+) we see that it is stable under the action of g+0 which we have just described. Lemma 5

W is a g+0 ^-module with the action x ' и = x и for all x e g+0 f) and и e U(g+X ^here “ :ll(g+) ^ Wis the natural quotient map. □ P(ju) is defined to be the induced g-module P ( p ) = P ( p ; A ) := и ( д ) 0 ц , ^ е ^ W( p ) .

Lemma 6

Let {iV/Xe / basis {1 ®

basis o f W{fx). Then P(/x) is a free left Vi(g_)-module with Furthermore, if for each i, w¿ is a weight vector o f weight %

Líe Algebras Admitting Triangular Decompositions

188

for 'i), then 7/ = M + ßi for some unique weight % in P(ix),

: P^, and in this case 1

w¿ is of

Proof By Corollary 2 of the PBW theorem U(g) is a free right U(g+0 module with any basis, say, {ujij^j of U(g_) as a basis. Thus P(/x) is the linear span of the vectors {uj ® w^}j and these vectors are a IK-basis for P(fi). Then the vectors {1 <S>w¡\¿ certainly generate Pifi) as a left U(g_)module. Moreover, if £¿^¿{1 w¡\ = 0 for some e U(g_), then writing z, = LjCijUj, Cij e K, we obtain 0 = LijCijiuj ® w¿X whence each c^j = 0. This proves the freeness. The statement about weights is obvious. □ Proposition 7 Pip) e F i f i M Proof W as a vector space. Since P^ is finite and, for all a e ¡2^, dim U(g^_)" is finite, we see that dim W is finite. Thus, by Lemma 6, Pip) is finitely generated as a g-module. Choosing a basis of W consisting of weight vectors, we see from Lemma 6 that Pip) is a weight module and that all of its weights lie in UaepjiM Л- a ) l Q ^ ( z К I Q ^ . Furthermore, since U(g_) has finite-dimensional weight spaces, it follows from Lemma 6 that Pip) does too. Thus Pip) ^ -^(A). □ Proposition 8 For every M e -^(Л), Hom^iPip), M) - Hom^(IK^, M). Explicitly the iso­ morphism is given by

Ф:Ф(Л)(г;о) =Л(1 0 1) for all A e Нот ^iPip), M), and its inverse is given by linear extension of 4 ^ (/)(x ® y) =д: у -/(i^o) for all f e Horn j(IK^, M). Proof. Let us check that Ф(А) is an ^-module map from IK^ ^ M. For all Ae h ■Ф (^)(У о) = h A ( i ® T) = A { h ■(1 ® 1)) = A{h ® 1) =A{1 ® /г - I ) = A(1 ® = Ф(А){({1,1г}оо) = Ф ( А ) ( к ■Vq), where we have used the fact that 1 e U(g+)°. Now consider First we should prove that it is well defined, namely that X • у ■fivo) is independent of the choice of у e U(g+) with у y. But, if

2.10

B ern stein -G el’fand -G el’fand D u ality

1»9

also y ' ^ y , then y ' = y + u , where u e e„ei>2^(9+)“- However, V q ^ and / e Hom^iK^, M) - /(t;«) e U(g^)“ • fiv^) e = (0) f^r all a Ei P2 since M ^ -^(A). Thus u ' fiv^) = 0. It is now clear that ^ exists and is linear. Let z e g. Then ^ (/)(^ ■

® ^)) = ■ ^ ( / ) ( ( ^ ) ® y) = ( z x ) y - / ( V o ) = z - x - y -f{Vo) =z •

®y ),

showing that ^ ( / ) ^ Homg(P(/i), M). Finally, we have < I > ( ^ ( / ) ) ( ^ o ) = 'P ( / ) ( l ® i ) = / ( ^ o ) and ^((^))(a;: ® y) = jc y • (^)(i;o) = X • y • A(1 <8> 1) = .4 (;r y

(l® I))

= A ( x ® y ), showing that and ^ are inverses of one another. Proposition 9 P(li) is a projective module in the category ^(A). Proof. Consider a diagram Pitx) N

^ M -

0

where all the modules and maps are in ^(A ). Then, in the notation of Proposition 8, we have

f/ / N ^

/

IK. 4>(A)

M ^

0

for which we can obviously find f e HomgOK , A/^), making the diagram

Lie Algebras Admitting Triangular Decompositions

190

commute. Then by Proposition 8, 'ir(f) ^ prove that g = A. But g o ^ ir(/)(jc ® y )

N). We want to

= g { x - y -fiVo)) = x - y - gi f i vo) ) = X ■y • ^ { A) V q =

'P (< I> (^ ))(JC ®

y)

= A { x ® y).



Proposition 10 Every object of F-^(A) is the image o f a projective module of the form 0/L i P(A^) for some A, 0 Proof Let M be a module in Fif(A), and let be a finite generating set consisting of weight vectors, say, m^ g From /¿: M^‘, 1 •-> as ]^-modules, we have ^(/¿) ^ Homg(F(A^), M). Then adding, we obtain a surjective map M. i= l

But ef=iP(A^) is projective and lies in Fif(A).



An important method for proving results in ^(A ) is the use of Verma composition series (VCS). The definition and basic properties appear in Section 2.6. The next few results deal with Verma composition series for certain modules in i^(A). If M has a VCS, then /(M ) denotes the length of one (and hence any) such series of M. Proposition 11 (i)

P(/x) has a Verma composition series. (ii) For a l l V 0 A i (2 + , [ P ( ijl): dim H om g(P(^), M(v)) (iii) [Pip): M(v)] = 0 unless < v < A.

M(v)] = dim

=

jjl

Proof Let {wJ/Li be a basis for W •= Wip), which is chosen so that e for some /3^ e P^ and so that > Pj => i > j. Let Wf^ := k = 1,2,... ,n, and define + i == (0). Thus W = W^z>W2 D • • • => Z) + i = (0). Observe that g+IT; d since e and Pi + a > p^ for all a e A^_. Since is also a weight module, is a (g+0 ]^)-module.

2.10

Bernstein-Gel’fand-GeFfand Duality

Inside P iti) = U(g)

191

define M ,:= U (g_) • (1 ® = U(g) -(1 ® IT,).

Then P{li) = M i d Mz Since the elements {1 ® w^} from a basis of P()ti) as a U(g_)-module, it is obvious that is a free U(g_) module of rank 1. Since 1 ® has weight ßk + f i , we see that = M(ß^ + ¡jl) (Proposition 2.3.3). This proves part (i). Since the multiplicities [P{^í)■.M(.v)] are invariants of the first equality of part (ii) follows from [P()u,):M(v)] = card{*lj3;t + ¡i = v) = dim For the second part of (ii) we have for e A | Ö+. dimHomg(F()u.), M (v)) = dimHom^(lK^, Af(v)) = dim M (v)^ = K(^v — ¡x) = dim U(g+)*^ ^ , where K is the Kostant partition function (Section 2.5). We get zero here unless V — IX a ^ Q+ U{0}. Then ix + a = v < h. v — ¡x = a ^ P^. Thus dim U(g+)’^-'‘ = dim (iii) In the proof of part (i) the only Verma factors M{v) occurring have V = !x + ßi^iox some jß^ e P^. □ Proposition 12 For M ,N ^ T^(A), M ® N has a VCS if and only if M and N have VCSs. Furthermore, if M, N and M ® N have VCSs, then for all weights fx, [M ® N, Miix)] = [M, Miix)] + [N, M(ix)l We prove Proposition 12 using the following lemma: Lemma 13 Suppose that M has a VCS, and suppose that fx ^ M is a maximal weight in M. Let 0 V M ' ^ , and set M ' ■= U(g) • v+. Then M ' = Mip ) and M / M ' has a VCS with l i M / M ’) = /(M ) - 1. Proof M' is a highest weight module with highest weight pair (ix,v+). Let M = M q Z) • • • D M; = (0) be a VCS (of length /) with M¡/M¡+l = M(ju,,). We prove the result by induction on /. If / = 1, M ' = M q = M q/M^, and we are done. Suppose that / > 1. If then by the induction assumption applied to Afj we obtain M' - Mip), and A /j/M ' has a VCS

Líe Algebras Admitting Triangular Decompositions

192

with KM^/M') < Then M / M ' has a VCS by adjoining the top term M /M j and KM /M') = 1 + KM^/M') = 1 + l(M^) - 1 = /(M) - 1. We are left with the case / > 1, u +^ Let M' ^ M/M^ be the canonical map. Then ¥= 0, and by the maximality of fi we obtain fi = ijlq and M /M^ - M(/i) = U(g) • D+. From the universal property of Verma modules we obtain a homomorphism (p : M ( f i ) M ' with v+. Thus the exact sequence 0 ^ Ml ^ M ^ M /M i == M(fi)

0

is split, and

M Now M' == M(fi) and M /M '

Ml 0 M'. has a VCS with /(Mi) = /(M ) - 1.



Proof of Proposition 12. If M = Mq D Ml D • • • D M^ = (0) and N = N q D Vi D • • • D = (0) are VCSs, then M e V = M o 0 A /^ D M i0 V D ••• D M^ 0 V = Vo D Vi D • • • D = (0) is a VCS for M 0 V. Conversely, let / be the length of a VCS for M 0 V. If / = 1, then evidently M = (0) or N = (0) since Verma modules are indecomposable (Proposition 2.2.2). Thus we may assume that / > 1. Let be a maximal weight of M 0 V, and for definiteness suppose that M^ ¥= (0). Let 0 # i;+e M^, and let M' = U(g) • u^. By the last lemma, M' == and (M e N ) / M ' — M / M ' 0 N has a VCS of shorter length than M. By induction on / we may assume that M /M ' and N have VCSs, whence also M and N. Now the statement on multiplicities follows from the first part of the proof. □ The next sequence of results aims at proving that every projective module in F ^(A ) has a VCS. Proposition 14 Every module in F-^ is a finite sum o f indecomposable modules, which are also in F-^. Proof. Any M e Fi^ has a finite set of generators consisting of weight vectors. Let G •= {¿;i,. . . , be such a set of generators, and let v^ 0 M^‘. Define o-(G) == E dim M^. We define o-(M) — min^ o-(G) as G runs over all such sets of generators of M. We prove this result by induction on o-(M). If cr(M) = 1, then M = U(g)i; for some v e M^ with dim M^ = 1. If M = Ml 0 M2 for some submodules, then M^ = M f 0 M^ => M f = (0), or

2.10

Bernstein-GeFfand-GeFfand Duality

193

= (0). Say, = (0). Then v e M f and M = Thus M is indecom­ posable. Suppose that 1. If M is indecomposable, there is nothing to prove. Suppose that M = 0 M2, where and M2 are nonzero submod­ ules. Let G be a generating set of weight vectors of M with a{G) = cr(M). For each g e G write g = gj + g2, g, e M,.. Then G^ := {gjg ^ G) ^ {0} generates M^, i = 1,2. From = Mf 0 for each ¡jl we see that < cr(Gi) < <j(G) = a(M), Thus and M2 have finite decomposi­ tions into indécomposables, hence also M. If M = where each Ij is indecomposable then clearly M e => Ij e F if for each ;. □ Proposition 15 (i) For all p. Ei K iQ ^ , P(fi) is a finite sum of indecomposable modules. (ii) A module M in Fi^(A) is projective if and only if it is a direct summand of 0/LiF(A^) for some A^,. . . , 0 1^*. (hi) Every projective module in Fi^(A) has a VCS. Proof, (i) Use Propositions 7 and 14. (ii) Let M e F # be projective. By Proposition 10 we have Aj,. . . , A^ e 1^* so that there exists an exact sequence

© F(A ^) ^ M - ^ 0 .

Since M is projective the sequence splits, and hence M is a direct summand of 0F(A¿). Conversely, any direct summand of a projective module is projective. (hi) Use Propositions 11 and 12. □ We now move toward the connection between indecomposable projectives in F ^ and irreducible modules in F if. Proposition 16 Each projective indecomposable object in Fif(A) has exactly one maximal proper submodule {in i^(A)). Proof. The existence of maximal submodules is given by Lemma 2. Now let I be finitely generated, projective, and indecomposable, and suppose that Mj and M2 are distinct maximal proper submodules of /. Then M^ + M2 = I.

194

Líe Algebras Admitting Triangular Decompositions

Form the direct sum of

and M2. Then we have Mj 0 M2

0,

where m ^) = + .m2 and i/i is known to exist so that cpij/ = id^ by the projectivity of I. Let p^: M^ 0 M2 ^ M^ be the natural projection, and define f¿ = / -^ c I, Then /1 + /2 = id/. Indeed for jc e 7, (/j + f2)(x) = (Pi + P2^° = (p° il/(x) = jc. Thus in particular /1 ° /2 = /2 ° /1 in the ring Endg(7). Let 7 be a finite sum of weight spaces 7^ so that J generates 7 (since 7 is in Fif). Fix 1 = 1 or 2. Since is a g-module map, //(7^) c 7^ and hence /.(7) c 7. Now we make a slight variation on Fitting’s lemma [Ja2]. Since dim 7 < 00, the descending chain / d / , ( / ) d / 2 ( / ) d ••• stabilizes at some A/j, so we have f^>U) = = • • • . Since / = U(g) • J, we have /■^'(/) = U(g)/^^'(/) = U(g)_^^''^*(/) = = • • • . Fix any weight fjb, and consider ■= Then by Fitting’s lemma [Ja2]

where s Z i n == n k= l

and « r ( 0 ) == U /t=i

= 0}.

Now by what we just proved = g^'C/**) = and hence = /^^‘( /) which is a submodule. We also see that if x = Ex^ e ®g~”(0), then for each nonzero x^ there exists ^ with /^ '‘Xj^ = g^*‘x^ = 0, and hence for k ■= max{A:^}, /¿*x = 0. Thus, in the obvious notation, x e / ~ “(0). Conversely, x = Ex^ e / r “(0) x^ G g ; “(0) for all M. Thus / " “(O) = e g ; “(0). In summary then, /= =

e { g Z i n ® 8Z^(0)) At © /r(0 ).

2.10

Bernstein-GeFfand-Gerfand Duality

195

This decomposes I into two submodules. Since I is indecomposable, one of them is (0). But /;.(/) c M, # /, and hence f ^ ‘i n * 1. Thus = (0). Set N = max{iV,, Then finally, since /, and / , commute, we have the contradiction id, = id2^ = ( / i + / 2 f ” = 0. This proves the uniqueness.



Proposition 17 Let L be an irreducible object in -^(A). Then, up to isomorphism, there is a unique finitely generated projective indecomposable module in i f that has L as a quotient. Proof (Existence): Since L is irreducible it lies in F-f. By Proposition 10, L is the homomorphic image of a finitely generated projective module P of -f. By Proposition 14, P = ®/Li/y where each /y is indecomposable. Since L is irreducible, L is the homomorphic image of one of the Ifs. (Uniqueness): Suppose that and I2 are finitely generated projective inde­ composable modules and that 7t¿: L are surjective homomorphisms. From

// / A ^1

TT2 0

we obtain / , making 771° / = 772- Now ker 77 ^ is the unique maximal proper submodule of (by Proposition 15). It follows that / is surjective, for if not, by Lemma 2, / ( / 2) lies in a maximal proper submodule of I, and hence lies in ker TTp But then 772 = ttj ° / = 0, which is not the case. Since 0 ker / ^ /2 ^ /1 0 is exact and is projective, there exists a homomorphism g: 12 splitting this sequence. Then 12 = k e r /e g /^ . Since ¡2 is indecomposable, ker / = 0. Then I 2 - h^ Propositions 16 and 17 establish a 1-1 correspondence between irre­ ducible objects in -f(K) and finitely generated indecomposable projective modules in -f(K). However, we already know (Proposition 1) the irreducible objects in -f(hj), namely the modules L(p), e A 1 (2+. Let / 1 < A . We define K / jl) to be the unique (up to isomorphism) finitely generated indecomposable projective module in i f ( A ) having L(/i) as an irreducible quotient.

196

Lie Algebras Admitting Triangular Decompositions

Every finitely generated indecomposable projective module in -^(A) has the form /(/x), /jl < A, Proposition 18 Let M G. t^(A). Then for all

¡jl

^ A iQ+,

[M:L{ii)] = dimHomg(/()Lx),M). In particular dim Horng(/()Lx), M) = 0 if

= (0).

Proof We begin with the simple observation that if I, M q, a category, I is projective, and M q Z) M^, then

are modules in

H om (/,M o/M i) = H o m (/,M o )/H o m (/,M i). Indeed every map / : / ^ Mq induces another, namely / : / -> M q/M^ and / = 0 iff / ( / ) c Mj. Thus there is an injective map A:Hom(/, M o)/H om (/, M^) Furthermore, if M q/M^, then since / I -> M q for which g = g, thus proving that It follows th at dim H o m (/, M q) dim Hom(/, Mf), Extending this by induction, we see that then

H om (/, M q/M^). is projective, there is a map g: A is surjective. = dim H o m (/, M q/ M ^ ) + if M = Mq 3

( 1) d im H o m (/,M )= E dim Hom (/, /=1

z> • • d M^,

+ dim Hom (/,M ;t)-

In our present case let M = Mq Z) Z) • • • d Mi^ = (0) be a local com­ position series at fi (Section 2.6). For each i either Mi_^/Mi — ¡Hi > f i o r M f ^ _ ^ / M i has no weights r > /x. In the former case X (2)

VÍ = (0)

if A

AX,,

2.10

Berastein-Gerfand-Gerfand Duality

197

Since

1. I(fji) has only one maximal proper submodule, call it 2. = Ufi), 3. Endg(L(/x)) - K.

Rifi),

In the latter case let us show that Н отд(/(д), = (0). Let / e Н отд(/(д), Since Li/i) is a quotient of I(fi) and {M i-i/MiY = (0), we conclude that kei f Rifi), = I( ijl)/R(/ jl)). Now Lemma 2 and Proposition 16 combine to show that / = 0. Since [M: L(/x)] is the number of times L(/i) occurs as a quotient in a local composition series at fi, Proposition 18 is proved. □ Proposition 19 Lei Д e Л 1 2+. Then ®

(finite sum),

where = dimHomg(P(jLi),L(i/)). We have

m j^v) = 0

fi < v < A,

Proof. By Proposition 14, P(jLt) is a finite sum of indécomposables. Of course each of these is finitely generated since P(/i) is. As we have seen, every finitely generated projective indecomposable module is an I(v), i; < Л. Thus

for some finite set of p and integers m jiv). Furthermore dim Horn g( P ( Д ), L(iü)) = dimHomg( ф mJ^p)I{p),L((o)^ = Lm^i/)dimHomg(/(i/),L(û>))

from 2. But from Proposition 8, dim Н о т д ( Р ( д ) , L((o)) = dimHom^CK^, L((o)) = dim L{o)Y. Thus mjfii) = 1 and mjfo)) = 0 unless (i < (o < A. □

198

Lie Algebras Admitting Triangular Decompositions

Theorem 20 (BGG duality) For all ii,v Ei A i Q+, [M{n.)-.L{v)] = [ / ( v) : M ( m)] in the category i^(A). Proof. From Proposition 18, it will suffice to show that [ l( v ) : M { fi ) ] = dim Horn g(/(i/),A i(iu,)). Let /Ji,v E A i Q^. Using Proposition 19, write (3)

P{v) = © m^{(o)I{(o),m^{a)) E I^.

We have (4)

[ P ( i') : M ( m)] = 'LrnXo>)[l((o) : M(v)]

by Proposition 12. From (3), Homg(P(v),M(M)) = Em,(a>)Hom3(/(a>),M(»^)) so from part (ii) of Proposition 11, (5)

[P(v): M {fi )] = E "i.(i^ )d im H o m g (/(a )),M (i/)).

As ¡jL,v vary we may consider (4) and (5) as systems of linear equations with the same matrix of coefficients (m^(ci))). Since mj^v) = 1 for all v and m^((o) = 0 unless i/ < co < A, we see that the matrix (m^(co)) is unipotent relative to any ordering of A i Q ^ that respects < . In particular the matrix is invertible, and we obtain at once that for all (o,v E A i Q^, dimHomg(/(io)

= [l((o):M(v)]

as required.



Corollary For any VCS o f Kfi), / ( m) =/o=>/l=5 ••• =>/„-!=>/„ = (0),

2.10

Bernstein-Gerfand-Gel’fand Duality

199

we have Io/I,^M (ß), Ij/Ij+i = M(vj),

vj> fi, j = 1 , 2 , . . . , n - 1.

Proof, [/(/x): Miß)] = [Miß) : Liß)] = 1. Thus in any VCS for I(ß) exactly one subquotient is isomorphic to Miß). From li ß ) Miß )

Liß )

0

we have a map ilr. l i ß ) M iß ) and iJ/Hiß)'^) ¥= (0). Thus iffHiß)) contains a generator of Miß), so if/ is surjective. Consider /j. Since it lies in the unique maximal proper submodule of l i ß ) (i.e., /j c ker tt), we have if/Hi) c Miß). Thus if/Ui) c N iß ) and I q/ I i -* M i ß ) / N i ß ) = Liß), which shows that /o //i = Miß). □ We may interpret the duality theorem in the way suggested in the introduction to this section. Set ==

Liv)]

and '■= [ ^ i f J - ) '■Liv)] Consider the matrices C = c^„- =[l i ß) - H^) ]= =

D =

for all

V e A i Ö+.

We have

E [/(cu):M (ir>)][M (a>):L(i^)] /1, V<(0

E [Mico):Liß)][Mi fJL,V<0)

Thus C =

and in particular C is symmetric and positive semidefinite.

200

Lie Algebras Admitting Triangular Decompositions

2.11

EMBEDDINGS OF VERMA MODULES

Throughout this section g is a Lie algebra with a fixed regular triangular decomposition and & is the category Let A e ]^* and consider the Verma module M(A). It is a very interesting problem (going back to Verma’s original work on these modules) to decide when another Verma module M(/¿) appears as a submodule of M(A). In the case of an invariant Kac-Moody algebra g, we will obtain an exact answer in Section 6.7 to this problem for a large range of values of A (all A when dim g is finite). If M ( ijl) is a submodule of M(A), then clearly Homg(M(/¿), M(A)) ¥=(0). Conversely, if e Horn ^ ( M ( ijlX (p ^ 0, then ( p ( M ( f i ) ) - M(/x) by Proposition 2.3.3, and hence M(/x) is in effect a submodule of M(A). Thus we are looking for conditions under which Homg(M(/¿), M(A)) ¥= (0). The main result of the section is Theorem 1 (Ku [Kuly Neidhardt [Ne]) Let

f)*. Then [M(A): L(/x)] ^ 0 <=> Homg(M (/x),M (A)) ^ 0.

The hard direction is “ => .” Our proof is taken from Neidhardt [Ne] and relies on the BGG duality theorem (Proposition 2.10.20). Proposition 2 Let )LL e and let N be a ^-module in category & that has no weights A with A > jLt. Then Extg(M(^i), N ) = (0). Proof. Consider any extension (1)

0^

^ P ^ M( f i ) - ^ 0 .

Let P^ be chosen so that fjL, (pv^ is 2lhighest weight vector of P. Since M(¡i) is a Verma module, there is a unique homomor­ phism (/í : M( jjl) -> P with {¡/((pu^) = u^. Clearly

/x. Thus M{iD and L(A) lie in the category ^(A). Consider the indecomposable

2.11

201

Embeddings of Yerma Modules

projective g-module /(/x) in ^(A). We are going to prove that > 0 and hence by BGG duality that [M(A): L(/x)] > 0. Let

[ K

i j l)

:

M(A)]

/ ( m) = / o ^ / i => ••• 3 4 _ i D/„ = (0) be a VCS for /(/x). We have 4 / 4 +1 for some weights /x^, where /xq = fi. (See Corollary of the BGG theorem, Proposition 2.10.2). Let 0 -> L (A )

0

be a nontrivial extension. From the natural map tt : I(fi) = 4 ^ M(/x) with kernel 4 from the projectivity of /(/x), we have /( m) T_T/ / /

0 ^

L(A)

P ^

M (fi)

0

with (p o TT = 77.

Now (p o 77(4 ) = '^■(4 ) = (0), so ^ ( 4 ) ^ ker 9 = L(A). In fact 77(4 ) = L(A), for otherwise ^ ( 4 ) = (0). Therefore 77 induces ¥: 7( m) / / i(= V A = M (n )) ^ P, and then splits the sequence contrary to it being nontrivial. Since L ( A ) = 7 7 ( 4 ) ^ D • ‘ • D 7 7 ( 4 - 1 ) ^ ^ ^ ( 4 ) ^ (OX there is a A : such that ^ ( 4 ) = L ( \ \ 'ñr(4+i) = (0) and hence a surjective map M(jjLf^) ^ 4 /4 + 1 ^ ^(>^)- This can only mean that /x^ = A, and hence [/(/x): M(A)] > 0, as we wanted. □ Proposition 4

Let M E: 0 be a highest weight module o f highest weight A. I f Extg(M(jLx), M ) (0), then Á. > jjb, and for some v e ij* with X > v > 11 we have [M(X):L(p)] > 0 and [M(v): L(fji)] > 0. Proof We have A > ju by Proposition 1. By assumption there is an exact sequence 0 -^N

M

L(X)^0,

where N is some maximal submodule of M. Every weight cp of N satisfies X >
202

Lie Algebras Admitting Triangular Decompositions

Using Corollary 1 of Proposition 1.12.4 we have Extg(M(iU.), L(A)) # (0), or Extg(M()u.), N ) ¥= (0). In the first case we obtain [M(A): L(^)] > 0 by Proposition 3, and hence we obtain our desired result with v = k. Suppose that Extg(M(/i), N ) # (0). Let ( 2)

N = N ^ z> N ,^ ••• 3AT„_i DA^„ = (0)

be a local composition series for N dX yi. By Corollary 2 of Proposition 1.12.4, Extg(M(^t), ¥= (0) for some ;. Using Proposition 2 = L{v) for some v. Then by Proposition 3, [M{v) : L()it)] > 0. It remains to see that [M(A): L(z/)] > 0. But is a subquotient of M(A) (since M is a quotient of M(A)) and[A/^:L(i/)] > 0. The result follows from the Corollary 1 of Proposi­ tion 2.6.13. □ Proof o f Theorem 1, (<=) By assumption there is a nontrivial g-module homomorphism 0 at once. (=>) The proof is for all pairs A, m,(A > m)? by induction on h t(\ — ¡i). If h t{\ - m) = 0, then \ = ¡JL, and the result is trivial. Suppose that A > m- Lot MA) be the maximal submodule of M(A). Since [M(A): L( m)] > 0 and A > Mj we see by refining M(A) d MA) d (0) that jjl

(3)

[N (k) :

>0.

Let

(0) = A^o c ATj c iVj c be a HWS of MA) (Proposition 2.6.10). Each is a highest weight module, say, of highest weight i = 1 ,2 ,... . Evidently (4)

A > )u.,

From

: L(/a,)] > 0 we obtain

(5)

[M A ) : L (n ,)] > 0,

for all i.

[M(A) : L ( m,)] > 0.

By part (iii) of HWS of Section 2.6, there is a A: such that = N'^. It follows at once that [M A )/M ^LC^u.)] = 0, and hence from (3), [M •

2.11

Embeddings of Yerma Modules

203

Lifi)] > 0. Thus for some j < k , [Nj/N j _ i : L(ju,)] > 0, (6)

and

[M(/ty) : L(/ii)] > 0

My ^

Case 1. fjL Ф fjLj. Then к > ¡Xj> ji. Using the induction assumption, Ф

(0),

n o m ^ {M ifij),M (X )) Ф

(0),

and so combining, we obtain Homg(M(/x), M(A)) Ф (0) as required. Case 2. 11 = fij. Then Nj/Nj_^ is a nonzero homomorphic image of Mill), and clearly Нотд(М (д), ^ (0). Let 0 < / < ; be chosen minimal so that Нот J^Mifi), N ik )/N¿) Ф (0). If i = 0, then Homg(M(/i), MA)) Ф (0). Consequently Нот^iM ifi), M(A)) Ф (0), and we are done. If i > 0, then from the exact sequence 0^N,/N,_, ^Nik)/N,_, -^Nik)/N,-^0 we have the exact sequence (Proposition 1.12.4),

Since the first term is (0) and the second is not, neither is the third; that is, Extg(Ai(/i), Ni/N i_i) ^ (0). Applying Proposition 4, there is a weight V e ]^* with X > ( i j > V > f x s o that : L (v)] > 0 and

[ M {

p

)

: L (/i)] > 0.

The induction assumption gives us Homg(A/(v), ¥= (0) and Homg(Ai(ju,), M{v)) ¥= (0). Furthermore from (5) and the induction assumption Homg(Af(ju,,), Af(A))) # (0). Combining all these, we obtain the desired result. □

2(M

Lie Algebras Admitting Triangular Decompositions

2 .12

D EC O M PO SITIO N OF M O D U LES IN CATEGORY Û

According to Section 2.11 the embedding of Verma modules Mijx) ^ M(A) is possible if and only if [M(A): Lifi)] > 0. A central issue is then when is [M iX ):U fi)] > 0? This question can only be answered adequately by spe­ cializing the class of Lie algebras g under discussion. This is precisely what we do in Chapter 6, where g is assumed to be an invariant Kac-Moody algebra. However, the relation on 1^* defined by A /i if and only if [M (A):L( m>] > 0 does lead to a useful equivalence relation on certain subsets (characteristic subsets) of 1^*. The main result of this section shows how this notion leads to a natural decomposition of any module M lying in Û into submodules, each of which lies in a subcategory of ^ governed by the equivalence relation. The material is derived from [DGK] with some simplifications from Section 2.11. These results are not used until Section 6.8 and are not necessary for any other part of this book. We will assume throughout that g is a Lie algebra with fixed regular triangular decomposition <5^= (^, g+, Ô+? ^ind that Q is finitely gener­ ated. A nonempty subset 5 of 1^* will be called characteristic if it has the following property Ae 5

and

[M(A) : L(/¿)] > 0 =>

e 5,

or equivalently, A e5 = > ch M (A )= for some family sets:

Y. c^ch L{/jl) fJL^S

in N. The following are examples of characteristic

1. Í)*. 2. P := {A eri< A ,a,-^ > 3. A 1 (2+ for A e

Z for all i G J}.

For A, we write Á > ¡jl if and only if [M(A): Li/i)] > 0. Let 5 be a characteristic subset of 1^*. We define an equivalence relation = '^s ^ as the transitive closure of in 5; that is, A /x <=►, there exists Aq, Aj, . . . , A„ e 5 such that Aq = A, A^ = ¡jl, and either A¿_j -< A¿ or A¿ A,_i for all i < i < n. For y e 5 we will let f denote its equivalence class in S. Each equivalence class of S is itself a characteristic set. Let 5 be a characteristic set. A module M in <^(g, 5^) is said to be of type 5 if [M :L (A )] > 0 => A e 5.

2.12

Decom position o f M odules in Category

205

&

Equivalently M is of type A if c h M = £ c ;,c h L ( A ) . Ae5

Let S c ]^* be a characteristic set. We define a category as follows:

= ^ 5(9,

1. The objects of 0^ are the objects M of ^ of type 5 2. The morphisms of 0^ are all the g-module homomorphisms between the objects of 0^, It is clear that direct sums, submodules, and quotient modules (see Proposition 2.6.13) of modules in 0^ are still in 0^. In the sequel we will generally have a single characteristic set 5 in mind (this will he K ' in Section 6.8). The primary interest will be in the equiva­ lence classes of • For A e 5 its equivalence class A defines a subcategory which for simplicity we sometimes denote by 0^ (so ^ if A /a). The following is obvious: Proposition 1

Let 5 be a characteristic set, and let A e 5. Then (i) M(A), L(A) e (ii) every highest weight module with highest weight A is in 0^\ (iii) E ^ 0 x ^ 0^. Proposition 2

Let S be a characteristic set, and let S2 ^ S be subsets that are unions of equivalence classes. Suppose that 5^ Pi 52 = 0 . Then for E ^ 0^ , F ^ 0^^ we have (i) E n F = (0X (ii) H om g(£,F) = (0). Proof (0 Evidently [E n F : L(p)] > 0 => [E : L(fi)] > 0 and [F : L(p)] > 0. Hence fi ^ Si n S2, contradiction. (ii) If e Homg(E, F), then
206

Lie Algebras Admitting Triangular Decompositions

Proposition 3

Let S be a characteristic set, and let A and fx be in S. Suppose that E and F are highest weight modules in &(,%, o f highest weights A and fi, respectively. If A and ¡X are not equivalent, then E x t(F ,£ ) = (0).

Proof. Consider first the case F = M(fx). By Proposition 2.11.4, if Ext{M(.fx), E) ¥= (0), then \ > fx and there is a ^ e such that [M(A): L{v)] > 0 and [M{v): Lip,)] > 0. Thus Á ~ v ~ p , contradiction. Thus ExtiM ip), E) = (0). Now in the general case we have an exact sequence of g-modules 0

K ^

M (p) - ^ F ^ O

and hence an exact sequence (Proposition 1.12.4') H om g(/¡:,£) ^ E x t ( F , £ ) ^ Ext(M (jit),£ ) . But K is of type ¡X, and E is of type Á. Thus by Proposition 2, Homg(£, E) = (0). Since ExtiM ip), E) = (0) by what we have just proved, we obtain Ext(F, E) = (0). □ Corollary

Suppose that Á , p ^ S , are not equivalent. Assume E g F g are modules each of which has a finite highest weight series iSection 2.6). Then ExtiF, E) = (0). Proof. Let He ) and /(F) denote the lengths of the given HWS of E and F. If HE) + /(F) < 2, then the result is immediate from Proposition 3. In general we reason by induction on /(F ) + /(F). For example, if (0) c F i c

c £

= F

and n > 2, then from 0 ^ F „ _ i - ^ F ^ £ /£ „ _ ! - > 0 we have the exact sequence E x t(F ,F „_ i) ^ E x t(F ,F ) ^ E x t(F ,F /F „ _ i),

2.12

Decomposition of Modules in Category 0

207

and the outside terms are (0) by the induction hypothesis. Thus also Ext(F, = (0). The case for /(F) > 2 is similar. □ Theorem 4 Let S under

be a characteristic set, and let S denote its set o f equivalence classes . Let M be a %-module in 0^, Then M decomposes as a sum M=

where lies in

Furthermore is the unique maximal submodule o fM that In particular this decomposition o f M is unique.

Proof Let (0) = Mo c Ml c M2 c • • ‘ be a HWS for M (Proposition 2.6.10). Thus each nontrivial module M„/M„_i is a highest weight module, say, of highest weight A„, n = 1 ,2 ,... . We are going to construct for each equivalence class ft e 5 a module having a HWS (0) = M o o C M i o C such that ® M „n,

(1)

( 2)

i(0)

if e ft, if A„ ^ ft.

We will then have M = © ^ ^ required. We construct all the M„ ft g 5, at once by induction on n. For n = 1 we set Ml = Ml, Mi ^ = (0) if ft Ai. Suppose that n > 1 and by induction we have constructed M„_i ft G 5, satisfying (1) and (2) for n — 1. We have M„/M„_i ~\ . Thus ^ we define (3)

if ft ^ A„.

To define M„ (4)

we consider the exact sequence

0 ^ M„_i/M„_i,;^^

0.

208

Lie Algebras Admitting Triangular Decompositions

From the induction assumption

SO

Ext(M„/M„_i,

=

e

Ext(M „/M „_„

= (0)

by the Corollary to Proposition 3. Thus (4) splits, and hence there is a submodule E of such that

and

Define M„ ■= E. Since Af„_i ^ and £ G . We" check (1).

are in

, so also

M„ = £ + M„_, =£ +

® 0 n#A„

^ =£+

But

£

n 0 ^ ^ A „ ^ n , ii

= (0)

0 M„ n#A„ since £

M„ = £ ®

0

g

>

by(3).

Thus

M„_n= 0

Condition (2) is obvious. This completes the induction step. Define — U “ =iAf„ Clearly e and we have our required decomposition of M. As for the second part of the Theorem, let be the sum of all submodules K oi M such that K e Then e and z) M^, But ^ n ^ n ' "" (0) Proposition 2, and hence = M^, □

209

Exercises

EXERCISES 2.1 Let H be an abelian group and tt : H //. Let e Hom(//, K^). We define

G LiV) a representation of

= {u ^ M \7 r(h ){u ) = (f>{h)v for all h ^ H } . Show that is a submodule of V and prove the “group version’’ of Proposition 2.1. Describe also the “group version” of Example 1 of 2.1 for the group H = {A ^ SL(n, K)|>1} is diagonal. 2.2 (a)

Let (^ ,g + ,2 + ,< j)b e a triangular decomposition of g. Show that any subalgebra § of g satisfying ^ and c § also possesses a triangular decomposition. (b) Let g¿, i = 1 ,..., r, be Lie algebras with triangular decomposi­ tions ^ g^+, o}). Prove that the direct product gj X • • • X g^ of the Lie algebras g¿ also has a triangular decompo­ sition. (c) Let (]^, g+, (2+, a) be a triangular decomposition of g and let a be an ideal of g satisfying a n = (0), ga = a, g+
2.3 Let g = §I„(IK) be considered with the triangular decomposition of Example 3 of 2.1, and let M = IK" be the g-module with the weight space decomposition given in Example 1 of 2.1. Show by direct compu­ tation that these two gradings are compatible. 2.4 Classify (up to isomorphism) all three-dimensional Lie algebras admit­ ting a triangular decomposition. 2.5 [Be2] Let g be a Lie algebra with triangular decomposition (Q+j G+j 9 ^ 9 be any automorphism of order 2 such that i/f(g“) = g“" for all a e g . The objective of this exercise is to obtain some information about the Lie subalgebra § of all fixed points of í/í. Of course § = {jc + il/(x)\x G. g}. Let / : 0 -» Z be a group homomorphism satisfying f(a ) e Z+ for all a e 0+. Set 9" =

L

9“,

f ( a) = n

thereby obtaining a Z-grading on g for which g+= E„>o9", ft = 9^* Let {e^li e K}, where each e g"', n- e Z+, be a set of genera­ tors of g+ as a Lie algebra. Define == ^ i E: K.

210

Lie Algebras Admitting Triangular Decompositions

Also define the subspaces

and

n = - 1 ,0 ,1 ,... inductively

by 9-1 = (0),

9 o = 5,

9„=

E

9^

0<j : ^n

§_i = (0),

= [x + il/(x)\x e 1^} = i),

§„ = linear spcin of

and all products

... ,e,^],

where M; + • •• +n¡ < n . Evidently 9 = U "=_i9„, § => (a) Prove by induction on N that {x + tlf{x)\x G g^jm od §^_i and [«,V • • • ’ (b) Prove that § = U (c) Let

• • •’

= h v •••

^N-V

and that {e¡\i g K} generates §.

gr(§)+=«e= 1§„/§„_! be the graded Lie algebra associated with the filtration ^ c • • • of Prove that 9+— under the mapping x ^ x + il/(x)mod for all jc e g" , « = 1 ,2 ,... . 2.6 Show that every highest weight submodule of a Verma module is a Verma module. 2.7 Let (a ) and <6>, a, ft e N, denote the ^^(W-modules of dimensions a 1 and & + 1, respectively. Prove that (a ) ® (b ) - (a

b) ^ (a + b - 2)

e ••• e . 2.8 Let B c 5L2(IK) be defined as in Proposition 2.4.8. Let = {X^\X e B}. Prove that 5L2(IK) = B^B U J (Birkhoff decomposi­ tion) and that this union is disjoint.

Exercises

2.9

211

Let M be any finite-dimensional § l2(lK)-module admitting a weight space decomposition M = where M"* = {x e M\h • x = ¿zx}. Prove that for all a ^ Z, (a) dim = dim M “"*, (b) the sequence {dim is monotonically increasing until a = 0 and monotonically decreasing after 0.

2.10 Let Af(A) be a Verma modules of the category T). Show that for M(A) to be isomorphic to M(A)^, it is necessary and sufficient that M(A) be irreducible. The results of Exercises 2.11 and 2.12 are due to D.-N. Verma. 2.11 Let n be a finite dimensional Lie algebra graded by a free abelian group Q — Z^ whose degrees lie in —Q+= —(N^\(0}). Let ch U (n )=

n

(l-e (-a ))'

L K{
be the character of U(n) (see Proposition 2.5.3). (a) Prove that the coefficients K( 1 and any
tion Q+, (t ), and let M(A) be a Verma module for g. (a) Show that any two Verma submodules M ( / jl) and M ( p ) of M(A) must have a nontrivial intersection. (There is a counting argu­ ment using Exercise 2.11.) (b) Prove that M(A) is Noetherian (see Exercise 1.14). In the remaining exercises we will assume that every Verma module has a (finite) composition series. This is not in general true (see Exercise 2.13). However, it is true for split semisimple finite-dimensional Lie algebras (see Exercise 4.7). (c) Prove that every Verma module M(A) has a unique irreducible highest weight submodule M (v) (v depending on A) and that it is a submodule of every highest weight submodule of M(A). (d) Prove that for all A, /x e 1^*, dimHomu(g)(M(ju), M(A)) < 1. (Hint: Let M and M' be the image of two distinct embeddings of M ( ijl) in M(A). Then M(v) of (c) is in both. Write the generators of M(v), M, M' in terms of the generator í;+ of M(A), and use the fact that U(g_) is a domain.)

Lie Algebras Admitting Triangular Decompositions

212

2.13 Give an example of a triangular pair (g, (with dim g < oo) and a module M e ^ ( g , for which M does not admit a (finite) composi­ tion series. 2.14 Let be an abelian Lie algebra and V an l^-module admitting a weight space decomposition. Let V* be the dual space of V viewed as a ]^-module. (a) If / e for some A e ]^*, show that f(V ^ ) = (0) whenever JJL

(b)

(K^)* —(K*)"'^ as K-spaces for all A e 1^*.

2.15 Let M e <^(g, ^ ) . Let N+ and N_ be l^-modules admitting weight space decompositions: ©

N i ,

N _ =

©

N Z \

where all weight spaces are finite dimensional. Let if/: N _

be a vector space isomorphism satisfying {¡/(h • n) = —h • il/(n) for a\\ h phism

and n e N_. Show that there exists a unique monomor­

satisfying f{ m ® n) = f(>lf{n))(m ) for all / G Uom^(N+, M “^), n e N_, m ^ M. Moreover for all fi the above linear map composed with the isomorphism of Exercise 2.14(b) determines an isomorphism ~ :Hom(A^+,M‘^)'' s 2.16 [BM] Let Q = ®/=iZa, be a free abelian group. Set Q+'= (Ei=iNa,) \ {0}, and consider the power series ring Q[0T Q+\ which is the set of all formal sums e Q. Suppose that (s^, ^2,. - is a sequence (possibly finite) of distinct elements of Q+ arranged in order of increasing height, and suppose that for each 5^ there is associated a sign e(5,) = ± 1. For each sequence (n) = (n^, « 2?• •) of

Exercises

213

nonnegative integers, all but a finite number of the n, being 0 and for all A e (2+ U{0} define X(n) = 2 ( ( n ) ) = 2 « , ,

B {n) = B {(n )) -

(X n,)!

sgn(n) = sgn((«)) = r ie ( s ,) " ', S(A) =

{(n)|Xn,i,-

= A}.

For A, a e write X\a if a = rk for some r g Z+. In this case A /a := 1/r. Let m: ¡2+ ^ N, a be any function, and suppose that for some choice of s = ^2, . . . ) as above: n

( 1 - € ( « ) ) '" “ = 1 - £ £ ( 5 ,)e(s,). i

(This situation occurs for several types of graded Lie algebras n = ®n “, where = dim n “ (see Proposition 2.5.5 and the Corollary to Theo­ rem 6.4.1).) The objective is to give a closed formula for the integers m „.

(a) Let X := 1 - E,e(s,)e(s,). Show that e{ka ) -log X =

£

m,

a, k

(b) Apply the operator I E:= £ e ( a , ) i= l

d de{ai)

to obtain £(X )

(c)

= XC(A)e(A),

where C(A) — E„|AW„/ii(a). By computing -£ (X )/X in a different way, show that C(A) = X e(i,)/ii(5,)

£ ( n ) s 5 ( A - i ,)

sgn(n)B (n).

214

Lie Algebras Admitting Triangular Decompositions

(d)

Show that the right-hand side in (c) can be rewritten to give C (A )=Ä i(A )

E

sgn(n)



(«)e5(A )

(e)

Use Möbius inversion (see Bourbaki, Ch. 1-3, App. Ch. 2) to prove that

"ior

E Ala

2.17

^

(ri£i(i/) )

“ (n)e5(A )

pr

,

1 1 '^/-

(a)

Show that the homomorphic image of a residually nilpotent Lie algebra need not be residually nilpotent. (b) Show that the sum of a finite number residually nilpotent ideals of a Lie algebra is residually nilpotent. (c) Show that the sum of nilpotent ideals of a Lie algebra need not be residually nilpotent.

2.18 Let (g, be a Lie algebra with triangular decomposition. Show that g/rad(g) is radical free. 2.19 Prove that the Shapovolov form for §I2(1K) is given by ^ a( / ” *

*^+) =

n

k= l

(('^ + P )(^) “

for

n e N.

(See Section 2.8 Example 3). 2.20 Determine all the characteristic sets 5 c 1^* and their equivalence classes in the case of §I2(1K). 2.21 Prove that for the Lie algebra §I2(IK) the decomposition M =

® Mj,

Ae5 of Theorem 2.12.4 is a decomposition into eigenspaces of the Casimir operator. 2.22 Show that for t e C , a b one has M(a) ^ M(b) as ^12(C) modules if and only if i) e N and a = —b — 2. (See Section 2.4 for notation.) 2.23 Let I = ]^ 0 h be a Lie algebra consisting of an abelian subalgebra and an ideal b that decomposes as a l^-module under the adjoint representation into weight spaces b = where G +c 1^* is a free additive semigroup.

Exercises

215

Let t)' be a copy of b as a Lie algebra, and let o-: b b' be the anti-isomorphism between them that associates to each i; e b, the element - u , as seen in b'. We make b' an 1^-module by defining h • cr(v) = —o-[h, u], (a) Prove that f' == f) 0 b' has the structure of a Lie algebra compat­ ible with this action of on b'. (b) Let g := b' 0 0 b, and extend a to an endomorphism of g by defining (rli) = id ij,c7 ^ = l. Prove that g may be given the struc­ ture of a Lie algebra with subalgebras b and b' by defining [b,b'] = [b',b] = (0),

(c)

and show that (1^, b, ¡2+? is a triangular decomposition of 9. Let g be any Lie algebra with triangular decomposition 0), ^+,Q+,o-)- Set 5g = g_0 0 g+ as a vector space with multiplication defined as in g except that now [g+, g_] = (0) = [ 9 - , 9+ ].

Prove that ^g is a Lie algebra with triangular decomposition s ^ = (ij, Q+,Q+,(t ), We call sq the suspension of g. A Lie algebra g, with triangular decomposition is called suspended if [g+, g_] = 0. (d) Let (g, be a suspended Lie algebra. Prove that ^ t (Q) = i^ r(9 ) = n (g ) = rad(g) = g++ g_. (e)

Let (g, <5^) be a suspended Lie algebra, and let M(A) be a Verma module. Show that every subspace fx e A J, (2^., is a submodule of M(A). Show that all the irreducibles modules in <^(g, D are one dimensional.

2.24 Show that every derivation of the Vivasoro algebra is inner.

Chapter Three

Lattices and Finite Root Systems Symbols are to mathematics as wooden pieces are to chess —L. Wittgenstein

Any Lie algebra g with triangular decomposition У has associated with it a root system Д c 1^* so that g = There is no a priori reason to expect Д to have a particularly rich structure of its own. But, as Example 1.1.8 shows, it can happen. In fact Д is remarkably interesting for all the finite-dimensional semisimple Lie algebras over C. The root systems that arise from such semisimple Lie algebras are simply called finite (reduced) root systems. Over time it has been realized that finite root systems appear in other contexts that often have no apparent Lie theoretical connection. Thus there has developed an axiomatic approach to root systems (exemplified by Bourbaki [B03]), free from Lie algebras, which allows them to stand on their own. We adopt this approach here, prefacing it by a section on lattices and concluding with sections that show how to construct Lie algebras out of lattices, in certain cases. The investigation of root systems was begun at the end of the 19th century by W. Killing and E. Cartan in their study of complex semisimple Lie algebras g. Both realized that to each nonzero root there is an associated involution that stabilizes Д. Later on, influenced by the work of H. Weyl [Wy], the group W generated by all these involutions (now called the Weyl group) assumed a major role in understanding and describing the representa­ tion theory of g. These Weyl groups are finite groups generated by reflec­ tions (in euclidean space) and as such fall into H. S. M. Coxeter’s classifica­ tion of reflection groups [Cxi], A simplified version of the classification of simple and semisimple Lie algebras making use of root systems was achieved by B. L. van der Waerden [vdW]. 216

3.1

Lattices

217

3.7 LATTICES A geometric lattice is a pair (L ,( | *)) consisting of a free Z-module L of finite rank together with a symmetric bilinear form ( I ) : L X L ^ Z. Normally the bilinear form is understood from the context, and we simply speak of geometric lattices L. By assumption, L has a basis Cj,. . . , over Z: L = Z^i 0 • • • e Ze„. If we extend the scalars to IKby forming V - = K ^ i L and extend the bilinear form to a K-valued bilinear form on V in the only way possible, then V becomes a quadratic space by considering the quadratic form associated to ( I ) (see below). It is useful to be able to view a geometric lattice as a subgroup of a real or rational space (take IK = R or IK = Q above). The spaces R Q ®jL are called the realization and rationalization of L, respectively. Notice that L is a discrete subgroup of R The principal example of a geometric lattice is 0 • • • 0 Zs„

in R" = R^i 0 • • • 0 Re„,

where {e^,...,e„} is the standard orthonormal basis of R" as a euclidean space. This lattice is denoted by . The simplicity of this example belies the subtlety of the subject. Let L be a geometric lattice, and consider the mapping q:x of L into |Z . Then q is the quadratic form on L associated with ( I ). The quantity (x|jc) is called the norm or square norm of x. Of course (-I*) can be recovered from its quadratic form in the usual way: (jcly) = q { x + y ) - q(,x) - q{y) . The concept of isomorphism between geometric lattices is defined in the obvious way: We say that (L,(-10) and ( L ,(•!•)') are isomorphic if there is an isomorphism f : L - ^ L ' of groups such that (x|y) = (/(x )|/(y ))' for all x,y ^ L. If q and q' are the corresponding quadratic forms, then this last condition can be replaced by q(x) = q'(f(x)) for all x e L. The concept of automorphism of a geometric lattice is defined in the obvious fashion. If L is a geometric lattice, then its group of automorphisms is denoted by Aut(L). We list below a series of invariants for geometric lattices—that is, quanti­ ties attached to a lattice that depend only on its isomorphism class. 1. Rank, Two free Z-modules are isomorphic if and only if they have the same rank. In particular the rank, rank(L), of a geometric lattice L is an invariant. 2. Determinant. Let e = be a Z-basis of the geometric lat­ tice (L ,(1 )), and consider the n X n integral matrix = (B^ ), where

218

Lattices and Finite Root Systems

Bij '= If e' = {e\,. . . , is another basis for L and A is the matrix corresponding to the change of basis; e\ = Ae^ = then we have (< l< ) =

E a =l

E

Aue,

1=1 Ij

k,l

where A^ is the transpose of A. Thus B^,=A^B^A, Since det(y4) e Z and A has an integral inverse, det(^4) = ±1, from which d et(5 ,0 = d e t(B J. The common value of this determinant, which is independent of the choice of basis, is called the determinant of L and is denoted by det(L). It is an invariant of L. The bilinear form (*|*) is nondegenerate or nonsingular if and only if det(L) 0. In the case that det(L) 0, we say that L is nondegener­ ate or nonsingular. Otherwise, it is said to be singular. 3. Signature, Suppose that L is a nonsingular geometric lattice and that IK c R. Then by extending (•!•) to V •= we may apply Sylvester’s theorem (Jacobson [Ja2, Ch. 6] and write V as an orthogonal sum 1. V~ of a positive definite space and negative definite space V~. The dimensions and m " of these subspaces are invariants of (L,(*|*)) and are indepen­ dent of the choice of IK. Their difference sgn(L) = m'^ — m~ is called the signature of L. L is positive definite (resp. negative definite) if sgn(L) = rank(L) [resp. sgn(L) = -rank(L)]. It is indefinite if it is neither positive definite nor negative definite. 4. Type, We say that the geometric lattice L is even or of type II if the square norm of x is even for all x. Otherwise, L is said to be odd or of type I. If L is a free Z-module of rank n and L is a subgroup (Z-submodule) of L, then L is a free Z-module of rank n' < n, [Ja2, Ch. 3]. It follows that if L has a geometric structure (-I ), then L together with the restriction of ( I ) to L X L is itself a geometric lattice. We describe this situation by saying that L is a (geometric) sublattice of L, We say that L is a fiill sublattice of L in case rank(L') = rank(L). If L is a full sublattice of L, then the index [L : L] of L in L; that is, the number of cosets of L in L is finite. There is a simple way to compute this index: Let ..., be a Z-basis for L and / i , . . . , a Z-basis for L , Then the two bases are related by the relations matrix («¿y) defined through fj

52 ¿=1

j = l,,,,,n.

3.1

Lattices

219

It is a standard fact [Ja2, Ch. 3] that by suitably replacing the bases {«1, and { /,,...,/„ } , we can arrange to have a relations matrix (a'y), / / = E a'ije'i, ¿=1 where (a' ,) is of the form

d'y

and the d, e Z^. satisfy ¿¡\dj if i < j. Then L / L = Z /d ^ l e • • • ® Z/d„Z, and therefore [L : L'] = d, • • • d„ = det(a'y). Since det(a'y) = |det(a,y)|, (1)

[ L :L '] = |det(a,y)|.

The reader will observe that in obtaining (1) we use only the facts that L', L are free abelian groups of the same rank n and that L' c L. Now using the bilinear form, det(L') = dct{{f!\fj)) = det(d,(e;.|e;.)dy) = dl ■■■ dl det((e'|c})) = dl • • •

det(L ).

Thus (2)

det(L') = [L :L ']^ d e t(L ).

5. Dual lattices. Let L be a free Z-module of rank n. We denote by L° the dual module of L. By definition, L° is the Z-module of all homomorphisms of L into Z. Let e = [e^,. . . , be a basis of L, and define ef e L° for all 1 < i < n by (Cj, e f ) = Sij

for all 1 < j < n.

Clearly e* — { e f , . . e f } is a basis of L°, which shows that L° is free of the same rank as L. The basis e* is said to be dual to e. Suppose now that L is a geometric lattice. For each jc e L we define G L° by A:®(y) = (3:|y) for all y e L. The mapping x ^ of L into L°

220

Lattices and Finite Root Systems

is a homomorphism of modules and is injective if and only if L is nonsingu­ lar. If this is the case, we can identify L with a submodule of L°. Since L and L° have the same rank, [L®: L] is finite. This index is called the index of duality of L and can be computed as follows: By the definition of e* we have

y=i and hence from (1) [L»:L] = |det(L)|.

(3)

Especially important is the case |det(L)| = 1.

= L, which happens if and only if

A geometric lattice L is said to be unimodular if det(L) = ± 1. From the preceding remarks it is clear that Proposition 1 The following conditions are equivalent: (i) L is unimodular, (ii) L° = L {under the above identification). (iii) The mapping x •-> jc° is an isomorphism o f L onto V . Unimodular or not, the bilinear form ( I ) of a nonsingular geometric lattice L extends to a nonsingular bilinear form on the extension V = of L. One has a canonical identification of V and V* through x x®, where x°(y) = (x|y) just as before. Then L® can be identified with the following subgroup of V: = [v ^ V\{v\x) ^ Z f o r a ll x e L } . 6. Direct sums. If {L¿,{'\‘)¿), / = 1 ,..., r, are geometric lattices, then we may form a new geometric lattice by considering the Z-module L = © L, ¿=1 with symmetric bilinear form (• | ♦) defined by

¿= 1

E y, = E (^ily,), i=l I /=1

for all X,, y, e L,-.

3.1

Lattices

221

Evidently rank(L) = Erank(L,), sgn(L) = E sgn(L^), det(L) = ndet(L^), L is even if and only if each is even, L is positive definite if and only if each

is positive definite.

It is easy to identify L° with One identifies with the Z-valued linear functionals of L that vanish on Then the linear mapping x° of L L° takes into L® for each i. We have [L “ :L ] = n m - L , ] . ¿= 1 The lattice (L,(*|*)) thus obtained is called the orthogonal sum of the family (L^,(-I*)/), i = 1 ,..., r. To describe this situation, we write L = JL L,. /=1 Example 1 (Matrix representation of lattices) Let B = be any n X n symmetric integral matrix. Let L be a free Z-module with basis ..., and define (*1*) on L X L by {e^\ej) = B^j. This makes L into geometric lattice that is nonsingular if and only if det(5) # 0 and even if and only if B^^ is even for all i. The isomorphism problem amounts to determining when symmetric integral matrices B' and B are related by invertible integral matrices A so that B' = BA. This prob­ lem is far more difficult (and interesting) than first appears, and in one form or another has a long history in number theory. For more on the arithmetic and geometric properties of lattices see [Se2] and [CS]. Example 2 (Some unimodular type I lattices). Let m, e and consider with a standard basis the bilinear form defined by the matrix m

-1 -1

and

Lattices and Finite Root Systems

222

We denote the lattice together with this bilinear form by This is an odd geometric lattice of rank m + «, signature m - n, and determinant ( - D". For convenience we denote by and by I". It turns out that every indefinite odd unimodular geometric lattice is of the form ^ 0 If L is any geometric lattice and we let L q == {x e L\(x\x) = 0m od2}, then it is obvious that L q is a subgroup of L and that 2L — {2x\x e L} c Lq. Thus L q is an even full sublattice of L. If L is even, then of course L q = L. If, however, L is odd, then [L: L q] = 2, and detiLg) = 4det(L). To see this, let X q ^ L with (jcqIjco) odd. Then, if y e L with (y|y) odd, y - X q E: L q. So we see that L = L q \ J ( L q + X q). The value of det(Lo) follows immediately from (2). The simplest example of this procedure for constructing even lattices is the construction of the lattices. Example 3 (Lattices of type D/) Beginning with I/", we construct L := {x: 0 I/‘l(jc|jc) = 0mod2}. Here L is an even lattice of determinant 4. L is called the lattice of type Di. The terminology comes from Lie theory and E. Cartan’s classification of simple Lie groups and Lie algebras. In Section 3.7 we will construct the Lie algebra of type Di directly out of this lattice. If £ i,. . . , £/ is the standard orthonormal basis of I'l' and / > 2, then the / elements •“ ^/-1 form a basis of L. Each of these Z elements has norm 2. Norm 2 elements play an important part in the theory of lattices, particularly as they appear in relation to Lie theory. An element x = e l/" has norm 2 if and only if X is of the form ±e- ± Sj with i ¥=j . There are 2(/^ - /) of these elements. By definition they all lie in our lattice L. The matrix ((«¿1«^)) determined by the basis above is 2 -1

0 B =

-1

2 -1

-1

2

0 -1 -1

2 -1 0 0

-1 2 -1 -1

0 -1 2 0

-1 0 2)

3.1

Lattices

223

Finally, let L° be the dual of L. Recall that [L°: L] = |det(L)| = 4. Thus /L is isomorphic either to Z/4Z or to Z/2Z X Z/2Z. Let co = e Q Then (ajo)) e Z for all / so that o> e L°. If / is odd, it is clear that po) ^ L =>p = 0 (mod 4). Thus lP

^ 1

77"" 4Z

if / is odd.

On the other hand, if / is even, then lo) e L. It follows that if L °/L - Z/4Z, then there exists y e L° such that 2y = o) mod L. But this is impossible since ^ L°. Thus L °/L - Z/2Z X Z/2Z

if / is even.

Example 4 (Lattices of type Ai) Fix / e Z+, and form the lattice I/+i with the standard orthonormal basis £i,..., £/+i. Define //+1 L := I X; n,e,- E « i = 0 • L is a subgroup of

and it is easy to see that

defined by

a: := 6: - 6: form a basis of L as a Z-module. Thus L is a sublattice of rank /. The definition of L guarantees that L is even and, since it is a subgroup of it is positive definite and is called the lattice of type Ai. Relative to the basis «1, .. ., the matrix of L is

-1

-1 2

-1

B = -1

2 -1

Let z •=

+ *• •

^ I /+1? and define

-1 2

224

Lattices and Finite Root Systems

One checks by direct calculation that (cojay) =

from which we have

0 ••• 0 From the matrix of

one easily sees that

det(y4/) = 2det(y4/_i) - det(y4/_2),

with d et(^ i) = 2, d e t(^ 2^ = Thus [L°: L] = det(^/) = / + 1 and the in­ dex of duality of is / + 1. Since (o^ has order / + 1 modulo L, we have lV l

-

Example 5 (The hyperbolic plane) The simplest example of an indefinite even unimodular lattice is the so-called (by E. Artin) hyperbolic plane U, Here U = Ze^ Ф Ze2, and the matrix defining ( I ) is (?

:) ■

This lattice has rank 2, determinant - 1 , signature 0, and is even and indefinite. It is a useful building block in the classification of indefinite unimodular lattices [Se2]. Up to now we have not seen any examples of even unimodular positive definite lattices. In fact such objects must have rank divisible by 8 (not obvious). The next example gives a method for constructing one for each rank of the form Sk. Example 6 (The lattices Fix a positive integer k, and set n = Ak. Let L = subgroup of Q " with the standard inner product. Let 0 mod 2}, let v ^ Q”, and let r =

, and view this as a L

q

=

{x

e

L |( x lx ) =

:= ZV + L q.

From Example 3 we see that is a group halfway between the lattice D,Ak and its dual D®*. Let r ' be the subgroup of Q comprised of elements satisfying for all 1 < i, j < n. (4)

2?,- s Z,

(5)

Qi -

Qj

e Z,

n

( 6)

^ = 0 mod 2. ¿= 1

3.1

225

Lattices

We show that T = F : (r c F): Clearly y e F (since n = 4A:). Suppose now that x = E7=i«,e, ^ L. Then X e L q <=» T,nf = 0m od2 <=> = 0mod2. Thus L q = I E «¿e,; n, G ZiEn, = 0mod2 ki = 1

(7)

In particular L q c F , and hence F = l u + L q F'. (F c F): Suppose that x = ^ F', Qi e Q. If some e Z, then e Z for all i [because of (5)] and hence x ^ L q [because of (7) and (6)]. If no Qi e Z, then there exist integers ..., such that X = $21(1 + 2m^)Si = i; + [because of (4)]. On the other hand, because of (3.6) n

$2 i ( l + 2 '” /) = 2A: + $2'^/ = 0mod2. /=1 Hence

e L q by (7), and therefore x e F.

This finishes the proof that F = F'. Moreover it shows that every element of F is congruent either to 0 or to i; modulo L q, Thus [F: L q] = 2. Let us show that F is a geometric lattice. We have Ak {v\v) = — = f c e Z . 4 If X e L q, X = En^e^, n, e Z, then En, = 0mod2, and hence (ylx) = i E ^ i =\ Thus ( I ) takes integral values on F x F. Notice also that for x g L q we have {v -\r x\v + x ) = (¿;|i;)mod2 and hence F is even if and only if k is even, or equivalently, if and only if n = 0 mod 8. We know that F is positive definite (being included in Q ® /^). Finally, recall that [L: L q] = 2 = [F: L q]. Thus 1 = det(L) = 4det(Lo) = det(F). This proves Proposition 2 For each positive integer k the geometric lattice and unimodular.

is positive definite^ even^ □

226

Lattices and Finite Root Systems

Example 7 (The lattices Ei, I = 6 ,1 ,8,9,10) Let be the free Z-module of rank 10 with basis a_i, a^, ag. Consider the following diagram (this is a Coxeter-Dynkin diagram; see Section 3.4). 8

?

-o -o -o

-o -o

(

O - 0 - 0 - 0 ^lo) “ 1 0 1 2 3 4 5 6 7 We give £’io ^ geometric lattice structure by defining (-I*) E^q x E^10 Z as follows: For all - 1 < i, j < 8, (aja^) = (a,lay) = joined (ajay) =

2, - 1 if / ^ y and the /th and ;th node of the diagram above are by an edge, 0 otherwise.

We define geometric sublattices E¿, i = 6, 1, 8,9 of E^^ as follows: 8

£ 5 = 0 Za,-, ¿=3

8

^7 = 0 Za^, /=2

8

F^g = 0 Za^, i=\

8

£ 9 = 0 Za^. i =0

We could (and later will) attach to each of these four lattices a diagram that carries the information of the corresponding bilinear form. This is done by removing an appropriate number of nodes from the original £^0 diagram in the obvious way. We will later see that the lattices £g ,. . . , E^q are intimately related to Lie theory. Corresponding to each of E^, £ 7 , and £ g , there is an exceptional finite-dimensional simple Lie algebra. £9 corresponds to the affine KacMoody Lie algebra E\. The lattice £^0 corresponds to a hyperbolic KacMoody Lie algebra that is of much interest to physicists. We study these lattices in a number of steps ( - 1 . . . 3). [1] It is convenient to start with £g. Let . . . , eg be an orthonormal basis of I^, and define ..., ^ by Pi = ^i+i - ^/+2. ^ 7 = i ( £ l + eg) -

1 < / < 6, K «2 +

• • • +£7).

^8 = e? + eg. It is trivial to verify that usual inner product of Q

• Pj = (ajay) for all 1 < /,; < 8 (here • is the Ig), and hence £g = ©f^iZjS,. Using the j8/s,

3.1

Lattices

227

we are now going to show that ^8 —Tg (see the previous example for notation). It is clear that eZ/S^cTg. Conversely, suppose that x = (jCj,... , Xg) belongs to Fg. By using Pj if necessary, we can eliminate jCj. The resulting vector lies in L q [see (4)] and has = 0. By means of j8g we can assume that the sum of its coordinates Ef=2^/ = 0*We then have (0,X2, . . . , Jig) =X2(s2 - £3) + (^2 + ^3)(^3 - ^4) + • = X2)3i + (X2+X^)P2 + • • •

+ (^2 + **• +Xj){Sj + {x2

+ •••

+Xj)l3^

£g)

e eZ/3,-.

We conclude that is an even unimodular positive definite lattice. [0] To determine the structure of Eg, we consider the element a = qiq + 2ai + 3a2 + 4a 3 H- 50:4 + 6a^ + 4a^ + 2aj + 3ag. The coefficients of a have considerable significance as we will have reason to see later in Section 3.5. For now we note that they have the remarkable property that each n¿ is half the sum of the n/s for the nodes j that are adjacent to i in the diagram —for instance, «5 = 6 = |(5 + 4 + 3) = ^(«4 + «5 + n^). Writing this as 2n,. = (a ,|a ,> ,. = - 52 («,1«;)«; leads to

(a,la) =Ia,[52 j =0, i =0,...,8. In particular (a\a) = (Lw/aja) = 0, so a is isotropic. Since {a, a^} is a basis of Eg it follows that Eg is singular; that is, det(£9) = 0. We also observe that since E^ is positive definite. Eg is positive semidefinite. [-1 ] Consider the basis { - a _ i - a, a, a^,. . . , ag} of E^q. The matrix of Eiq with respect to this basis is given by 0

/M« 0 1

1 0

where M,g is the matrix for Eg Thus E jo = E^ ± U, where [/ is a hyperbolic plane and detCEjo) = det(£g)det(t/) = - 1 , showing that E^q is unimodular. E^q is even, and its signature is sgn(Eg) + sgn(t/) = 8. An example of an element of E^q of negative norm is given by a _ j + 2a. Summarizing, E^q is a rank 10 (indefi­ nite) even unimodular lattice of signature 8. [2] Ej, being a sublattice of Eg, is positive definite and even. To compute its determinant, we write a above in the form a = «0 +

228

Lattices and Finite Root Systems

Let L '= Z2aj 0 Z«2 0 * * * 0 Zag. Then {)3, «2» • • • ?^8^ ^ basis of L and [^gi L] = 2. Writing p = a - aQ immediately gives (a ,1)8) = 0, for 2 < / < 8, and ()S|)8) = 2. The matrix of L in this basis is therefore M,

o\ 0

y0

•••0

2/

where M7 is the matrix for E-^ and hence det(L) = 2 det(£7). On the other hand, det(L) = [£^gi L p det(jEg). Thus det(L) = 4, and therefore det(^7> = 2. [3] As above, is positive definite and even. Let )8 be as in [2] and write )3 = 2«! + )8'. Set L := Z3q'2 0 Zo:3 0 • • • 0 Zag. Then {)8', « 3, . . . , ag} is a basis of L', (a ,1)8') = 0 for 3 < i < 8, and ()8'|)8') = 6. Thus det(L') = 6 det(£g). On the other hand, [E^: L ] = 3 and det(L') = [E^: L Y so that det(L') = 18. Combining these two, we conclude that deti^^) = 3[4,5,6,7 ,8] The reader who is finding this game amusing may continue by removing nodes 3 ,4 ,5 ,6,7 in succession, obtaining lattices that might be called ^ 5, J&4, JE3, E2, El with determinants 4,5,6,4,2,. In fact it is easy to identify these with the lattices of type D5, .^4,^42 ± A i , A i ±A^, and A^, respectively. (These games, 24 in all, can be found in Exercise 3.6.) If L is a geometric lattice, we define for all n e Z, L(n )

: = { a e L | ( q :| q : ) =

n)

.

Proposition 3 Suppose that L is a definite geometric lattice. Then (i) each set L{n) is finite, (ii) Aut(L) is a finite group. Proof. Replacing (*| ) by - ( I*), if necessary, we may assume that (*1) is positive definite. Then L(n) = 0 if n < 0, so we consider L(n) for n > 0. There are two ways to see that L(n) is finite, each with its own merits 1. Let £ = be the realization of L. Then E is a euclidean space, L is a discrete subgroup of E ^ d for each n > 0, S{n) •= {x e E\(x\x) = /1} is a sphere of radius yfn . Since S(n) is compact and L is closed discrete, L(n) = S(n)C\ L is finite. 2. (*1*) extends to a positive definite bilinear form in V = Q Lti e = {ci,. . . , e^} be an orthogonal basis of V, and let ^ Q>o be such that (eje^) = q^. Each element of L can be written as a rational linear

3.2

Finite Root Systems

229

combination of the e/s. Since L is finitely generated, we conclude that there exists an integer N such that all elements of L can be written as integral linear combinations of e\ , e ', where e- — N for all 1 < i < m. Define

L

© Ze'. i= l

If x' = e L', then {x'\x') = N~^Lnjq^. Hence for each n e Z there exist only a finite number of x' e L' such that (x'\x') < n. Since L c L, we conclude that each of the sets L{n) is finite. To prove that Aut(L) is finite, let {ej,. . . , be a basis of L. Define e Z >0 by Qi '= and set 5 == U Then 5 is a finite set that generates L and is stable under Aut(L). Two automorphisms of L are equal if their actions on S coincide (because S spans L). But there are only finitely many ways in which Aut(L) can act on S (because S is finite). Thus Aut(L) is finite. □

3,2 FINITE ROOT SYSTEMS In this section we introduce the beautiful combinatorial objects called finite root systems. Historically these first appeared in the analysis of finite-dimen­ sional simple and semisimple Lie algebras. Since then they have been used also in the theory of lattices, the representation theory of associative alge­ bras, and the theory of singularities, just to mention a few instances. The simplest example of a finite root system is the set of norm 2 vectors of a positive definite geometric lattice L. Usually root systems appear in the theory of Lie algebras during the classification of split simple and semisimple Lie algebras. These algebras are decomposed into what amounts to a triangular decomposition, and the corresponding root systems are finite root systems in the special sense defined below. The classification problem reduces to classifying finite root systems. Our approach is the reverse. We begin by defining finite root systems, determining their basic properties in Sections 3.2 and 3.3, and using them to construct simple and semisimple Lie algebras in Section 3.7. The notion of a base for a finite root system, which is the main subject in Section 3.3, plays an important part in the theory. In the first place, bases allow us to classify finite root systems. Equally important for our purposes, they allow us to write down a canonical presentation for the corresponding Lie algebras, which in turn is the starting point for generalizing the finite-dimensional semisimple Lie

230

Lattices and Finite Root Systems

algebras to infinite-dimensional counterparts. The abstract theory of root systems was initiated by Witt [Wil]. We begin with a few generalities about reflections. Let L be a vector space over a field IK of characteristic 0. An endomorphism 5 of F is called a reflection (of K) if 1. = 1 and 5 ^ 1 , 2. s pointwise fixes a hyperplane (= subspace of codimension 1) H of V. If V is finite dimensional, it follows from this definition that the minimal polynomial of 5 is — 1 and that s admits - 1 as an eigenvalue of multiplicity 1 and 1 as an eigenvalue of multiplicity dim F - 1. In particular the minimal polynomial of s has no multiple roots, and all of its eigenvalues lie in IK. As a consequence 5 is a diagonalizable automorphism of F (see Section 7.1). Furthermore dct(s) = - 1 . If a e F is an eigenvector of s with eigenvalue - 1 (i.e., if sa = - a \ then V=Ka®H,

(1)

where H = {x ^ V\s(x) = x}. We call H the hyperplane of fixed points of s. Given an element a e F, a ¥= 0, we say that an endomorphism 5 of F is a reflection in a if 5 is a reflection of F and sa = —a. Notice that there are as many reflections in a as there are hyperplanes H of V supplementary to a [i.e., satisfying (1)]. In particular this number is infinite whenever dimtt,(F) > 1. Let 5 be a reflection in a, and decompose F as in (1). Let F* be the dual space of F, and let F X F* -> IK be the natural pairing. Define «V

^

by

(a, a ^ ) = 2, = ( 0),

and consider the endomorphism ( 2)

of F given by >

X - (x,a^)a.

Then it is evident that s = Conversely any decomposition (1) of F into a hyperplane H, and a one-dimensional supplement IKa gives rise to a reflection in a by using (2). Note When using this notation, it is inevitable that we have to make a choice whether to define (., .> from F X F* to IK or from F* X F to K. We have chosen the former, but later, when F is finite dimensional and we talk about reflections on F and F* at the same time, we will identify F** with V

3.2

231

Finite Root Systems

in the usual way and write reflection on V* in the form x* (a, x*)a^.

x* —

Proposition 1 Let V be finite dimensional, and let and S2 be reflections of V in the same a. If Si S2, then S1S2 is not a semisimple transformation o f V. Proof Let Hi and H 2 be the fixed point hyperplanes of tively, and set Í = Clearly

and ^2, respec­

1. det(0 = 1, 2. t pointwise fixes Ka 0 (//1 fl //2)If t is semisimple then t becomes diagonalizable by a suitable extension of the base field K (Section 7.1). It is clear then that conditions 1 and 2 imply that t = 1 and hence that Si = S2□ Proposition 2 Let ^ be a subset of V, and let Aut(A) be the group o f automorphisms of V stabilizing A. Suppose that A is finite and that A spans V. Then (i) Aut(A) is a finite group, (ii) For each a e A there exists at most one reflection s o f V in a such that s e Aut(A). Proof (i) If two automorphisms of V coincide on A, then they are identical (since A spans V). Thus Aut(A) is finite whenever A is. (ii) Let a e A, and suppose that Si and ^2 are distinct reflections in a that stabilize A. Then t = S1S2 ^ Aut(A) is an automorphism of V of finite order [by (i)] and hence semisimple by Maschke’s theorem [Ja2]. Now (ii) follows from our previous proposition. □ Suppose now that V carries a nondegenerate symmetric bilinear form ( 1 ) and that 5 is a reflection of F in a which is also an isometry of (*|*). Then, if we decompose F = Ka 0 / / as in (3.8), we have for all x e / / (a\x) = ( 5( a)U (x )) = ( - a l x ) , so (a|x) = 0. Thus Ka = H ^ , and we have (3)

V=Ka±H,

It follows that the restriction of ( I*) to both Ka and H is nondegenerate. In

232

Lattices and Finite Root Systems

particular (a\a) ¥= 0. Conversely, if a e F is nonisotropic, then the restric­ tion of ( I ) to / / := IKa-^ is nondegenerate and then the reflection in a given by the orthogonal decomposition (3) is an isometry. This is the unique isometry of V that is also a reflection in a. It is called the orthogonal reflection in a and is denoted by If one uses (• | •) above to identify V with F* (so that x e F < ^ ( | A : ) e F * ) , then it is clear that la (4)

(a|a)

In other words, (5)

s^(x) = x

2(x\a)a (ala)

Let F be a flnite dimensional vector space over a field K of characteristic 0. Assume that dimB^(F) > 1. A subset A of F is called a finite root system in F if the following conditions hold: RSI: A is finite, 0 ^ A, and A spans F. RS2: For each a e A there exists a '' e F* such that ( a , a ' ' ) = 2 and such that the reflection of F defined by ^ ^

-

(v,a-}a

stabilizes A. RS3: <j8, a " ) ^ Z for all a and p in A. The reflection whose existence is assumed in RS2 is necessarily unique (by part (ii) of Proposition 2). In particular a" is uniquely defined for each a, and this makes RS3 meaningful. In the sequel we will write instead of The dimension / of the space F spanned by A is called the rank of the root system. We refer to F as the ambient space of A and sometimes write (A, F ) to emphasize this. The elements of A are called roots. (This terminol­ ogy will be made clear when root systems are linked to Lie algebras.) For a e A,a'' is called the coroot associated with a. The set of coroots is denoted by A". The elements of GL(F) that stabilize A are called automorphisms of the root system A. The group of all these automorphisms is denoted by Aut(A). Axiom RSI together with part (i) of Proposition 2 imply that Aut(A) is a finite group. By assumption, if a e A, then e Aut(A). Thus {r^;|a e A} generates a subgroup W = IF(A) of Aut(A). This group is called the Weyl group of the root system A and is of fundamental importance in Lie theory.

3.2

Finite Root Systems

233

Since rj^a) = —a for all a e A, it follows that A = —A and that —1 e Aut(A). Whether or not - 1 is in depends on the root system (see the ^3,^3 Examples). Notice that if Aa e A for some A e (K^, then is a reflection in a stabilizing A. By the above observation In particular Ta ^ ' ' - a a e A. Let V and V' be IK spaces and A and A' root systems in V and V', respectively. We say that A and A are isomorphic if there exists a linear isomorphism F ^ F ' such that (A) = A. We write A = A to describe this situation. Note that if o- e Aut(A), then e Aut(A) and that the map or cr(f>~^ is a group isomorphism from Aut(A) onto Aut(A). More­ over, if a e A, then r^(f>~^ is a reflection of F ' in <^(a) stabilizing A, and therefore (6)

4>rA ‘ = r.
for all a e A.

This shows that under the above isomorphism IF(A) is mapped onto 1F(A). Proposition 3 Let is he a root system in F. Then IF(A) is a normal subgroup o f Aut(A). Proof If cr G Aut(A), then cr g GL(F), and we can view a as an isomor­ phism of A into itself. Our present result then follows from (6). □ As our first examples of root systems we have the following: Proposition 4 Let L be a positive definite geometric lattice o f rank I with rationalization F'. Suppose that the set L(2) of norm 2 vectors in L is nonempty and spans a subspace V of V'. Then L(2) is a finite root system in V and its reflections are the orthogonal reflections r^ o f V in the elements o f L(2). Proof By Proposition 3.1.3 L(2) is finite, and hence RSI holds. For each a e L(2) the orthogonal reflection r^ in a is 2(x\ a)a r ^ - . x - ^ x ----- , I , = (a|a)

- (jc|a)a.

Evidently r^ is an automorphism of L and hence stabilizes L(2); therefore RS2 holds. Identifying F* and F by ( 1 ) , we see from (4) that = a. Thus for G L(2), = (j8|a) ^ Z, and RS3 holds. □ Example 1 Figure 3.1 illustrates the root system A formed by the vectors L(2) of the lattice of type A^. The roots are the vectors from the centre 0 to the vertices of the cube-octahedron. The edges join vectors a, p

234

Lattices and Finite Root Systems

A, 0-0-0

B3 o — o = ^ o Figure 1.

for which a./3 = 1. The planes through which the reflections take place pass through the diagonals of opposite faces of the surrounding cube. The Weyl group is isomorphic to the symmetric group 54. In fact, if T denotes the set of four pairs of opposite triangular faces of the cube-octahedron then each of the six reflections generated by root pairs ± a acts as a distinct transposition on T, thereby giving all of the transpositions. If we adjoin to A the vectors from 0 to the centres of the square faces, we obtain another root system A' (later we will see it is of type B^) with 12 + 6 = 18 roots. The three reflections determined by these new roots evidently lie in Aut(A). However, their product is the mapping - 1 (central inversion), which acts trivially as a permutation on T and is not in W(A). On the other hand, the product tt of any two of them is a 180° rotation about the line L that is the intersection of their reflecting hyperplanes. The same line L is the intersection of two orthogonal reflecting hyperplanes of A so that tt e IF(A). Thus W{A) = {±1} X IT(A), [PT(A'):IT(A)] = 2. In fact we have W{A) = Aut(A') = Aut(A). The pair of graphs labelled

and ^3 are explained in Section 3.4. The

3.2

Finite Root Systems

235

reasons for changing the labelling of the roots in passing from -^3 to become clearer when we discuss bases in Section 3.3

will

Example 2 {Ai) (See Example 3.1.4) The set of roots L(2) is precisely the set of vectors of the form - Sj with i j, and the orthogonal reflection r in Si - Sj is the linear automorphism of V defined by

In other words, r is the linear automorphism defined by the transposition Si <-> Sj of the basis {e^,. . . , ei+J. It follows that W = 5^+^. Although we have defined root systems for spaces over arbitrary fields of characteristic 0, it is more convenient to develop the theory for spaces over the rational numbers Q. At the end of the next section we will see that it is easy to reduce the general situation to the rational case. However, until further notice, V denotes a rational vector space of dimension / and A c F a finite root system. Proposition 5 Let tx he a root system on V. Then there exists a positive definite symmetric bilinear form (*|*) on V that is invariant under Aut(A). I f V and F* are identified via such a form, then a" = 2a/ {a\ a) for all a e A. Proof Let (.,.) be any positive definite symmetric bilinear form on F. Define (•!•): F X F ^ Q by (^ly ) =

L

forall

e F.

o-e Aut(A)

It is clear that this form has the required properties. The statement concern­ ing a = 2a/{a\ a) now follows from (4). □ Proposition 6 Let ^ C.V be a root system. Then (0 A" is a root system in F*; (ii) PF(A) = W(A^) and Aut(A) = AutCA""), the isomorphisms being de­ fined by inverse transposition (see below); all a ^ A and A = ^ (under the canonical identifica­ (iii) q; = Qjv V tion o f V and F**). Proof Let (*1*) be a positive definite form on F that is invariant under Aut(A). Using (*|*) to identify F and F*, we have (as above) a" = 2a/(a\a). This shows that A" c F* satisfies RSI.

236

Lattices and Finite Root Systems

For each a e Aut(A) define
<£;,(r*(i;*)> =

for all y e F, r* e F*.

(
^ (y ),i3 '') = |(7 ‘(y)!

2(vla(/3)) (^1^)

2P

\

W )

I

2(v\o-(/3)) ( ( r(^ )k (/3 ))

= (v,{aiP)y}, and hence ( 8)

a*{p'^) = ( a { ^ ) y .

It follows that O'* stabilizes A"; in particular r* stabilizes A'" for each a e A. Now for i; e F and v* e F*, ( v , r : { v * ) ) = (r^(v), v*y = (v - ( v , a ^ } a , v * y = (u,v* - ( a , v * ) a - ) , which shows that r * : i;*

i;* - < a ,i;* > a''.

Thus r* is a reflection in a" and = a (see the note on pairings in the previous section). This proves RS2 and part (iii). Finally, for all a ' ' , ^ A'",

which proves RS3. The mapping o- >-> o-* is evidently a homomorphism of Aut(A) into Aut(A") [resp. W(A) into W(A" )]. It is seen to be injective from o-** = a and surjective by reversing the roles of A and A". □ The root system A" is called the root system dual to A. One should be aware that the mapping A ^ A" defined by a a '' is not the restriction of a linear map in general. In fact it is obtained by inversion with respect to a suitable (/ - l)-sphere.

3.2

Finite Root Systems

237

Example 3 The root systems dual to ^3 and are illus­ trated in Figure 3.1. Notice that for a e A(y43), a" = 2a/ ( a\ a) = a, whereas for a e A(^3) \ a" = 2a/ (a\ a) = 2a. The root system AiB^Y is of type C3. We leave it as an exercise to verify that AiB^) and A(^3)" are not isomorphic. The reader may wonder about the role of ( •| •), which seems to be quite arbitrary and yet quite significant. In fact it is essentially unique. We leave the precise sense of the uniqueness to Propositions 3.4.7 and 3.4.8. Some indication of this already appears in the following discussion. Let (*|*) be a symmetric bilinear form on V as constructed in Proposition 5. Then

(9)

2iß\a) ( a la )

for a,/3 e A.

Recall, on the other hand, that in the euclidean space U between a and is given by the expression

cos(6) =

the angle 6

(i3|a) [(a |a )(/3 lj8 )]

1/2

Hence ( 10 )

( ß , a ^ ) ( a , ß" ) = 4cos^(ö).

The left-hand side of (10) is the product of two integers, whereas the right-hand side is in absolute value < 4. Thus the possible values of 6 are severely restricted. We collect below all information that follows from the above. There are two main cases to consider: Case 1. a and ß are proportional. Suppose that ß = Aa, A e Q. Since both ( ß , a " ) and ( a , ß " ) are integers, it follows from (9) that both 2 A and 2A“ ^ are integers. We conclude that A e {± ± 1, ± 2}. These are the only possible multiples of a root. [In the sequel we will say that a root a g A is indivisible if ^ A. If a root system consists only of indivisible roots we will say that it is reduced. Otherwise, we say that it is nonreduced. We denote the set of reduced roots of A by Case 2. a and ß not proportional. The only possible solutions of (10) (up to interchanging a and ß) are given by Table 3.1.

238

Lattices and Finite Root Systems

Table 3.1

0

0

1

1

1

2 3

1 -1

-1

-1

-2 -3

-1

0 IT/ 2 7t/3 7t/4 ir/b 27t/3 3-77/4 57t/6

(a|a)/(j8li3) Undefined 1

2 3 1

2 3

Order of 2 3 4 6 3 4 6

We determine the order of as follows: Both act on the and space = Qa © Qp, and on this space the transformation has the prescribed order. There are two simple ways, one geometric and one alge­ braic, to see this. Embedding ^ into real 2-space U one can use the fact that the product of two reflections is the rotation through twice the angle between their reflecting hyperplanes. A completely algebraic way is to observe that the matrix for relative to the basis [a, of ^ is

\

-1

)

and its characteristic polynomial + (2 - 4cos^0)A + 1 has roots Now let and be the hyperplanes of V consisting of fixed points of and respectively. Let V' = Then L = K' ® Since acts like the identity on K', it has the prescribed order as a transformation on V, The rest of the information contained in the table is clear. Here are a few more facts about root systems. Proposition 7

is a reduced root system. Proposition 8

Let a, p ^ A be nonproportional roots. I f (a|j8) > 0, then a — p is a root. If (a\p) ^ Oj theft ot “1“ ^ is Cl foot. Proof. If (a|)3) > 0, then <j8, a '' > > 0 and > 0. Since their product is less than 4, at least one of these two quantities equals 1. If a = )3 - a e A, and hence a - /3 e A. If = 1, then r^a = a - ¡3 ^ A. The second assertion follows from the first by replacing )3 by —/3. □

3.3

Bases for Finite Root Systems

239

Let i= , r, be K spaces, and for each i let be a root system in Let V = and identify each L; with a subspace of V. Each can then be thought as a subset of V. We let A == U [=iA^. Let us show that A is a root system in V. It is clear that A spans V. Let a e A^ c L; c V, and let a" e K* be defined by means of the canonical identification F* = Then is a reflection on V stabilizing A (it acts like in Vi and like the identity on Vj, j i). Also = (0), and (A^,a ") (z I . Thus RS2 and RS3 hold for A. We denote the reflection in a by both for a e A^ and for a e A. The root system A in F constructed above is called the direct sum of the root systems A^. To describe this situation, we write A = Ai V

V A.

Let W d e ^ te the Weyl group of A and WK the Weyl group of A^. The subgroup of W generated by the r^, a e A^, is evidently isomorphic to (the restriction map w ^ w\y. being the isomorphism). S i n c e a n d commute if a g A^, j8 e Ay with i ^ j \ we conclude tjiat W = W j X • • • X Wj , - Wi X • • • XW^. There is no harm in identifying and and we do so freely in the sequel. A root system A is called decomposable if there are root systems Aj, A2 such that A = Ai V A2. Otherwise, A is called indecomposable. Any root system can be decomposed uniquely into indecomposable root systems (see Section 3.3). Proposition 9 A root system is decomposable if and only if there exist nonempty subsets A^, A2 of A such that (i) A = Ai UA 2, (ii) (aljS) = 0 for all a e A^ and j8 e A2. Proof (=>) The proof is clear from the definition. («=) Let Fi and F2 be the span of A^ and A2, respectively. It is trivial to verify that Aj and A2 are root systems in F^ and F2, respectively, and that ASA1VA2. □ 3.3 BASES FOR FINITE ROOT SYSTEMS Let A be a finite root system with ambient space F. It is evident that we can choose a basis of F from A. However, it is possible to do this in a very special way that naturally divides A into positive and negative subsets A+

Lattices and Finite Root Systems

240

and A_ with A_= -A+. The key result (Proposition 5) is that any two of these special bases are translates of each other by the Weyl group W. Thus the structure of a base is an invariant of W. This leads immediately to the definition of the Cartan matruc of a finite root system and the introduction of the Coxeter-Dynkin diagrams. Let A be a root system in a I -space V. A subset n = [a^,. . . , a:/} is a base for A if Bl: n is a basis for K as a vector space, B2: every root can be expressed (necessarily uniquely) as an integral linear combination of the a^, where all the coefficients are either nonnegative or all are nonpositive (loosely, all the coefficients have the same sign). We now return to the case K = Q. Throughout this section (-I*) denotes an Aut(A)-invariant positive definite symmetric bilinear form on V (see Proposition 3.2.5). Proposition 1 Every finite root system has a base. Proof We start by putting a total ordering > on the rational space V that makes V into a totally ordered vector space. By definition this means that > is a partial ordering on V and that 1. for all v,w ^ V either u > w,w > v, or w = u, the possibilities being mutually exclusive; 2. if V > w and X e F, then v + x > w + x; 3. if V > w and c G Q+, then cu > cw. For instance, if we choose a basis . . . , Ui), we may define the lexico­ graphical ordering by declaring that for two unequal elements, 'La¿v¿ > Lb^Vi if and only if at the smallest i for which a^ b^ we have a, >b, . ^ In any case let V+= {z; e V\v > 0} so that V = U{0}U V- (U denotes disjoint union). Let A+:=Ari]^+ and A_— Afll^-. A root a e A+ is called simple if a cannot be written as ¡ 3 y, where j8, y e A + . Let n = {«1, . . . , a^} c A+ be the set of simple roots. We reason in steps: 1. I f a, P ^ Yl, a ¥=p, then (a|j8) < 0 and (a, ) < 0: We have ex­ cluded the possibility that a and jS are proportional since then, say, P = 2a = a a and p is not simple. If (a\p) > 0, then a — p and p - a dire roots (Proposition 3.2.8). One of these, say, p - a, belongs to A+, and then p = (p — a) a shows that p is not simple.

33

Bases for Finite Root Systems

241

2. The elements o f O are linearly independent : Suppose that = 0, where not all the c, are 0. Let / ‘^= {i|c, > 0} and / “ = {i\c^ < 0}. Then both and I~ are proper subsets of k} (otherwise, 0 would belong to either or V~). Let x = Then x ^ 0, and X= c^a^. Thus 0 < (x|x) = ^ step 1, which is a contradiction. 3. Yl is a base o f A: If y e A+ is not simple, then y = a + )3, where a, p ^ A^. Then y —a = )3 > 0, so y > a, and similarly y > p. It follows by induction on > that every element of A^. is a sum of simple roots. Since A_= —A+, B2 holds; and since A spans F, O is a basis of V, □ Example 1 Let L be a positive definite geometric lattice for which L(2) 0. Consider the root system L(2) (Proposition 3.2.4). Suppose that 11 c L(2) has the properties 1. The Z-span of Yl contains L(2); 2. (a|j8) < 0 for all a, P ^ Yl, a Then n is a base of L(2). For suppose that y e L(2), y = E ^ e n '^ a ^ ’ e Z. If the are of mixed signs, we may write y = y++ y_, where y+— y_:= y - y+. Then (y|y) = (y+|y+) + 2(y+|y_) + (y_ly_). Since (y J y +) e 2Z+ and the assumption (2) gives (y+|y_) > 0, we have (y|y) > 4, which is impossible. The elements of II are linearly independent by the argument of step 2 of the last proposition and span the same rational space as L(2). Referring back to Section 3.1, this shows that the a-bases given there for the lattices L of types Ai, j g are actually bases for the corresponding root systems L(2). Proposition 2 Let ^ d V be a root system, and let S cz A be any nonempty subset. Let V' be the subspace of V spanned by the elements of S, and set A = A fl F'. Then (i) A is a root system in F', (ii) any base of A can be extended to a base o f A. Proof If a e A, then a" can naturally be viewed as an element of F'* by restriction. Then for all a, e A, r , ) 8 = ) 8 - < ) 8 , a - > a e A n F ' = A,

and it is clear then that A is a root system in F'.

242

Lattices and Finite Root Systems

Now let {«1, . . . , be a base of A', and consider a basis for V of the form {v^, q:^}. Then the base of A obtained from the lexicographic ordering of V determined by this basis contains « i , . . . , □ A subset 2 of a root system A is called a positive system of roots if S = A n 1^+ for V+'-= {v ^ V\v > 0}, where > is some total ordering on V. We have seen that the simple roots of a positive system of roots 2 form a base n in X. In fact FI is the only base of A lying in X. To see this, we introduce the height function ht := h t^ : A

(11) by

htl £ m „a\ =

E aen

Notice that /3 e A is in if and only if ht(jS) > 0. Let O ' be another base of A inside X. Then ht(a') > 1 for all a' e O'. Each a e O is expressible as a = where the m^, e Z are all of the same sign. In fact the m^> e N for otherwise a e A_. Now 1 = ht(a) = Xm^.ht(o:') =>« = «' for some a' e O'. Thus O c O ' and, in view of card(n) = dim(F) = card(n'), we have Yl = O'. Every base Yl can be used to determine a lexicographical ordering of V and then a positive system in which it lies as the simple roots. We call A+= A+(n) the system of positive roots corresponding to O. Clearly A ,(n) =

e A

/3=

E

rn^a,m ^

>

o}.

Summarizing, we obtain Proposition 3. Proposition 3 (i)

Every positive system o f roots contains exactly one base. This estab­ lishes a 1-1 correspondence between positive systems o f roots and bases. (ii) The elements of any base are indivisible. (iii) I f {«1, is a base, then (a^, aj" > < 0 for all i ¥=j. □ Proposition 4 Let Y\ be a base o f A. Then (i) { r j a G n} generates W as a group-, (ii) A^^^ = WY\ == {wa\w ^ W , a ^ O}.

3.3

Bases for Finite Root Systems

243

Proof, Let n = {aj,. . . , aj}. Let Wq be the subgroup of W generated by Tj,..., A*/ (for convenience, we denote by r^). We begin by proving ( 12 )

= W ^n.

We use induction on the height function ht = htp^ relative to Yl to prove that := A^®^ n A+c W^Yl, Let /3 e If ht(iS) = 1, then j3 e n . Suppose that ht(j8) > 1. If (jSla,) < 0 for all i, then writing )3 = e N, we have 0 < ( ^ 1^ ) = Lnii{l3\ai) < 0,

which is impossible. Thus (p\ a , ) > 0 for some i. Then (13) r,.(/3) = 13 - {p, a,'' >a, = Y,

+ (m, - )a, e A"®'*.

j * i

If rrij = 0 for all i i then ^ = m,a,. Since /3 is indivisible, /3 = a„ contrary to ht(/3) > 1. Thus some Wy ¥= 0, and hence nij > 0. It follows that r,(/3) e A+'’. Since = 2()3|a,)/(o:,|Q:,) > 0, ht(r,(/3)) < ht(/3), and we may assume by induction that /-¿(jS) e WqTI. Write r,(^) = for some w'^ in Wq. Then /3 = WqU^. with Wq = /-¿Wq e Wq. In addition by (6), -1 The conclusion of all this is that c IFoIl and that e Wq for all j3 G A™**. Since whenever /3 and Aj8 e A, we see that g for all -y G A. Thus Wq = IT, proving part (i). Finally, r,(a,) = —a,-, showing that - n c ITon, so IT o n -----ITon and A^f“ = -A'®“ c W q U . This proves that ^r®d (- ]YqTI. The reverse inclusion is obvious. This finishes part (ii). □ If n is a base for A+ and a e O, then Q a fl A+ is one of {a} or {a, 2a}. In either case we have the following simple facts:

(14)

1. stabilizes A + \(Q a fl A+) 2. r ,A ^ = - ( Q a n A ^ ) U ( A A ( Q a n A ^ ) .

The point is that for any root )3, /3 and rj^p) differ only by a multiple of a. It follows that if )8 e A+ and j8 ^ Q a f l A+, then the expression for in terms of elements of II still contains nontrivial (hence positive) contributions from elements 7 ^ n \ { a } [see (13)]. Thus r^(j3) e A +\ Q a fl A+ also. Simple as these remarks are, they play an important role in understanding the structure of W (see Chapter 5).

244

Lattices and Finite Root Systems

We have the following key result: Propositions. (Conjugacy o f bases) Let (A, V) be a root system. (i) I f li is a base o f A and w then iv(n) is also a base. (ii) Any two bases o f A are related in this way. Proof (i) The proof is obvious. To prove part (ii), let and II2 be two bases of A with corresponding positive systems A+ and A+. Let A_ := -A+ for / = 1,2. It suffices to prove that there is w ^ W with w A \ = A+ (see Proposition 3). If A + n A^_ = 0 , then A+ c A+, whereupon they are equal and hence III = Il2 by (i) of Proposition 3. Suppose that card(A+ n A^_) = n > 0. Then III ^ ^ since, otherwise, 111 c A+ and Hi = II2. Choose a e III n A^_, and consider r^A \. It differs from A+ only in that —a (and possibly —2a) replaces a (and 2a). But a e A^_, so - a e A+. Thus card(r^A^^ n A^_) < n. Since r^A \ is the system of positive roots for r^IIi, we are done by induction on card(A+ n A^_). □ This proposition says that the Weyl group is transitive on the set of bases of A. In fact it is simply transitive on the set of bases; we prove this in Chapter 5. Proposition 6 Let tsbe a reduced root system in V and let A'' c F* be its dual root system. Let Yl be a subset of A. For U to be a base o f A, it is necessary and sufficient that ••= [a"\a ^ A) be a base o f A". Moreover, if A^ and A \ denote the positive systems o f roots defined by II and II'', respectively, then a e A+ if and only if ^ A+. In other words, {A ^Y = A+. Proof Let identify V and F* via (• ). Fix an ordered basis of F*, and use its lexicographic order to define a system of positive roots A+ and a base n '' := {aj',. . . , a I } of A ''. The above choice of ordered basis of F* = F defines a positive system of roots A+ of A. Since = 2 a / ( a , a), we conclude that for all a e A, (15)

a e A+<=> a '' e A \.

We claim that II — {ai, .. .,ajf is a base of A. Since II c A+, we must show that a^ = p + y, with and 7 in A+, is not possible. Now if a^ = + 7

33

Bases for Finite Root Systems

245

with P and y in A+, then = ''a,«/ = SOthat either r^,p e A_ or r^y e A_. Assume that y is similar). Then {r^ p Y e A l, and hence by (8)

= r%p^ =

e A_ (the case of

^ a: .

By (14) (applied to A" and the base II"), it follows that P" = a ," , whence P= Then y = 0, which is absurd. This shows that II is a base of A. The rest of the proof is easy. □ Up to now most of our results have been proved about root systems under the restriction IK = Q. In what follows we show how the general situation is dealt with. Let F be a vector space over a field IK of characteristic 0. By restriction of the base field to Q c IK, we can think of F as a rational space, which we denote by F(Q). Notice that dimQ(F(Q)) = dim„^(F)dimQ(IK). A (rational) subspace U of F(Q) is called a rational form or a rational structure of F if the canonical K-linear mapping K 0Q i/

F

is an isomorphism. (This map is the unique linear map satisfying k ^ u ^ ku for all A: e IK and m e i/). Equivalently C/ is a rational form of F if 1/ has a (rational) basis that is also a basis for the K-space F. In any case notice that dimQ(i/) = dim„^(F). Example 2 Let

^ ^ be a basis of F over IK. Then i / :=

© QU^

AeA

is a rational form of F. Next we show how the concept of rational form allows us to understand the relationship between root systems (A, F ) for IK-spaces and rational root systems. Proposition 7 Let (A, V) be a finite root system where the ambient space Vis a K-space. Then the rational span Vq o f L in V is a rational form o f F, and (A, Fq) is a finite root system. Furthermore for each a ^ ^ the reflection r^ o f (A, Vq ) is the

246

Lattices and Finite Root Systems

restriction to Vq o f the corresponding reflection o f (A, F), and the coroot Vq is the restriction to Vq of the corresponding coroot of

of

Proof Let Vq be the rational span of A in V. Let a e A. Clearly a" (F q) c Q and hence a" induces an element also denoted by a " , of Fq . It is now easy to see that (A, Vq ) is a root system. It remains to show that Vq is a rational form of F. Let II = {a^, be a base of (A, Vq ), hence a Q-basis of Vq . Then II spans F (over K) since A does. Suppose, if possible, that Y, CiUi = 0, /=1

c,- e K,

where some c^ ¥= 0. Then for each jS e II, Ec, = 0, ¿=1 which shows that the matrix A = « a ,, a p ) defined by II is singular (where A is viewed as a matrix with coefficients in IK). However, we know that A is nonsingular when viewed as a matrix with coefficients in Q. Since nonsingu­ larity remains unchanged by extension of the base field, we conclude that the elements of II are linearly independent over IK and hence that II is a IK-basis of F as desired. □ Remark 1 The above proposition makes it clear that all our results about the structure of rational root systems generalize to arbitrary root systems. For example, any base of (A, Fq) is a base of (A, F ) (showing the existence of bases). Similarly any base of (A, F ) is a base of (A, F q ) , and hence any two such bases are conjugate under W. Let n = {«1, . . . , O'/} be a base of A. The Cartan matrix of A (with respect to n ) is the / X / integral matrk A = where Aij ■■= = («yl“ /) ’ Interchanging the ordering of and changes A by simultaneous inter­ change of rows i and j and columns i and j. Combining this with the IF-conjugacy of bases, we see that A is uniquely determined by A up to simultaneous row/column permutations.

3.4

Graphs and Coxeter-Dynkin Diagrams

247

We note the following properties of A: CMl CM2 CM3 CM4

A¡¿ = 2 for all i. Aij G - N if / ¥=j.

There is a positive diagonal matrix D (D = diagidj,. . . , d j, > 0) such that AD is symmetric. CMS: AD in CM4 is positive definite. For CM4 and CM5 simply observe that A diag

, (“ ii«i)

(«/I«/)

= ((a,l«y)).

In Section 3.4 we use CM1-CM3 as the definition of a “generalized” Cartan matrix. We will also see that CMl-CMS characterize the Cartan matrices of finite root systems. Notice that CMS implies that A is nonsingular.

3.4

GRAPHS AND COXETER-DYNKIN DIAGRAMS

We have many occasions to use square matrices of integers in the sequel, notably matrices like the matrices A satisfying the conditions of CM in Section 3.3. Representing these by graphs is an extremely economical and useful idea. In this brief section we show how we wish to attach a graph to a matrix and review the basic definitions and facts about graphs that we will need. There are no proofs in this section. The reader may refer to [Bg] or provide them as an (easy) exercise. Let N* = U {oo}. Let J be a nonempty set. A matrix M = is said to be combinatorially symmetric if for all i and j in J, CSl: Mij G N*, CS2: CS3: M,, = 0. Example 1 Let F be a IK-space, and let ^ family of automor­ phisms of V, For all i and j in J, define M^j as follows: ^

I order of s^Sj

if s^Sj is of finite order, otherwise,

M,- = 0. Then M =

is combinatorially symmetric.

if i ^ ;,

248

Lattices and Finite Root Systems

Let M = be a combinatorially symmetric matrix. We may represent M by a labeled graph T = (V,E,M) with vertices (or nodes) V = {vj\j ^ J] and directed edges (or arrows) E = e J X J, i ¥=j, M^j 0}, which are assumed to be marked by the quantities (M^y). Note that if M^j = 0, then there is no edge e¿J. By definition, then also will be missing. M is called the incidence matrix of F. We often think of as being M^j arrows from i to j [or of type (i, j)] and refer to them as such. Example 2

(0 M= 2 lo r;

2 0 0 00 1 0 o V2 0

J = {1,2,3} ^

0 .

There are several simplifying conventions that we will use for our graphs: 1. If M,y = 1 and Mji > 1, we omit the edge e,y. 2. If Mij = Mji # 0, we replace the edges and eJ¿ by a single undi­ rected edge labeled by their common value. 3. If M,, is small (< 4 usually), then we may elect to replace a labeled edge by a corresponding multiple edge. We also use this convention in 2. 2

Example 3 0 ^ 0

becomes O

by convention 3. O ^

2

O by convention 1, and then O => 0

O becomes 0 — 0 by convention 2, and then

O — O by convention 3. M of Example 2 now appears as

0 = 0 ^ o. Example 4

0—

0 1

0

o

3.4

Graphs and Coxeter-Dynkin Diagrams

249

corresponds to fo 1 0 io

1 0 3 1

0 1 0 0

o' 1 0 oj

In the sequel all graphs are assumed to be reduced by these conventions. We assume that the reader is familiar with the standard notions of graph theory. For definiteness we repeat the definitions that we will adopt for this book together with a few well-known facts. Let r = (V, E, M), F = (K', M'), where M and M' are indexed by J and J', respectively. 1. r and F' are isomorphic if there exists a bijection a: J ^ J' so that ^a(i),«(;) = ^ i j for all (j, y) e J X J. From this we obtain the concept of an automorphism of F. 2. F is a subgraph of F' if there is an injection a: J J' so that K(0,a(;) = for all i , j e J. 3. F is disconnected if J is the disjoint union of two nonempty sets Jj and J2 so that = 0= for all Jz) ^ Ji X Jz4. If F is not disconnected it is connected. 5. A path (of length n) in F is a sequence (/ q, ^1, • • •, of elements of J so that for each k = ¥= 0. The path is said to connect V: ^0 to V ih 6. F is pathwise connected if every two vertices are connected by some path. 7. Pathwise connected and connected are equivalent. 8. A cycle or loop in a graph is a path (/ q, ¿1, . . . , of length n > 3 for which ¿Q, are all distinct and 9. A forest is a graph with no cycles. A tree is a connected forest. 10. Two vertices (or nodes) are adjacent if there is an edge between them. 11. The valence of a vertex is the number (possibly infinite) of vertices adjacent to it. 12. Any finite tree with more than one vertex has at least two vertices of valence 1. 13. A connected graph F is bipartite if J can be partitioned into two nonempty subsets Ji and J2 so that M^j = 0 whenever /, j e or 14. Any finite tree with at least two nodes is bipartite.

250

Lattices and Finite Root Systems

Let J be a nonempty set, and let A = be a matrix with integer coefficients. We say that ^ is a Cartan matrix (some people call it a generalized Cartan matrix) if CMl: CM2: CM3:

A,.= 2 for all / g A¿j< 0 for all i ¥= A¿j= 0 <=>Aj¿ = 0

J, j in J, for all i

^ j E:

J.

Example 5 Let II = {a^,. . . , a j be a base of a finite root system A. Define A¿j for all 1 < i, j < I by A¡j = . Then ^ is a Cartan matrix. Let A he a Cartan matrix. Then M = 2I-A (where / is the J X J identity matrix) is a combinatorially symmetric matrix and defines a graph r = r(A) ^ (V,E,M). r is called the Coxeter-Dynkin diagram of A. Example 6

A =

2 -1 0 0 l:

-1 2 -1 0

0 -2 2 -1

O' 0 -1 2.

O — o =?• O — O

Example 7 Consider the finite root systems L(2) of types D,, Ai, E^, E^, Eg. (Example 3.3.1). Referring back to Section 3.1, we see the Cartan matrices of D, and A i displayed. The corresponding Coxeter-Dynkin diagrams are T{Ai):

0 -0 -

------0 - 0 O

r(A ):

0 —0 —

—0 —0 ^ O

For the E series we have already used graphs to define the matrices. The

3.4

Graphs and Coxeter-Dynkin Diagrams

251

Coxeter-Dynkin diagrams are 0 1 0 —0 —0 —0 —0

^ £ 7 ):

r(£ 8 ) :

0 1 0 —0 —0 —0 —0 —0 0 1 0 —0 —0 —0 —0 —0 - 0

The Cartan matrix A is indecomposable if T (^ ) is connected, and it is decomposable otherwise. To say A is decomposable is equivalent to saying that A can be reindexed (by simultaneous row/column permutation) so that it assumes the form 0 0

^2

where A^ and A 2 are (necessarily) Cartan matrices. A Cartan matrix A = i.Aij)i is symmetrizable if there exist nonzero rational numbers e„ i e J, so that for all i , j e J or equivalently e,- '-<4,7 = ej

for all i , j e J.

This concept is of considerable importance in the sequel so it is good to have an easy way to recognize a symmetrizable matrix. Proposition 1 The Cartan matrix A is symmetrizable if for each cycle (/ q, • • •, A:

i = A: :

in r(>l),

A: : .

Since \Aij\ = is the number of arrows (edges) joining i to this condition can be restated as the products of the numbers of arrows in one direction around any cycle equals the product of the number of arrows in the other direction.

252

Lattices and Finite Root Systems

We now return to the case of finite root systems to illustrate and apply some of the concepts just introduced. Example S Bases for the root systems of types A 2, and along with their Coxeter-Dynkin diagrams are shown in Figure 3.1. We will see shortly that to each diagram there is (up to isomorphism) only one reduced root system. Let us clarify the relationship between root systems and Coxeter-Dynkin diagrams. Given a root system A and a base II of A, once we index the elements of II, we can write down a Cartan matrix. From the matrix we derive an incidence matrix and corresponding diagram. Reindexing the elements of II leads to the “same” diagram with the nodes similarly reindexed. Choosing a different base II' of A, we find a w e IF such that wU = n '. Since (w(a)\w(p)) = (a|j8), II and vvll lead to the same matrix A and then to the same diagram. Now we show that the diagram r(A) determines A to within isomorphism. Proposition 2 I f A and A' are two reduced root systems such that F(A) —F(A'), then A ~ A'. Proof We may assume that F(A) = F(A'). Index the / nodes of the diagram with the numbers 1,..., / in any way. This gives rise to Cartan matrices A and A' for A and A. Let II = { a ^ , a n d II' = {a[ , . . . , a]} be the corresponding bases. Let V and V' be the ambient spaces of A and A'. There is a unique linear isomorphism : F ^ F ' such that (a¿) = a', i = 1,. . ., /. Let r¿ and r¡ be the reflections in a¿ and a', respectively. Then

Since Aji = A'ji, it follows immediately that r[ = r¿(l>-1 Hence we have an isomorphism W ^ W' with <^(w) = ) in the category of group representations; that is, the diagram W

X

♦1 W' commutes.

V

---- >

[* X

V

---- V

3.4

Graphs and Coxeter-Dynkin Diagrams

253

In particular, <^(A) = <^(W^II) = ^(W)(l>(Ji) = W'U' = A' (Use Proposi­ tion 3.3.4) which shows that (f>is an isomorphism. □ Remark 1 It would be more accurate to require that r(A) ^ r(A) (in the sense of graph theory) rather that F(A) = F(A') in the last proposition. It is easy to make this minor formal modification if needed. Example 9 (Rank 1 and rank 2 root systems) Suppose that A is a root system of rank 1. Then A has a base II = {a}, and the Coxeter-Dynkin diagram is a single node O and the ambient space is V= Ka. The Weyl group W is generated by and rj^a) = - a . Thus ^red = w H = {a, —a}. If A then ± 2 a are also roots (Section 3.2, case 1) and A = {a,2a, —a, —2a) (said to be of type If A = then A is said to be of type Suppose next that A is a root system of rank 2 and that II = {a^, «2) is a base. Then A ^2 '= («i, «2" ) ^21 '= ( ^ 2^^ 1" ) ^^e nonpositive integers. Reindexing, if necessary, so that |^2il ^ fhe possibilities listed in Table 3.2 (see Section 3.2, case 2) Reduced root systems for each of these diagrams are easily constructed. They are shown below in real euclidean 2-space (as far as a sheet of paper can represent euclidean 2-space!) The reader can easily construct these: For instance, for A 2 one has the Cartan matrix is generated by

| ^ ^j and its Weyl group W

and ^2- where ^1( ^ 1) =

'*1(^2) = «1 + 0^2.

''2(^1) = Oi^+ a2,

''2(«2) = “ «2-

Thus .

-« 1 <— ^ «1 (aj + a2)

- («1 + «2) —ao <— > an determines IF • II = Table 3.2 ^12

0 -1 -1 -1

'■ 21

0 -1 -2 -3

Coxeter-Dynkin diagram

0 0 0 —- 0 0 <= 0 0 - ^ 0

Name Ai VA Ai Cl Gi

254

Lattices and Finite Root Systems

vAi

+ 3«2

Figure 3.2. Reduced finite root systems of rank 2

If A is not reduced, then 2 a is a root for some indivisible root a. Using W, we obtain 2a¿ as a root for / = 1 or 2. Then (2a^)'" = and we must have <j8, \af ) e Z for all )8 g A. This happens only in and in C2 with / = 1. Up to isomorphism all the possibilities are shown in Figures 3.2 and 3.3. Proposition 3 Let s be the reflection in a vector a given by a decomposition IKa ® H of a vector space V. I f M is a subspace o f V invariant by s, then either IKa a M or M(zH, Proof. If there exists x g M \ / / , then sx —x = ca ^ Ka \ {0}, so IKa c M. □ Proposition 4 The following are equivalent for a root system A in a K-space V: (i) A is indecomposable. (ii) r(A) is connected. (hi) V is an irreducible W-space.

3.4

255

Graphs and Coxeter-Dynkin Diagrams

2ao «2

, «2

«1 «1

2«!

2(

A, V (BC\

iB C \ V (,BC\

(B0 2

Figure 3.3. Nonreduced finite root systems of rank 2

Proof, (ii) => (i) Suppose that A is decomposable: A = Aj V A2. Any bases III and II2 of Ai and A2 combine to form a base II = Hi U Il2 of A. Since for a e III, jS e ^2? = <)3, a '' > = 0, the diagram F(A) is composed of the two disconnected subdiagrams r(Ai) and F(A2). (iii) => (ii) If r(A) decomposes into two disconnected subdiagrams Fi and F2, then any base II of A decomposes nontrivially as IIi U II2 with = 0, whenever a e 111, p e II2. Then the linear spans Fi and F2 of III II2 are both W invariant, so V is reducible. (i) => (iii) Suppose that M is a nontrivial IT-invariant subspace of V. Using Proposition 3.4.3 we partition A as Ai U A2, with Ai = ( a e Ala e M},

A2= ( a e A|<M,a-> = (0)). If A2 = 0 , then A c M, so M = F. If Ai = 0 , then {M\a^ > = (0) for all a e A, so M = (0). By assumption neither of these happens. Thus Ai # 0 , A2 ^ 0 . By definition (p, a '' > = 0 for jS e Ai, a e A2. Thus A = Ai V A2. □

256

Lattices and Finite Root Systems

Proposition 5 Let V be a K-space and A a root system in V, Define a bilinear form К on Vby K{x,y)=

Y, аеД

Then K is nondegenerate, symmetric, and invariant under Aut(A). Moreover the restriction of K to the rational span Vq of A is positive definite. Proof K is clearly symmetric, and its restriction to Vq is positive definite since c Z . It follows that this restriction is nondegenerate and hence that K itself is nondegenerate (since A spans V). The invariance of K follows from the fact that = = (;c,(c7-(a))" > for all X El Vq and for all a Aut(A) [see Proposition 3.2.6 and equation (3.2.8). □ The bilinear form K constructed above is called the natural bilinear form of A. It is deeply connected with the Killing form of certain semisimple Lie algebras (see Exercise 6.4). In the previous paragraph we indicated that invariant bilinear forms are essentially unique. We now set about giving precise meaning to this. Proposition 6 Let Vbe a K-space, and A be an indecomposable root system in V. Let B be a bilinear form on V that is invariant under the Weyl group W o f A. Suppose that B Q. Then (i) B is nondegenerate, symmetric, and invariant under Aut(A). (ii) I f B' is any bilinear form on V that is W-invariant, then B' = kB for some fc G IK. Proof Consider the left radical of B, namely {x e V\ B(x, y) = 0 for all y e F}. Since B is IT-invariant, this is a IT-stable subspace of V, which is also proper (since B ^ 0). By Proposition 4 the left radical is (0). Similarly the right radical of B is trivial, and hence B is nondegenerate. Let B' be as in part (ii) of Proposition 6. Since V is finite dimensional, there exists / e Endj^(F) such that B\x,y)=B{f{x),y). Let us show that / commutes with IT. Indeed, if vv e IT, then using the fact

3.4

Graphs and Coxeter-Dynkin Diagrams

257

that B and B' are PT-invariant, we obtain B{fw{x),y) =B'{w{x),y) = B ' { x , w - \ y ) ) = B{f{x),w-\y))=B{wf{x),y). Thus Bdf w - wf)(x), y) = 0 for all x and y in V, and hence Jw = wf since B is nondegenerate. Now let a e A, and consider e W. Write V = Ka O H, where H is the hyperplane of V consisting of fixed points of r^. Since fr^ = r^f, we have f { K a ) = / ( l - r J ( F ) = (1 - r J / ( F ) c Ka, and therefore there exists A: e K such that /( a ) = ka. Consider now V' — ker(/-Al). Then V' is IT-invariant (because / commutes with W) and V ^ (0) (because K a c K'). By Proposition 4, V' = V, and therefore B' = kB. This establishes part (ii). Now part (i) follows from part (ii) together with Proposition 6. □ Proposition 7 Suppose that A is decomposable and that B is a Wdnvariant bilinear form on V, Let V ”^iA^ be the decomposition of A into indecomposable factors. Let Bi denote the restriction o f B to where is the ambient space o f A T h e n B(Vi,Vj) = (0) for i ¥=j and B = Furthermore, if is the natural bilinear form of A^, then B = for unique c^s in K. Proposition 8 Let A be an indecomposable root system in V. Let (*|*) be a non-degenerate W-invariant symmetric bilinear form on V. Then for a and P in A we have (ala) = (P\p) ^ W a = Wp. Proof is obvious since ( I ) is PT-invariant by definition. =» We may assume that K = Q and (• | •) is positive definite (Proposition 3.3.7 and Proposition 6). Since Wa spans V, we may replace a by a suitable wa and assume that (a\p) 0. Then 2(a\p)

and by replacing p by - p if necessary, we may assume that (p, a " ) > 0. From (a, p" ) ( p , a ^ ) < 4 we are left with two possibilities: 1. {a, p^ ) = 2 in which case a = p (see Section 3.2), 2. (a, p " ) = (p, a - > = 1 in which case r^r^r^p = r^r^ip - a) = r j , - p —(a —p)) = a. □

258

Lattices and Finite Root Systems

3 .S

CLASSIFICATIO N OF CARTAN M ATRICES A N D FINITE R O O T SYSTEM S

Let A = (Ajj) be an (/ + 1) X (/ + 1) Cartan matrix. (For convenience we will number the rows and columns of A from 0 to /). We think of A as an endomorphism of via A \ \ ^ \A for all X = ( xq, Xj, . . . , Xi) e An element n e of A of eigenvalue 0.

is called a null root of

In other words n = ( wq,

if n is a (left) eigenvector

satisfies

(1)

n A = 0,

(2)

n ^ 0,

(3)

Hi > 0

for all 0 < / < /.

A Cartan matrix is said to be affine if it is indecomposable and admits a null root. If A is affine then det(^) = 0. Example 1 Let ^ = possibilities are ' ^ - ' ^ ■’ - ( - 2

h t sl 2

i )

X

2 affine matrix. Then ab = 4. The



-< )

(we may assume that a < b). Examples of null roots are given by (1,1) for A^l^ and (1, 2) for A^^^. Our next objective is to classify all affine matrices. As a consequence of this classification we will obtain a classification for all finite root systems. (In this section we establish only that finite indecomposable reduced root sys­ tems lie in a certain list. In Section 5.3 we will complete the classification by showing that all these root systems actually exist.) Our approach follows [BMW]. Let A = (^¿y), 0 < /, j < /, be an affine matrix, and let n = (riQ, be a null root. Then =0 /=0

for all 0 < y < /,

C lassification o f Cartan M atrices and Finite Root System s 259

3.5

and hence for all 0 < 7 < /,

(4)

Y , \ ^i j \ ni = 2tij. 1=0

i*j

Proposition 1 Let A be an (/ + 1) X (/ + 1) affine matrix, and let n be a null root o f A. Then (i) all the coefficients o f n are positive and the 0-eigenspace o f A is Un. In particular, if n' is a null root o f A, then n' = qn for some q ^ (ii) There exists a unique null root { n ^ , n f ) o f A satisfying (5)

(6) Proof. Write {0,

ni ^

for all 0 < i < I,

g.c.d. {«0, •••,«;} = 1( 6) = I U J, where I = {i|n, > 0}, J =

= 0).

Because of (4) we see that Aij = 0 whenever / e l and j e J. Since A is indecomposable, either I or J is empty. Hence J = 0 , since n 0. Thus > 0 for all /. Let m = (mo,. . . , m^) be a left 0-eigenvector of A. We can choose A e R such that n^ — Am, > 0 for all 0 < / < /, n, - Am, = 0 for some /. Then n - Am is a null root. By the above argument n, —Am, = 0 for all /. Thus m = An. This proves part (i). As for part (ii), since A has rational coefficients and 0 e Q is an eigenvalue of ^ has a rational 0-eigenvector. By part (i) it is a multiple of n. Thus we may assume first that n e then by clearing denominators that n e and finally, removing common factors, that n is as in part (ii). Uniqueness follows from part (i). □ The null root n = (« q, . . . , n^) of A described in part (ii) of last proposi­ tion will be called the null root of A, We call n, the mark of the / node of the Coxeter-Dynkin diagram of A.

260

Lattices and Finite Root Systems

Example 2 Let 2 -1 0

-1 2 -1

0 -3 2

The Coxeter-Dynkin diagram of A is

00 0^0 1 2 -

and n = (1,2,3) is the null root, since with its marksisgiven by 1

= 0. The Coxeter-Dynkin diagram 2

3

0 0^0 -

0

1

2

Next weclassify allCoxeter-Dynkin diagrams arising from affine matrices A, Let r be the Coxeter-Dynkin diagram of A. The nodes are indexed from 0 to /, and we let be the mark of the i node. To each (/,;)-arrow (an arrow from the i to the j node with i j) we attach a weight n^/rij. Since there are ;)-arrows, and we have from (4) that for all 0 < j < I, (7)

n: L \Au\- = 2 ¿= 0 i^j

We conclude that 1. The sum of all the weights o f the arrows arriving at any node is 2. If there is a (y, /)-arrow there is also an (/, ;)-arrow and its weight is n^/n^ (the reciprocal of nj nj ) . Together with property 1 this implies property 2. 2. The weight w o f any arrow satisfies \ < w < 2, and hence we have property 3, 3. There are at most four arrows arriving at any node. Using properties 1 and 2, it follows that property 4 holds. 4. There exists no weight w satisfying f < w < 2, and hence by taking reciprocals, we have property 5. 5. There exists no weight w satisfying \ < w < \ . Because of property 5 it is impossible to complete a sum of weights lying between f and f to 2. Thus we have property 6. 6. There exists no weight w satisfying j < vr < f , and hence taking recipro­ cals results in property 7. 7. There exists no weight w satisfying \ < w < \ .

3.5

Classification of Cartan Matrices and Finite Root Systems

261

By using the seven properties above, we investigate the diagrams that may arise according to the number of arrows arriving to a node. Four Arrows Arrive at a Node. Suppose that 4 arrows arrive at a node i. Each of these arrows must have weight If one of these arrows is of type (;, /), then there is at least one arrow of type (/, j) and each of these is of weight 2. Hence there is a unique arrow of type (/, j) (of weight 2), and hence no other arrow may arrive at j. The only possibilities are (each diagram is given with its marks). 1

1

o

0

1 0 ^ 0

0 0 -0 -

1

|2

1

|2

0

0

1 1

1

1

2

1

1



0 =>0 ^ 1 1

Bcf>

2

1

0 0^0 -

2

o » 0 -

Each of these diagrams is complete in the sense that it satisfies property 1. (See below for some remarks on the labeling convention.) Three Arrows Arrive at a Node. Let the weights of these arrows he w^ < W2 <Wy Recall that w^ > ^. Suppose that w^ = ^. Then W2 w^ = f - Thus W2 < I, and hence either W2 = or We see that the only possibilities are (w^,W2,w^) = {^ , ^ , 1) ,

or

or

Suppose that vwj = f . Then W2 + w^ = j. Thus W2 < f , and hence w^ W2 = W3 = f . We have {W^,W2,W3) = Suppose w^ > f . Then W2 + w^ < j , and hence vi^2 < f which violates w^ < W2. Having determined all possible weights we study each case separately

262

Lattices and Finite Root Systems

Case (j,

1). We start with

‘Q\

2

2

1

2

2

or 0 ^ 0 - 0

p - O

O In either case all nodes except the extreme right-hand node are full (sum of arriving weights = 2). These diagrams can be extended to include an arbitrary number, say, /, of nodes of the form 1

Q\

2

2

2

/ 0 - 0 ---------------O

1

"

2

2

0 ^ 0 - 0 -

2

-o

0 1

and then completed to one of the following diagrams (with 1 + 1 nodes)

.

0

a /O

0-0---- o

o

1

1

1

2

2

2

2

0 - 0 ----------- o « o 0 1

1

BCP>:

22

2

2

0 ^ 0 - 0 ----------0 ^ 0 1

1

2

2

0^0-0---- o'\ 1

cp>:

0

2

^

0

2

- 0

O

o

2

---------------- 0 ^

1

0

3.5

Classification of Caitan Matrices and Finite Root Systems

263

Case ( |, f , f ). We start with

0—0—0 3

4

o—o<=o

3

In either case the node with a mark 2 is full. In the first diagram the nodes with mark 3 have one arrow of weight | arriving at them. There must be one more arrow of weight f arriving at them. This leads to

o-o-o-o-o 2

3

4

3

2

and, by a similar argument, completes to

0 0 0 6 0 0-0 -

-

1

-

2

-

3

-

4

3

2

1

The same type of reasoning shows that our other diagram leads to O -O ^ O -O -O 2

4

3

2

1

Case (j, f , f ). We start with

o-o-o 5

6

4

The node with a 3 is full, and the diagram can only be completed to 3

0 0 0 0 0 6 0-0 -

-

1

2

-

-

-

3

4

5

2

3

2

-

6

4

2

Case ( f , f , f ). We start with 2

0 - 0<=0

Q 0 0-0 -

2

3

2

3

2

0^ 0

264

Lattices and Finite Root Systems

and these complete in unique ways to 1

?

£:

0 0 6 0 -0 -

-

-

O -O -O ^ O -O

6 6-0 ^

A t Most Two Arrows Arrive at Every Node. We start with one of the following 1

.1

1

o-3!o

A^P:

1

^

1

1

o ^ o = ^ o

0-0 ----- 0-0 1 1

1 1

or

0^0-0---o1 1 1 1 The first two diagrams are complete, while the other two complete to one of 1

.o

0-0 ------- 0-0 1 1

1 1

or o « = o - o -------------- 0 ^ 0

1

1

1

1 1

-

A t Most One Arrow Arrives at Every Node. Since the diagram is connected, the only possibility is Q —Q , which is not affine. No Arrows Arrive at Every Node. Since the diagram is connected, the only possibility is Q , which is not affine.

3.5

Classification of Caitan Matrices and Finite Root Systems

265

Proposition 2

Let A be an (/ + 1) X (/ + 1) affine Cartan matrix. Then its Coxeter-Dynkin diagram T is of the form where is in the following list {all diagrams have / + 1 nodes and are given with their marks): In particular affine matrices are symmetrizable. 1

,o 0-0 ---------1

/> 2

0-0

-

1

1

1

1

Q

\,

0 0 -

o^^

2

^^ 3 2

^

1

CP:

--------- 0 ^ 0



0 ^ 0 - 0 - - ------ 0 - 0 < ^ 0 1

2

2

2

2

^^ 2

1 1

1

/O O i” :

^

0 - 0 ------- ---------

0 - 0 ,

' i “ 1

1

E<‘>;

o-o-O-o-o 1

E y '- -

2

2

1

0 0 0 6 0 0-0 -

1

^

3

-

2

-

3

-

4

-

3

2

1

5 01 02 03 04 05 66 04 - 02 " ^

-

-

-

-

01 0 03 0 -02 2 4 -

-

= ^

-

-

266

Lattices and Finite Root Systems

G<»: r:

0 - 0 ^ 0 1

2

3

0

O

1

1

Q ^ 0 - 0 ---------0 ^ 0 2

2

2

^^ 3 1

1

0^ 0-0 1

fiC p :

1

------------------------------------------------------------------

1

0

-

1

0 ^ 0 - 0 - ---------0 ^ 0 1

2

2

2

0=^0

1

1

^^2

' ^ 2 2

o-o-o^o-o 1

2

3

2

B C P>=^P: G p:

0 0^0 -

1

2

1

Remark 1 The meaning of the number a e {1,2,3} appearing in be found in [Mo3]. An alternate nomenclature is used in [Ka5].

can

Remark 2 Suppose that A is an affine Cartan matrix. Then is clearly a Cartan matrix. The Coxeter-Dynkin diagram of A ^ is obtained by reversing the arrows on the diagram of A (since we are interchanging the roles of Aij and Aji), By inspection in Proposition 2 it follows that A ^ is also affine (or see Proposition 3.6.5). For example, has matrix 2-1 O] ^ = ^-3 2 - i j and diagram Q ^ Q _ Q , while A'^ has diagram Q

__Q

and is affine of type G^^\

We now begin the classification of the Coxeter-Dynkin diagrams of all finite root systems. Let A = (A^jX 1 < i, j < I, be the Cartan matrix of a finite indecomposable reduced root system A arising from a base II = ( a j,. . . , of A. Thus ^ ij

{

}•

3.5

Let

Classification of Cartan Matrices and Finite Root Systems

267

e A be chosen so that the height of 4> is maximal. That is, ht(o;) <

(We will see that and hence


for all Of e A.

is unique.) Then for all

( (f), a / ) > 0

e n we have ht

< ht

(f>,

for all 1 < i < 1.

If we choose a positive definite PT-invariant bilinear form as in Proposition 3.4.6, we have > 0,

1
Define for all 1 < i < I,

^ 0/ = -

I.. ^ (a ,la ,)

= - ( « ; )

and 2 (g ,l< /> )

^io — We can then define an (/ + 1) X (/ + 1) Cartan matrix A by A^j = {A^j) for all 0 < i, j < I where A qq == 2. Lemma 3 A is an affine Cartan matrix. Proof. That ^ is a Cartan matrix follows from construction. We show that A is indecomposable. Indeed the 0 node of the Coxeter-Dynkin diagram f of is connected to some other node for otherwise (<^|<^) = 0. With the 0 node removed, the diagram left is connected (since A is indecomposable). Thus f is connected, and hence A is indecomposable. To establish the lemma, we must show that A admits a null root. Write /
-(f>.

Clearly n^ > 0. Let Wq == 1, and let n == (nQ, n^,..., n^). Then for all 0 < ; < /

268

Lattices and Finite Root Systems

we have

1=0

= A qj + ^ /=1 = 0.

(« > ;)

( “ yl“ ;)

This shows that n A = 0 and hence that A is affine.



Theorem 4 (i) Up to isomorphism there exists a 1-1 correspondence between finite indecomposable reduced root systems and the diagrams listed below. This correspondence is given by attaching to a root system its Coxeter-Dynkin diagram with respect to any base,

0-0-0----------O 1

Br.

2

2

2

0 - 0 — 0 ^ 0 2

2

2

Q: 0 - 0 —

1

0<=0

^^2 1

Or-

1 2 0 - 0 ----------------

2/ o

/> 4

0 1

1

2

^

2

1

o-o-o-o-o z.

1

2

3

?|4.

3

2

2

3

4

5

s |6

4

2

3

4

2

2

3

£7: o-o-o-o-o-o

f.^2-

2

o-o-o-o-o-o-o o-o=o-o 0 ^ 0

3.5

Classification of Cartan Matrices and Finite Root Systems

269

(ii) If A is an indecomposable reduced finite root system, H = • • • aj) a base o f A, and T is its Coxeter-Dynkin diagram with respect to H, then A has a unique root (f>whose height with respect to H is maximal. Moreover, if

4> = H riiOLi, i= l

then the n^ are the marks o f Y as they appear in the graphs o f part (/) of the Theorem, and for all a E: ^ we have a < r^a for all 1 < f < /. That is, r^a = a - ka^, where A: > 0, or equivalently (a, a ^ } > 0 for all 1 < / < /, or equivalently (a|a^) > 0 for all 1 < i < 1. 1. If a = is dominant, then m^ > 0 for all i: First, 0 < (a |a ) = Urnfala^) together with (a|a^) > 0 for all i im­ plies that some > 0, and hence a e A+. Write {1, ...,/} = I U J, where I = {i\m^ > 0} and J = {i\m^ = 0}. Since (a, a ^ ) > 0, we see that = 0 for all i e I and j e J. Since A is indecomposable, we conclude that J is empty. 2. If a = and p = are both dominant then with respect to the Q^-partial ordering (see Section 2.5) either a > ¡3 or p > a: From argument 1 we have (a\p) > 0. Thus {a, = 2(alj8)/()3|/3) > 0, and hence a - p e A (Proposition 3.2.8). Suppose > Pi for some i. Then a — p e A forces a - p e A+ c (2+. Thus mi > Pi for all i. 3. Let a E A be of maximal height with respect to H. Then a is dominant. Moreover (a |a ) > ip\p) for all roots P: That a is dominant is clear. Suppose that A has roots of unequal lengths. If e A is of length different than that of a, we must show

Lattices and Finite Root Systems

270

that (a\a) > (p\p). By replacing p by wp for some vv e we may assume that p is dominant. Indeed, if p is not dominant, then (p,a^^) < 0 for some i and r^p > p. Repeating this argument if necessary, we obtain at last a dominant root. The argument of Step 2 shows that a - j8 e A^. Thus («1«) - (P\P) = ( a + P\a - P) = {a\a —)8) + (P\a — p) > 0 (the last inequality since a and p are dominant and a — p ^ Q+), Finally, (a\a) > (p\p), since a and p are supposed to have different lengths. 4. There exists a unique root (f> = of maximal height. Moreover i\(t>) > {p\p) and 4> > P for all e A: The first two assertions follow from arguments 2 and 3. Let j8 e A. Using the same argument as in 3, we conclude that there is a dominant root y with y > p. Now (j) > y > p hy 2. The root (f> above is called the highest root of A (with respect to II). We reserve the notation ..., for its coefficients. A root is called long if it has the same square length as (f>. 5.

If n^ = 1 for some 0 < f < / , then is long: Note that Uq = —(!> is long by definition. If f > 0 and if is not a long root, let i = Iq, ¿1, . . . , t)e a minimal set of distinct indices in { !,...,/} so that = («/J«/,) = ^ each 1 < j < k, A: , ¥= 0. Thus from the Table 3.1,

0 - 0 -----------0 - ^ 0 ^0 ^k-l with m > 1. Then r,^0 n, = 1.

r,^k-la:^k = ma:^0 + ma, +

H-m^

+ a, < S contradicts

Proof of Theorem (except for existence). Let A be an indecomposable finite root system, and let II = {a^,...,« /} be a base of A. Suppose that the Cartan matrix of n (hence of A) is A. Let (f> = be the highest root of A

3.5

Classification of Caitan Matrices and Finite Root Systems

271

with respect to II. Using Lemma 3, form the affine matrix A, The CoxeterDynkin diagram t of A is the Coxeter-Dynkin diagram of A extended by one node, the extended node being determined by —(f>. The marks are riQ= 1, /Ip , rii and — has the same square length as some i = 1, . . . , /). 5. f has marks = 1 only over nodes corresponding to long roots (by argument 5 above). Regarding claim 3, it is useful to observe that whenever we have the appearance of two nodes like Q s ^ Q , Q ’ O Coxeter-Dynkin diagram F or F, then, naming the corresponding roots a, ¡3, we have 2(a\p)/(p\p) = —4, —3, or —2 and 2(p\a)/(a\a) = —1, whence (a\a)/(p\p) = 4, 3, or 2, respectively. Thus the node has multiple arrows into it only if there are roots of longer square length than a¿. Now looking at the classification of affine matrices in Proposition 2, we observe that claims 1-5 eliminate all the diagrams except those of the form Moreover, up to a diagram automorphism these diagrams have a unique node with mark = 1. The diagram Xi is obtained by removing such a node. □ Remark 3 The number of nodes whose mark = 1 in is actually the index of connection [P: Q], where P and Q are the weight and root lattices of the root system of type Afp Simply by staring at the diagrams in Theorem 4, we obtain Corollary Let A be an indecomposable reduced finite root system with Coxeter-Dynkin diagram F. Then (i) there are at most two different root lengths in A; (ii) there is at most one multiple arrow in F; (iii) there is at most one node that is connected to more than two nodes, and such a node is connected to exactly three nodes; (iv) the corresponding Cartan matrix is symmetrizable.

272

Lattices and Finite Root Systems

3.6

THE PERRON-FROBENIUS THEOREM AND ITS CONSEQUENCES

On the set oi m X n real matrices we define two partial orderings > and ^ as follows: Given m X n matrices C = (c,,) and D = C >D C^ D

Cij > dij for all

i
either C = D or 1
and

and

1 < j < n,

> d^j for all

1 < ; < n.

As usual we write C > D (respectively C > D) io denote that C ^ D and C > D (respectively C D), We say that C is positive (resp. nonnegative) if C > 0 (resp. C > 0, where 0 denotes the zero matrix of appropriate size. If C in a square matrix, we say that C is primitive if 0 for some A: e Z+ C is called semiprimitive if e l C is primitive for all e e Throughout this section will denote the set of all column vectors X = (jCi,. . . , such that x > 0. The main result of this section is the following:

Theorem 1 Let C be a semiprimitive nonnegative n eigenvalue r satisfying

X

n matrix. Then C has a real

(i) r > 0. Furthermore r > Q if C is primitive or if n > 1; (ii) there exist positive left and right eigenvectors for r, each unique up to positive scalar factors; (iii) r > 1^1 for all other eigenvalues s of C and the multiplicity o f r is 1; (iv) if C > D > 0 and d is an eigenvalue of D, then \d\ < r and \d\ = r if and only if D = C. The eigenvalue r is called the Perron-Frobenius eigenvalue of A. Example 1 Let T be a finite labeled graph, and let C = C(T) be the incidence matrix of T. Thus the vertices of T are labeled ! , . . . , « in some way and is defined as the number of arrows from vertex i to vertex j for i # j and c¿¿ = 0 for all i. Certainly C > 0. It is straightforward to see that C is semiprimitive if and only if T is connected. Indeed, if « = 1, this is trivial. Suppose that n > 1, C is semiprimitive and (e / + C)^ >- 0. Then for all > 0, where the sum runs over all . . . , j ^[i,n] i, j, Ec;.,., • c;.Ill2

3.6

The Perron-Frobenius Theorem and Its Consequences

273

and dpq '= (s i + C)p^. Observe that the inequality itself is independent of s (> 0). Suppose that i ¥=j. Take any summand > 0, and omit all factors that are diagonal entries (Cp^X The remaining product is still positive, and by definition of C defines a path from vertex i to vertex j. Conversely, suppose that we have a path of length m = m(i,j) from i to Then we obtain a product ‘ j > 0, and we see that (C'”),y > 0. Then, for all e Z+ and e > 0, ( ( e / + includes the summand • ** c, fS — e > 0 (k factors of eX and hence we see > 0. Now if r is connected taking M == max{m(/,y)}, it is easy to see that (el + C )^ 0. Thus C is semiprimitive. In particular, if ^ is a Cartan matrix, then C '= 2 —A is its incidence graph, and C is semiprimitive if and only if the graph is connected (i.e., A is indecomposable). Later on we will prove the remarkable fact that the Perron-Frobenius eigenvalue of C(T) is 2 if and only if r is the Coxeter-Dynkin diagram of an affine Cartan matrix. Our proof of Theorem 1 follows [Sn]. We begin with a sequence of lemmas. We assume first that C is primitive and that m has been chosen so that > 0. Lemma 2 If a> Q and Cx = ax for some x e Proof If X ¥= 0, then a’^x = C ^x

q,

then either x ^ Q or x = Q.

0, so jc

0.



Lemma 3 Let C j,. .. , C„ be the rows o f C, and define

by I \ R ( x ) = m i n i ----->

I

i

T forallx = ( x ^ , . . . , x ^ ) .

(IfXj = 0, CjX/Xj is understood to be +oo.) Then R assumes a maximum value r at some point x e q\ {0}. Proof Let M = max^ y{c,y}. Then for x e R > o \ R(x)Xj < CjX =

^

for each j = 1, . . . , n.

k Adding, we obtain R{ x) Y,Xj < nM(l,Xi^),

274

Lattices and Finite Root Systems

whence

< nM. Thus R is bounded above. Define r '=

sup

Evidently 00 > r > 0. Since each of the functions CjX/Xj is continuous where it is defined, R is continuous. Furthermore R(x) = R{ax) for all a e and hence r = sup x^S where S ’= [R>o ^ [x\x^x = 1}. The latter being compact, R assumes a maximum on S, hence on R>o\№}. This proves the existence of x as required. □ Henceforth r will be the quantity defined in Lemma 3. Lemma 4 If X e

\ {0}

if rx < Cc, then rx = Cx and x

0.

Proof By assumption (C - r)x > 0. If this is not zero, then C(C'”x) - r{C^x) = C^{C - r ) ( x ) > 0. Setting x' := C"*x, we have rx' < Cx' and hence rx'j < Cjx' for all ;, contrary to the definition of r. Thus (C - r)x = 0 and x 0 by Lemma 2. □ Proof (of Theorem 1). We begin by assuming that C is primitive. By the definition of X (Lemma 3), rx < Cx and hence by Lemma 3.4, rx = Cx,

X

0.

Suppose that Cx = sx for some x e C" \ {0}, ^ e C. Then for each j =

( 1)

\sxj\ = |C^-x| < Y,Cji\Xi\ (=

+ooii Xj = 0).

3.6

The Perron-Frobenius Theorem and Its Consequences

275

Set

Then \s\ < R { x ) < r. Now if \s\ = r, then from (1) rx < Cx so by Lemma 4 rx = Cx, Set

jc >- 0.

Then

Since the Xy e C \ {0} and the > 0, we see from this equality that jCj,..., all have the same argument, say, 6. Thus Xj = e'^\xj\, j = 1, . . . , and X = e^^x. Hence Cx = sx => Cx = sx, which proves that s is real and finally that s = r. Suppose that x, x' are nonzero eigenvectors for r. We can assume from the argument just given that x, x' > 0 and choose a e R minimal so that some component of x — ax' equals 0. Then x — ax' > 0, and by Lemma 2, X - ax' = 0. This proves that x and x' are linearly dependent (hence multiples of Jc) and the multiplicity of r is one. Replacing C by C^, we obtain a positive left eigenvector for C with Perron-Frobenius eigenvalue r'. Thus all eigenvalues s of satisfy \s\ < r'. Since C and have the same eigenvalues, r = r'. This concludes the proof of parts (0, (ii), and (iii) in the primitive case. For part (iii) suppose that D < C and that D > 0. Suppose that y is a nonzero eigenvector for D with eigenvalue d. Then using (1), we get Idly < D y < C y , where y = ( ly j,. . . , ly„l)^. Let 3c^ be a positive left eigenvector for C with eigenvalue r. Then |dl;c^y <

x^Dy < x^Cy = rx^y.

276 SO

Lattices and Finite Root Systems

\d\ < r. If \d\ = r, then ry < Cy, and by Lemma 4, ry = Cy,

y > 0.

Thus ry < Dy < Cy = ry. It follows that Dy = Cy, and since all entires of y are positive, D = C. Now suppose that C is semiprimitive. Then for all e > 0, C(e) ■= el + C is primitive. Now C(e) has the same eigenvectors as C and has all its eigenvalues shifted by e. Thus, if x is the right Perron-Frobenius eigenvector of C(e) for some, hence all, e > 0 and the corresponding eigenvalue is r^, we have C ( s ) x = ex + Cx = r^x so Cx = rx. where r ‘= r^ - e is independent of e. Obviously r > 0, since > 0. If n > 1, then some row, say, Q, of C is not 0, and 'LJ^iC^Xj = rxj together with X > 0 gives r > 0. The remaining statements, parts (ii)-(iv), are now obvious. For part (iv) we use C(e) > D(e) > 0 for all e > 0. □ Let A be an indecomposable Cartan matrix, and write A = 21 — P. Then, as we saw in Example 1, P > 0 and P is semiprimitive. We let r = r{A) be defined as the Perron-Frobenius eigenvalue of P. A is called of finite (resp. affine, indefinite) type according as r{ A) < 2

(resp.= 2, > 2).

The apparent conflict in the use of the word affine is resolved in the following proposition. Proposition 5 [Vi] Let A be indecomposable Cartan matrix indexed by J = { ! ,..., /}. One of the three mutually exclusive cases occurs: (i) Finite. A is o f finite type <=>

e

<=>

e IR^\ {0},

<=>3 x ^

\ {0},

jc > 0 with Ax < 0, X > 0 with Ax > 0, Ax with Ax > 0.

0,

3.6

111

The Perron-Frobenius Theorem and Its Consequences

(ii) Affine. A is o f affine type <=>

\ {0},

<=>

G -+

a:

> 0 with Ax = 0,

with Ax = 0.

(iii) Indefinite. A is o f indefinite type <=» 3 j : e

«=>

R ^ \ {0},

G

\ {0},

<=> 3 x G Z+

a:

> 0

with Ax

<

0, Ax

0,

jc > 0 with Ax > 0,

with Ax < 0.

Moreover, A and A ^ fall under the same case. Proof Write A = 21 - P, and let r > 0 be the Perron-Frobenius eigenvalue of P. Let u and u be associated left and right Perron-Frobenius eigenvectors for P. Thus w 0, i; 0 and uP = ru, Pv = ru. If r = 2, then uP = 2u => uA = 0 A is affine. Conversely, if A is affine with null root n, then nP = 2n and 2n • i; = nPi; = rn ' v. Since n • i; > 0, r = 2. Thus A

affine

r{ A ) = 2.

The rest of the affine case is already done in Proposition 3.5.1. Henceforth assume that A is not affine so that r # 2. Suppose that AG R^ \ {0}, a : > 0, and Ax < 0. Then A x < 0 = > P x > 2 x = > uPx > 2wc => rwc > 2wc => r > 2. Thus A is indefinite. In precisely the same way, A G R^ \ {0}, A > 0, and Ax > Q =>A is finite. This proves all the implica­ tions “ < = 3 a ... Suppose that A is indefinite. Then the set F :=

{a G

WjPx

>

2

a

}

is a nonempty open cone (note that u ^ V) and hence there exists a point AG K n Q +. Scaling A , we can assume that a g Z +. Then ^ 0. In precisely the same way, A is finite => 3 a g Z+ with Ax > 0. This proves all the implications “ => 3 a ... The remaining implications now follow auto­ matically. □ Remark 1 Proposition 5 is a version of Vinberg’s lemma [Vi]. We have phrased it in terms of Cartan matrices in order to make it fit most easily into the material to follow. Vinberg uses some properties of dual convex cone theory to establish his lemma, although he points out that the proof can be carried out by the Perron-Frobenius theory, as we have done.

278

Lattices and Finite Root Systems

We have already classified the Cartan matrices of affine type. We now show that the Cartan matrices of finite type are precisely those whose diagrams appear in Theorem 3.5.4. Let A = (Aij) and A' = (A]j) be Cartan matrices of dimensions / X / and r X /', respectively. We say that A is inferior to A if there is an injective map

such that IA'a \ < I

I

for 1 < i, j < V.

Thus A is inferior to A if the Coxeter-Dynkin diagram of A can be obtained from that of A by removing nodes and arrows. Proposition 6 Let A be an indecomposable Cartan matrix with Coxeter-Dynkin diagram T. (i) (ii)

I f r appears in the list o f Theorem 3.5.4, then A is inferior to some affine matrix, I f r does not appear in the list o f Theorem 3.5.4, then there is an affine matrix inferior to A,

Proof (i) The proof is clear by the way in which we obtained the list of Theorem 3.5.4. (ii) Suppose that T is not in the list of Theorem 3.5.4. If T contains a cycle then some A^l^, A: > 2, is inferior to F. If F contains Q Q with ab > 4, then either

Q^ O

O^ O

inferior to F. If F contains a node of

valence > 4 (i.e., a node with 4 or more adjacent nodes) or two nodes of valence 3, then is inferior for some k. If there are two multiple edges (i.e., O # 0> !>’ then O = 0 - 0 --- 0 - 0 = O some orientation of the arrows is inferior. If there is a single multiple edge and a node of valence 3, then

o =o-o-o-o;

,o 'O

(again with some orientation) is inferior. If there is a single multiple edge and every node is of valence < 3, then Q — Q — 0 ^ 0 — inferior since Bi, Cl, and are excluded by hypothesis. Finally, we are reduced to

3.6

The Perron-Frobenius Theorem and Its Consequences

279

the case of only single edges, and the hypothesis leads us to conclude that one of or is inferior. □ Let A' = 21 — P \ A = 21 — P be two indecomposable Cartan matrices of dimensions /' X /' and / X /, respectively. Then A' is inferior to A if and only if there is an injective map *: /'} ---- > such that F/y < for all 1 < i, j < /'. Then /' < /, and we may assume, if we wish, that /* = i for each i. If I' < I , then extend P' to an / X / matrix P' by filling the new entries with zeros. Then 0 < P' < P, and the spectrum (= the set of eigenvalues) of P' differs from that of P' only by the possible addition of zero. By part iii of Theorem 1 all eigenvalues d of P' satisfy d < r(A) (:= Perron-Frobenius eigenvalue of P), and equality occurs if and only if ?' = P. It follows that KA'X the Perron-Frobenius eigenvalue of P \ satisfies r(A') < r ( A ) with equality if and only if ^ ' = ^4. Thus Proposition 7 Let A and A be indecomposable Cartan matrices. Then A inferior to A => r(A) < r(A) with equality if and only if A = A. Putting Propositions 6 and 7 together, we have Proposition 8 The Cartan matrices o f finite type are precisely those whose diagrams are listed in Theorem 3.5.4. Proposition 9 Let A be a symmetrizable indecomposable Cartan matrix, and suppose that A is symmetrized by e = diagie^,. . . , e^}, where each > 0. Then (i) Ae is positive definite <=>A is o f finite type, (ii) A s is positive semidefinite A is o f affine type, (iii) Ae is indefinite A is o f indefinite type. Furthermore the eigenvalues o f A are all real. Proof Let sY'^ be a square root of s^, and let s^^'^ -= diag{sj/^,. . . , sY^}. Then the equations A^Sj = A -^s^ show that is symmetric, and of course A is similar to Furthermore for y e U^, y^(As)y = so A s is positive definite, positive semidefinite, or indefinite as s'^'^^Ae^^^ is. But the latter is determined by the eigenvalues

280

Lattices and Finite Root Systems

of being all positive, all nonnegative, or not all nonnegative, respectively. However, the spectrum S p e c i e o f is real and is equal to S pecif) = Spec(2 —P). Since the eigenvalues of P are maximized by the Perron-Frobenius eigenvalue r, Spec(2 —P) is minimized by 2 —r. The result follows from the definition of finite type, affine type, indefinite type. □ The approach to Cartan matrices through the use of the Perron-Frobenius theory came to our attention through the work of N. Iwahori [Iw]. The theory of the spectra of graphs is quite extensive; see, for instance, [CDS].

3 .7

CONSTRUCTING L IE ALG E BR A S F RO M LATTICES

In this section we show how one can construct a Lie algebra from any positive definite, even geometric, lattice L by using the elements of norm 2 in L. The construction produces a free Z-module of finite rank (a finitely generated torsion-free abelian group) of the form 9^ = L ®

( 1)

© e L (2 )

together with a multiplication [•, •]: 9 l X 9^^ ^ 9z. that satisfies the two Lie identities: skew-symmetry and the Jacobi identity. In as much as our scalars are integers rather than elements of some field, is a Lie algebra over Z, sometimes called a Lie ring. This Lie ring (see Section 1.1) will be graded by L with as the elements of degree a and L itself as the elements of degree 0. Of course should it happen that L(2) = 0 , none of this would be of any interest. Henceforth we will assume that L(2) 0. One easily obtains L-graded Lie algebras Qo< over a field IK(even if IKis of characteristic 0) by extension of the base ring (see Section 1.1) 9iK ==

= ( 11^

®

© e L (2 )

The Lie algebras obtained in this way from the lattices of types ^4/, Z)/, £5, Ej, and £’g are the Lie algebras of the same name, and they provide us with about one-half of the so-called finite-dimensional split simple Lie algebras. Our approach follows [FLM]. We make the following observation: Suppose that ( L , ( | • )) is a positive definite geometric lattice. Then for a, /3 e L(2) precisely one of the following

3.7

C onstructing Lie Algebras from Lattices

281

holds: a

(2)

/3 ^

U

a

p ^

and

a

p = 0 and

+

{0} and

(a|/3) > 0, («1/3) = - 1 , (a|/3) = - 2 .

by the Schwarz inequality. |( a |^ ) |< ( ( a k ) ( / 3 |/ 3 ) ) ‘/^ = 2 with equality if and only if a and p are linearly dependent, and (2) follows at once. From the point of view of defining the multiplication on the main task is to define the products [X^, X^]. Of these the most interesting is the case when (a\^) = —1. Then [ X ^ ,X , ] = The choice of sign is a very interesting problem which ultimately is related to making a suitable central extension of L by Z/2Z. The details of this are left to Section 3.8, where we study such central extensions more carefully. For now it suffices to assume that there is a biadditive mapping s: L X L satisfying (3)

e (a , a ) = | ( a |a ) (mod2)

fo ra lla e L .

and hence also (4)

e(a, p) + e(/3, a) = (a|j8) (m od2)

for all a, p ^ L

We then define [X^, X^] = ( — for (a\p) = —1. Notice how skew-symmetry follows form (4). The last part of the section is devoted to determining the basic properties of like showing that admits a triangular decomposition with an anti-involution o) interchanging X^ and - X _ ^ for all a e L(2). As we know L(2) is a finite root system in its Q-span. Once a base {a^,. . . , a/} of this root system is chosen, we use it to determine a set of Lie algebra generators of g^^ and a set of relations, which, as we will see in Chapter 4, actually gives a presentation of g^. Since L(2) is a root system, we call the elements of L(2) roots. Define g^ by (1).

282

Lattices and Finite Root Systems

Define [•, • ] on

as follows:

[L,L] = (0), [a, Xp] =

= - [Xp, a]

0

(5)

for all a e L, j8 e L(2);

if(«l/3)>0, if ( a |/ 3 ) = - l , if( a |/3 ) = - 2 .

Xjg] = I -a

for all a,/3 e L(2),

Proposition 1 with the bracket defined by bilinear extension o f (5), is a Lie ring. Proof. First we look at the skew-symmetry. The only nontrivial case is when (a\fi) = —1. Then, as we noted above,

Note that (a|j8) = - 2 happens precisely when j8 = - a in view of the fact that (• I ■) is positive definite. The Jacobi identity involves looking at a number of cases. The hard part is checking that (6 )

[x.,[x,.x,]\

+

-0

when a, j8, y e L(2) and a + /3 + y ^ f^(2). There are three subcases: (1) two pairs of roots add to 0, (2) exactly one pair of roots adds to 0, (3) no pair of roots adds to 0. 1. Suppose that a + /3 = 0 = ^ + 'y- Then a = y and (6) reads

which trivially holds. 2. Suppose that a + /3 = 0. Then /3 + y = - a + y, and certainly at most one of a + y and - a + y may be a root [we need (±a:|y) = -1 ]. If neither is a root, then by (2) either (a\y) = 0 or a = +y. Since we are in case 2, the

3.7

Constructing Lie Algebras from Lattices

latter is impossible, and hence (a\y) = 0. Also (p\y) =

283

so clearly (6) reads

[X ^,[X ^,X .J]= 0. We may assume then that exactly one of + a + y is a root, say, a + y (the other case is similar, since then j8 + y is a root). Now the left-hand side of (6) reads [ x _ ,,[ x ^ ,x ,]] + [X ^,[X ,,X _J]

= 0, since e(a,a) = ^(ala) mod 2 = 1 mod 2 and (a|y) = ~ 13. If none of a + ^ , ^ + y , y + a are roots then (6) is trivially true. Suppose then that /3 -I- y is a root. Then (a|/3) -t- (a|y ) = («1^ + y) = —1, since a -t- /3 -I- y e L(2). Because we are in case 3, (a\P) > —1, (a|y ) > —1. The only possible solution is for («1)3) = 0 (resp. —1) (“ ly) = ~ 1 (resp. 0). Assume the first case. We have then (a|/3) = 0 , ( a |y ) = - 1 ,

and

(^ ly ) = “ 1-

The left-hand side of (6) reads (7)

{( -

^

Adding e(a, ^ + y) -I- e(/3, y) = e(a, /3) -f e(a, y) + + e(y, a) = sip, y) -I- e(/3, a ) + e(y, a), we get e ( a , p ) + £(j8, a ) -I- e ( a ,y ) -I- c(y>“ ) = ((ali3) -I- (a ly )) mod2 = lm od2, which shows that (7) is 0. The other case is similar. Define a bijective linear mapping 9l

0L

y

+

284

Lattices and Finite Root Systems

by =

for all a g L (2) ,

« li = id. It is easy to see that a> is an anti-involution of g^: Obviously it has order 2, and we have [
= [a,X_^]

= - ( a \ P ) X _ p = (a\l3) 0 , if(a|/3 ) = - 1 , if(a |j8) = - 2. =
—1 0

for all a e L(2), /3 g L,

if a + ¡3 = 0, otherwise.

Proposition 2

The symmetric bilinear form on 9^ is even, nondegenerate, and invariant. It admits co as an isometry. Relative to {'V) we have the orthogonal decomposi­ tion g^ = L ±

±

(ZAT, e Z 2 f _ J .

{a, - a )

Each submodule 0 Z X _^ is a hyperbolic plane. The determinant of (-I*) on is ( - 1)^ det(L), where k = \ card(L(2)X Proof. The orthogonal decomposition is obvious, and it is clear that 0 ZZ_^ is a hyperbolic plane (Section 3.1). The nondegeneracy follows imme­ diately, and the statement about determinants is left as an exercise. The

3.7

Constructing Lie Algebras from Lattices

285

invariance condition has to be checked on a basis made up of the and a basis of L. There are four cases. Case (;), j = 0,1,2,3, accordingly as there are 0, 1, 2, or 3 basis elements of L in the expression ( [ a , 6 ]|c) + ( è |[ a ,c ] ) . We treat only the case (0), which is also the most involved. We suppose that we are looking at (8)

We have to show that it is 0. If a + j8 + y 0, this is automatic. Suppose that a + /3 + y = 0. Then - y = a + /3 e L(2), and (8) becomes

(9)

- ( - 1)

eioc,

/3)

( - 1)

e(a,y)

However, £(oc,p) + e ( a ,y ) = e ( a ,j8) + e{a, - a ) + s (a , -/3 ) = e(a, —a) = s(a, a ) = 1 (mod 2), which shows that (9) reduces to 0. Finally,

= (x jx ,), from which we can see that co is an isometry.



Using the results of Section 3.3, we choose a system of positive roots L(2)+ and a base c L(2)+. Then every element of L(2)+ is a nonnegative integral linear combination of a ¡ and L(2) = L(2) + U - L(2) ^ ,

L(2) + n - L(2) + = 0 .

Let 9 - '“ ®aeL(2)+ ^ ^ -a “ ^^9+)- Then are obviously Z-subalgebras of and

and g_

= g_0 L 0 g+. The spaces ZX^ are root spaces in the usual sense that they are eigenspaces for ad L (strictly speaking we should be talking about Z-modules rather than spaces). The corresponding eigenfunctions are the functionals á: h ^ {a\h). We usually identify á and a. With this convention we have a triangular decomposition (g+, L, (2+, co) of g^ with root lattice Q = ©/^jZa¿. (Here

Lattices and Finite Root Systems

286

we are working with a Lie algebras over Z rather than over some field; see Section 2.1.) Note that [K

9^ = IK 0^ 9_©

K

L ®K

is a triangular decomposition of K 0^ 9 l * In the case where L is generated (as an abelian group) by L(2), we have Q = L. This can easily be arranged by replacing L by the Z-span of its norm 2 vectors from the outset. Proposition 3 Suppose that L is an even positive-definite geometric lattice. Let {a^,... ,a¡\ be a base of the finite root system L(2). Let

be the corresponding triangular decomposition o f the associated Lie algebra Then (i)

= 1, . . . , /} generates g+ and = 1, . . . , /} generates g_ as Lie algebras over Z; (ii) ifL(2) generates L (as an abelian group), then {X^,, X _ ^fi = 1 ,..., /} generate as a Lie algebra over Z; (hi) if L = L^ L L2 (see Section 3.1), then 9^ = 9^^ X 9^^^. Proof (i) It suffices to prove the first statement. Let A+ be the set of positive roots of L(2) relative to the base {a^,. . . , and let m be the subalgebra of 9^ generated by X ^^,. . . , X^^. Let a = Xc^a^ e A+ be a root of height k > 1 (see Section 3.3 for the definition of height). By a standard argument (Proposition 3.3.4) we have that (alay) > 1 for some 1 < j < I and hence that (alay) = 1 by the Schwarz inequality. It follows that a — Oj = rjU ^ L (2). Since ht(a - af) = k - 1 > 0, a - ay e A+, we may assume inductively that ^ Then

shows that g m. It follows that m = 9+. (ii) Use part (i) and the relations [X^,, X_^] = -a^. (iii) If L = Lj _L L 2, then L(2) = L^d) V ¿>2(2). The subalgebra 9 ^; i = 1,2 of 9^ spanned by L^ and [X^\a g L f l ) ) is evidently isomorphic to g^., and it is clear that 9^ = 9 1 © 92 and [9^, 92] = (0). □

3.7

Constructing Lie Algebras from Lattices

287

Theorem 4 Let L be an even positive definite geometric lattice. Let L(2) be the set of elements of norm 2 in L, and let L be the sublattice o f L spanned by L(2). Let K be a field o f characteristic 0, and consider the Lie algebras g= K § = (K 02 where and are the Z~Lie algebras o f the lattices L and L . Let 5 be the centre of g. Then (i) g = 3 X (ii) 3 is the subspace o f K L orthogonal to K ^ respect to the invariant bilinear form o f given by Proposition 2. Moreover dim(3) = rank(L) - rank(L'),

and

[g ,g ] =

(iii) ^ is semisimple. I f L(2) = Aj V • • • V is the decomposition of L(2) into indecomposable root systems and L^ is the sublattice o f L generated by A^, then = IK 9/, is a simple Lie algebra and ^ X *** X In particular g is simple if and only if the root system L(2) is indecomposable and spans L. Proof Let I) = K

L. Then g = i) ©

© KX^ aeL(2)

is a triangular decomposition of g. Let X=a

a:

e

3, and write

^ x “, aeL(2)

where a and a:“ e By the way the multiplication in g is defined it is clear that all the ;c“ = 0 and that (ala) = 0 for all a e L(2). In other words, 3 c L' , where L'^ := (jc © f)l(A:|y) = 0 for all y © L'}. Conversely, it is clear that L' c 3, so we have 3 = L' - rank(L') = rank(L) —rank(L'). Moreover g = 3 ® (K 02 L') © and since [3, §] = (0), we have g = 3 X

and dim(3) = dim()^)

= 3®

288

Lattices and Finite Root Systems

From Proposition 3, ^ X ••• X Suppose that we know that each is simple. Then, since 3 = (0) ^ L = L', g is simple if and only if L = L' and L(2) is indecomposable. To finish the proof of the theorem, we prove that each is simple. For this we may assume that L is generated by L(2), that L(2) is indecompos­ able, and that g = § = Let a be a nonzero ideal in We begin by showing that a n L # 0. As above, let ]^ = IK 02 Then a is an 1^-module by the adjoint representation and hence is a sum of 1^-weight spaces (Proposition 2.1.1). The weight spaces of § are f) and the one-dimensional spaces KX^, a ^ L(2). If e a, then [X_^, X^] = a e a. Thus in all cases a n L ¥= 0. Let {«1, . . . , a/} be a base of L(2), and let 0 9^= g a n L. Then for at least one ¿, (j8|a^) 0, and we have [X^,,p] = -(a^\IB)X^, e a. Thus suc­ cessively X^,, X^], and X_^_ = a-]/2 lie in a. The argu­ ment can be repeated to deduce that X^,, aj, X_^. are in a if (aj\a^) 4^ 0, that is, if «y and are joined by an edge in the Coxeter-Dynkin diagram. Since L(2) is indecomposable, the Coxeter-Dynkin diagram is connected (Proposition 3.4.4) and hence all the X lie in a. By Proposition 3, a = ^. □

Remark 1 We have shown that the Lie algebras of type Ai, Di, F7, and £g over fields of characteristic 0 are simple. It is not hard to consider­ ably relax the restriction on the characteristic. In the light of Proposition 3, we have a set of Lie algebra generators of which arise from a choice of a base for the underlying root system L(2). There is obviously something rather special about this since we know that bases of L(2) are all conjugate by the Weyl group W, In the next section, where we look at the way in which the sign problem is solved, we will also see that W lifts (in a slightly subtle way) to a group of automorphisms of g^. These automorphisms take a given set of generators into some other sets {±X^^^J, w ^ W, showing that all the generating sets obtained in choosing a base of L(2) are essentially alike. This means that any relations that we find amongst the are essentially invariants of the algebra (relative to L). Let L be an even positive definite geometric lattice which is generated by L(2). Let {«1, . . . , a/} be a base of L(2), and let A = (A^j) be the Cartan matrix of L(2): A^j = (ajay). Set

( 10 )

fi

a/’

^

1, . . . ,/.

Then we easily have (11)

[hi,ej] =Aji€j, [ h i , f j ]

=

[ci, fj] =

- A j i f j ,

for all I, y e ( 1, . . . ,

.

3.8

Central Extensions of Lattices

289

Now consider i * j. If = (ay|a,) = 0, then a, + i A and = 0. If = - 1, then a^ + aj e A, but 2a, + aj i A, so [e,,[c,, e^]] = 0. Since these are the only possibilities, we obtain ( 12 )

(ade,.)

= 0

for all i

j,

(a d /,)-^ " " V , = 0

for all i

j.

and similarly

The relations (11) and (12) provide the correct starting point for constructing a far more general class of Lie algebras. This is the subject of Chapter 4. The apparently unnatural ordering of the indices which appears in (11) and (12) is chosen to conform with this more general setting. Of course it is immaterial here, since A^j = Aj^.

3.8

CENTRAL EXTENSIONS OF LATTICES

Let L be an abelian group, and let be a central extension of L by a (necessarily abelian) group A. By definition this means that we have an exact sequence of groups ( 1)

0

0

and that i{A) lies in the center of . It is convenient to adopt additive notation for L and A and multiplicative notation for (which will not be abelian in general). Let (f>: L ^ be a section of L in L " , that is, an arbitrary mapping satisfying tt • (¡>= id^. For convenience we assume that <^(0) = 1. Then every element of L" is uniquely expressible as for some a ^ L and a E: A. When the maps (j>and i are understood, we will sometimes, for convenience, write (a, a) instead of Given a central extension L" of L by yl, as above, and a section of (f) of L in L ^, we define a mapping e: L X L

>A

by

[This definition makes sense, since i is injective and (a + p)~^(f>(a)(f>(p) e ker(7r) = i{A).] If our central extension is fixed, then the map s depends on the choice of section (f>. Later in this section we will discuss this dependence

290

Lattices and Finite Root Systems

in more detail. Notice that

( a , a ) ( ^ , b ) = (a)i(a)(p)i(b) = (a)4>(P)i(a)i(b) =
( a , a ) ( ^ , b ) = {a + p , e { a , p ) + a + b),

and therefore s allows us to understand the structure of L ^ in terms of that of A and L. It is a straightforward consequence of the associative law that s satisfies the condition (3) e(a -h p , y ) + e (a ,

= e ( a ,)8 + y)

s(P,y)

for all a, p , y G L.

A map e: L X L ^ A satisfying condition (3) is called a 2-cocycle on L with values in A. One knows (see [Ja2], Chapter 6 [Ro]) that any such map can be used to make the set L X ^ into a group by using (2) as multiplica­ tion; moreover the resulting group L " is then a central extension of L by A. A simple way to obtain a 2-cocycle is to take any biadditive mapping s: L X L -> A. Then e{a p , y ) = e(a, y) + y) and e(a, /3 + y) = s(a, p) + s(a, y) so that (3) trivially holds, and one can easily see how the above construction makes into a central extension of L by We are interested in the case A = Z/2Z. For our purposes it is enough to assume that e is bilinear (this is in fact not a restriction). Then e(2a, j8) = 0 = e(a, 20) for all a, p ^ L, so s determines a bilinear form e: L / 2 L

X

L/2L —

Conversely, any bilinear form s on L / 2 L lifts uniquely to a Z-bilinear mapping on L with values in Z/2Z. At this point we introduce quadratic forms over the field F2 == Z/2Z. This theory was originally worked out by Chevalley [Chi]. The principal thing to be aware of here is that the usual relationship between quadratic forms and symmetric bilinear forms is no longer valid. Instead we have a relationship of quadratic forms to alternating forms and arbitrary bilinear forms to quadratic forms. Let K be a vector space over F2. A mapping q:V

F.

is called a quadratic form on V if the associated mapping b : V x V ---- > F,

3.8

Central Extensions of Lattices

291

defined by (^)

+



—^ (y )

is bilinear. It is evidently symmetric. Furthermore 0 = ¿ ( 0, 0) = q(0) + g (0) + ^ (0) = > q{0) = 0, whence b(x, x) = qix) + qix) = 0 for all x, and hence b is alternating. The set Q(V) of all quadratic forms on V is also a vector space over F2 if we use pointwise addition of functions. Let B(V) denote the vector space of all bilinear maps on V, and let denote the subspace of alternating bilinear forms b on V. Obviously the bilinear forms in B%V) are symmetric. By definition we have a linear map II : 0 ( F ) ~ ^ B \ V ) ,

which attaches to a quadratic form its associated bilinear form. Notice that II (q) = 0 if and only if ^ is a linear map (linear maps are quadratic forms). A quadratic form is entirely determined by knowing the values q(xi) and b{Xi, Xj) on a basis {x,}, s j of F. In fact this follows simply from the identity q( x + y ) = q ( x ) + q{y) + b { x , y ) . Given any bilinear form s on F, we may define a quadratic form q^ by = e{x,x) thus establishing a linear map □: B ( V ) ---- > 0 ( F ) with kernel precisely B%V). The associated bilinear form of q^ is b^, where be(x, y) = s{x, y) + e{y, x).

(5)

In the next result we put this backwards: Given a quadratic form q, find a bilinear form e such that q = q^Proposition I

(i) 0 ^ B%V)

B(V)

0 (F )

0 is an exact sequence-,

(ii) if dim(F) = «<<», then dim B%V)

|

Proof Let q G 0 (F ). Let {x,|i e J} be a basis for F over F2, where J is some well-ordered set. We define s by establishing values for £(x„ X j ) for all

292

Lattices and Finite Root Systems

/, j e J. Choose six^, Xj), i < j\ arbitrarily and define e(xj, Xi) = b(Xi, Xj) + s(Xi, Xj)

for / <j,

where b is the bilinear form associated with q. This is forced by (5). Finally, define e(x,,jc,) =q(Xi). Consider the quadratic form defined by e. It agrees with q on the x^ and its associated bilinear form, given by (5), agrees with b on the basis {;cJ. Thus q^ = q, and q ( x) = s{x, x)

for all x ^ V,

Obviously, if card(J) = n, then there are 2( 2) choices for the bilinear form s.

We now turn to the problem that was left unresolved in Section 3.7: to determine a cocycle for a geometric lattice (L,(*| • )) that satisfies equations (3.7.3) and (3.7.4). Proposition 2 Let L be an even geometric lattice. Then there exists a central extension L" of L by Z/2Z with cocycle s : L X L ^ Z/2Z satisfying (i) e(a, j8) + s(p, a) = (a|j8) mod 2 (ii) s(a,a) = I (a |a ) mod 2 for all a, p ^ L. Proof Let L = L /2 L , and let : L L be the natural homomorphism. L is a vector space over F2 = Z/2Z. Define q :L

F.

by q{a) = ^(a\a) mod2. This is a quadratic form with associated bilinear form b ( a , p ) = (a\p) mod2. By the last proposition there is a bilinear form e: L X L q(a ) = s(a, a)

for all a ^ L,

F2 such that

3.8

293

Central Extensions of Lattices

and we know that (6)

e (a , P) + e()8, a ) = ¿ ( a , jS) = (a|/3) mod 2, and

(7)

e ( a , a ) = j( a \ a ) mod2.

Finally define e: L X L ^ Z/2Z by s(a, p) = e(a, $),



Remark 1 In order to avoid a lot of cuml^rsome notation we will often omit the overbars in symbols like q{a), b(a, p) writing simply q(a), b(a, p), and so on instead. Remark 2 The proof of Proposition 2 can be used, with only minor modification, to show that for every quadratic form q on L / 2 L there is a 2-cocycle e on L with values in Z/2Z such that e(a, a) = q{a) for all a. The second cohomology group H \ L / 2 L , Z / 2 Z ) of L / 2 L and the space Q of quadratic forms in L /2L are isomorphic as groups. The construction of L" leaves open the question of uniqueness, since there are many choices for a cocycle satisfying condition (7). To establish the fact that L" is unique up to isomorphism, we need Proposition 3. Proposition 3 Let V be a vector space over F2, and let b be any alternating bilinear form on V, Let B = {x^\i E: J } be a basis of V , and for each i e J let c, e F 2 be arbitrary. Then there is a unique quadratic form q on V such that (i) the bilinear form associated to q is b (ii) q(xi) = Ci for all i e J. In particular we have 0 --------

'B(V)

Q(y)

where the kernel of I1 is F* as noted above. Proof We can assume that J is totally ordered. If q exists, it must satisfy (8)

q{x + y ) = q{x) + q{y) + b { x , y ) .

As a consequence, if {w^,. . . , have (9)

is any subset of the basis B, then we must

«(«iMi + ••• +a„M„) =

“y) i<j

for all a-^,,,,,a^

e

F2.

294

Lattices and Finite Root Systems

Use (9) and the conditions qix^) = c, to define q on V. It is straightfor­ ward to show that it is a quadratic form satisfying (8). □ Now let us suppose that s and e' are two cocycles on L satisfying the hypotheses set down in Proposition 2. Let the bilinear mapping 6 on L be defined by 6( a , )8) = e (a , jS) + e '(a , )8)

for all a , )8 e L.

Then & (a ,a )

= e(a ,a )

e'(a,a)

= |( a |a ) + ^(ci\a) = 0 mod2. Thus b is alternating and by Proposition 3 there is a quadratic form u on L satisfying u(a + jS) + u(a) + u(p ) = b(a, p)

for all a, ¡3 ^ L.

Write this in the form ( 10)

s'{a,P) + u(a + )8) = s ( a , ^ ) + u{a) + w(jS).

Use s to define the group structure on L ^ = L X (Z/2Z); that is ( a , a ) ( p , b ) = {a + p , e { a

p) + a + ¿).

Define (!>': L by (f)'(a) = ( a , u { a ) ) . This section gives rise to another cocycle s" of L. Assuming that the extension group Z/2Z is identified as a subgroup of L "" in the obvious way, then s" is defined through

3.8

Central Extensions of Lattices

295

But

= ( a + ^ , s { a , p ) + u{a) + u(l3)) = ( a + ^ , s '( a , )8) + w(a + /3)) = '(a + p ) s ' ( a , p ) . Thus e" = s'. In other words, e' is a cocycle on L arising from some other section of L in L ^. Alternatively, the group extensions and L'^deter­ mined by e and s' are isomorphic: We use the set L X (Z/2Z) and the corresponding group laws given by (2). The mapping 0 : L" L'^defined by (a, a) ^ (a, u(a) + a) is an isomorphism, and we have the commutative diagram

( 11)

Proposition 4 Let L be an even geometric lattice. Up to isomorphism o f the type given by (11); the extension o f L by Z/2Z given in Proposition 2 is unique. □ Let L = ® j^ j Z a j be a free abelian group, and let 0 ---- > Z/2Z

L"

L ---- > 0

be a central extension of L by Z/2Z. Fix a section of L in L ", and let e: L X L ^ Z/2Z be the corresponding cocycle. Define z ^ L " by z *•= /(1) where 1 •= l(mod2) g Z/2Z. Then z^ = 1, and if we adopt the notation e" for (f>{a\ every element of L'" can uniquely be written in the form e“z", where a ^ L and n g Z/2Z. The multiplication of is now given by [see (2)]

( 12 )

_ ^oc+fi^eia,P)+n+m

Let J? be a commutative ring, and let /?[L"] be the group algebra of L" over R. Thus /?[L^] is a free i?-module admitting the set {e“z"|a g L, n G Z/2Z} as a basis and has multiplication given by bilinear extension of

296

Lattices and Finite Root Systems

(12). Consider next the free submodule j of i?[L"] defined by ;■= © a^L

+ e“z)

(the sum is direct since the terms e" + by assumption). By (12) we have ( e ^

+

e ^ z ) e ^ z ^

are linearly independent over R

_|_ ^ a + / 3 ^ e ( a , / 3 ) + H - n

=

= e"^^(l + z ) =

+ e^-^^z e j,

showing that j is a right ideal of A similar argument shows that j is also a left ideal (recall that z is in the center of L ") and hence that j is two sided. Because 1 + z = + e^z, it is immediate that j is generated by the single central element 1 + z. Consider the .R-module homomorphism f:R [L ^]^R [L ] of i?[L"] into the group algebra /?[L] of L (Section 2.5) defined by / : e“z"

e^(-iy.

This map is surjective, and its kernel is precisely j. Hence R[L^]/j == R[L] as i?-modules. The multiplication of the quotient algebra R[ L^]/j induces, via this isomorphism, a new multiplication on R[L]. We denote the resulting algebra by R[LY , and call it the twisted group algebra of L (by the cocycle e; see Borcherds [Bel]). Explicitly R[LY is a free /^-module admitting the family {e“|a e L} as a basis and has multiplication satisfying the identity (13) Evidently f?[L] (with its usual algebra structure) is not in general isomor­ phic to since R[L]' need not be commutative. Let L" be the central extension of L with a cocycle e determined by Proposition 2. Let e Aut(L). We will show that there is an automorphism " of L " (as a group) that stabilizes the central subgroup Z/2Z in L^ and that induces on L. We begin by considering the cocycle on L defined by £*^(«,/3) = e((a),{P))

for all a,f3 ^ L .

3.8

Central Extensions of Lattices

297

Since e * ( a , ^ ) + e'^{p,a) = e{(^)) + = ({a)\ on L by b (a,/3 ) = s { a ,P ) + £"^(«,/3), just as we did above, with b(a, a) = 0 mod 2 for all a. Let u be a quadratic form satisfying (14)

u{a + /3) + « (a ) + m( j8) = b ( a , p ) .

Define '' [in the notation of (12)] by (15)

^>"(£“7") =

We have '{e“z ‘’e'^z‘’) = = ^(a) + {p)^uia) + u ( ^ ) + b ( a , ^ ) + e ( a , P ) + a + b ^

g<^(a)+a>(P)^«(a) +u(£) +£*<“•

_

^ 4 > ( a ) ^ u ( a ) + a^((3)^u(P) + b

= ^{z )= z. Thus ^ is an automorphism of L" fixing z. Evidently ^ lifts on L. Lemma 5 (i) Every lifting o f an automorphism ^ and iff^ are liftings o f (j> and if/ with quadratic forms u and v, then is a lifting o f il/(f> with quadratic form u + v.

298

Lattices and Finite Root Systems

Proof. Begin with the case ф = 1. Let ф" be any lifting of ф. Then

for some Л: L F2. From (12) we see that Л is Z-linear. Now recall that linear maps are quadratic forms, and with и replaced by Л and b replaced by e Hequation (14) is satisfied. This proves part (i) when ф = 1. Now suppose that ф ^ and ф^ are as in part (ii). Then ф^ф"{е^г^) = _

^фф(а)^иф(а) + и(а) + а ^

which is what we wanted to show. Finally to finish part (i) in general, let ф" be any lifting of e Aut(L). Let ф^ be 2i lifting of ф given by a quadratic form u. Then (o^ = ф^ lifts 1 and so is given through some linear map Л, as above. Then ф" = ф"о)^ is given through the quadratic form Л + w by part (ii). □ Define Auto(L") to be the group of all automorphisms of L" that fix z. Each ф^ ^ Auto(L) determines an automorphism of L, and we have an exact sequence (16)

1 ---- --------- > A uto(L^) ---- > A ut(L) ---- ^ 1,

where К is the subgroup of elements of Auto(L^) inducing 1 on L. Proposition 6 к = (L/2L)* {the dual space of L /2 L ) via the map Л •-> Л" for all Z-linear maps Л: L ---- > F2, where A^(c“z^) =

Proof The mappings A" are indeed automorphisms of fixing z, and the proof of Lemma 5 shows that every lifting of 1 e Aut(L) is of this form. From part ii of the lemma, A^ = (/i + A)" for all /x, A e L. □ To obtain results about the automorphisms of the corresponding Lie algebra 9^, we apply the above results on automorphisms to the special case when L is a positive-definite geometric lattice. We will assume that L " is the extension of L given by a cocycle e satisfying the thesis of Proposition 2. We return to the ordered pair notation (a, a) for elements of L '".

3.8

Central Extensions of Lattices

299

Let (l>^ ^ Auto(L^), and let denote the automorphism of L induced by (¡>^, We know that for some quadratic form u, (f>"(a,a) = {(l>(a),u{a) + a) where, for & = e + u satisfies (14). Let = L 0 ®aeL(2)^'^a the Z-Lie algebra of the lattice L, as constructed above, and define an endomor­ phism of g^^ through

= Let us verify that ^ G L, then

a e L (2 ).

is an automorphism of g^. Indeed, if a e L(2) and

= ( - ! ) “<“>( while if a, ^ G L(2) then fO

i f ( a |^ ) > 0 ,

-<^(o)

if («1/3) - - 2 ,

and

iO

if{(a)\(p))>0,

if(<^(a)|«^(/3)) = - 2 . We see that "([X^, X^]) = ["(Xj,"iX^)] by taking into consideration the following facts: .

( a |/3 )

=

(< ^(a)l< f>(i3))

and

(a + P) = (f>(a) +

300

Lattices and Finite Root Systems

• From (14), u(a + /3) + e(a,IB) =

u (a )

+ m( j8) +

b ( a ,P )

e(a,/3)

+

= u{a) + m(/3) + e(a,l3) +

+ e(a,/3)

= uia) + u(p) + ei<j>(a),HP))-

♦ if (a |^ ) = —2 then j8 = —a and hence (16)

m( “ )

Suppose next that <(>'' and

+ m()S) = 0. e Auto(L^), and write

4>"(a,a) = { ^ ( a ) , u { a ) + a), i/r"(a,a) = (tl /(a),v(a) + a).

Then by Lemma 5 il>"4>"(a,a) =

, {u + v
Therefore for all a e A, (u+v4>Xoi) ^

(«)•

On the other hand,

= (-l)

(u+vXa)

X.

Thus we have established the existence of a natural homomorphism 4> of Auto(L^) into the group Aut(g^, L) of automorphisms of g stabilizing L (see Section 2.1). Proposition 7

If L(2) generates L, then AutoCL"") - Aut(g^, L) under the mapping i>. Proof If e Auto(L") determines the identity automorphism of g^, then (f> induces 1 on L, and hence the quadratic form determined by is a linear

3.8

301

Central Extensions of Lattices

mapping A by Proposition 6 and (16). Since A van­ ishes on L(2) and hence on L. From (15) we see that (f>" = 1 and hence that is injective. Now let e Aut(g^, L). Then by restriction r¡^ determines a (group) automorphism of L. By IK-linear extension of ry" we obtain an automor­ phism of IK ® stabilizing IK <8>L. Extend (*| * ) to a IK-bilinear form on K 0 L. Recall that K 0 g^ has a triangular decomposition with root spaces K0 corresponding to the roots a: h ^ (a\h) (see Section 3.7). By Proposition 2.1.3, 7]^ determines an endomorhism * of (IK 0 L)*, which permutes the roots. Using ( 1 ) to identify IK 0 L and (IK 0 L)*, we may view *(a) where

e IK^ (actually

foT 3.11 a e L(2),

e {1, —1}). Now we have

(Q^ I^ )^ /3 ^ < /> *( /3 ) “

'*7^ ([<^5 ^ / 3 ] )

~

['*7^ ( ^ ) j

= a^(*(^))AT^*(^), from which (17)

(a\p) = ((a)\*{p))

for all

L(2).

On the other hand, the equation V - { [ X , , X p ] ) = [r,-X^,v-Xp] together with the definition of multiplication on g^ leads directly to (18)

(a\p) = (^(a)\cl>*(p))

fo ra lla ,i8 g L (2).

Since L(2) generates L, (17) and (18) give = 0

and

(i> eA u t(L ).

Let denote both a lifting of 4> to Auto(L") and the corresponding automorphism of g stabilizing L. Then ¡1" :=" “ ^77" e Aut(g^, L) and pointwise fixes L. Let { aj,. . . , a„} be a base for L(2). Then = c¿X^,, where c¿= ±1. Let A: L F2 be the unique linear mapping defined by Ci = ( - 1)'^^"'^ Using Proposition 6, we may lift A to A" ^ K and replace is surjective. □

302

Lattices and Finite Root Systems

Remark 3 As an important application of these last two propositions we consider the Weyl group W of L. We assume that L is positive definite and that L(2) generates L. Then, since W c Aut(L), by (16) and Proposition 6, W has a preimage W" in Auto(T"), which is a 2*^^"*^^-fold cover of W. According to Proposition 7, W" may be identified with a group of automor­ phisms of stabilizing L. If w" e and w" ^ w then (19)

W^\l = W,

and for all roots a, ( 20)

= ±X ^^.

The group W is sometimes called the Demazure-Tits group. For more on its structure, see [MPS].

EXERCISES 3.1 Let 6i,

be the standard basis for /-dimensional euclidean space

(a)

Show that {±e, ± Sj\i j} U { ± e j is a root system of type and that {±e^ ± Sj\i # /} U {±2eJ is a root system of type Q (see Sections 3.1,3.3,3.4). (b) Show that the Weyl groups of these root systems are isomorphic to Si tx (Z/2Zy. (Interpret this as all permutations and sign changes of the e/s.) (c) Consider the root system {±Si ± 6j\l < i, j <1, i ^ j) of type D/ (Sections 3.1,3.3). ( i) Prove that the long roots of Bi and the short roots of C / form root systems of type (ii) Prove that the Weyl group of Di is isomorphic to 5/ K (Z/2Zy~^, (Interpret this as all the permutations and even number of sign changes of the e/s.) (d) Show that the set {±£, ± £y|l ^ i, j < 4, i ¥=j} U {^{ ±£i ± £2 ± ^3 ± «4} u (± £ ,|l < i < 4}}

(e)

is a root system of type F^. Show that both the sets of short and long roots of form a root systems of type D^. Let A be a root system of type D^, Show, by looking at the Coxeter Dynkin diagram, that [Aut(A): W(A)] = 6. Show that Aut(A) is isomorphic to the Weyl group of type F4.

Exercises

303

3.2 Compute the determinants of the root lattices of types Bi, Ci, and G2. 3.3 Let A be a finite indecomposable reduced root system. Let II = {ai,. . . , a/} be a basis of A. Show that there exists a unique short root in A of maximal height (with respect to II). Show that if = then p is dominant, and hence all c, > 0. p is called the highest short root of A. Compute this root for A of type G2, F4, Bi, and C/. 3.4 Let A be a finite indecomposable reduced root system of rank / on a K-space V. Let II = { aj,. . . , a j be a base of A. Let A^ be the dual root system and II [a^ , . . . , a /} the base of A^ dual to II. Recall the root and coroot lattices Ô == E 2 a = 0 Za, c V, ae A

^= 1

Q ''= E 2 aeA (a)

a

I © Za^cz V * . ^'=1

Let P^:= [y e F*|<jt:,y> e Z for all x ^ Q ) and P := [ x ^ K|<x,y> e Z for all y e

c K.

Show that P (resp. is a lattice in F* (resp. V) (called the weight and coweight lattice respectively). (b) Show that Q P and that the group P /Q is finite (the order of this group is called the index of connection of A. The cosets (o Q, (0 ^ P, are called the congruence classes). (c) Let (o^,. . . , (Oi ^ P be defined by a ^ ) = 8^j. (The co/s are called fundamental weights. They form a basis of P dual to the basis of (2^.) Given a, e II, show that Oii where A = (-^¿P is the Cartan matrix of A. (d) Show that the index of connection of A equals det(^). (e) Let W be the Weyl group of A. Show that W stabilizes P, thereby acting as automorphisms of P. Show that W acts trivially on P/Q,

304

Lattices and Finite Root Systems

(f)

Compute P / Q and the congruence classes for all indecomposable reduced root systems A.

3.5 Let A c K be a reduced finite root system of rank /, and let II = be a basis of A. Let Q and P be the root and weight lattices. (See Exercise 3.4.) (a) Let Z[P] be the integral group algebra of P. Show that Z[F] has no zero divisors. (b) Let W be the Weyl group of A. Then W acts as a group of automorphisms of Z[P] via w' • E n^e{ii) = ^ n^e{wii.). fX^P /i, sP

(c)

Let Z[P]^ := {jc e Z[P]\wx = x for all w e W}. Let K' and K denote the field of fractions of Z[P] and Z[P]^, respectively. Show that Z[P] is the integral closure of Z[P]^ in K' and that K' is a Galois extension of K with Galois group canonically isomorphic to W. Fix iV e Z+, and let ^ e C. Fix z* e 0 and define ring homomorphisms

by

and by restriction f:Z {P T Let p' = k e r/', p = k e r/, k' = field of fractions of Z[P]/p', and k = field of fractions of Z [F ]^/p. Show that k' is a Galois extension of k with Galois group canonically isomorphic to Wd/ W j , where Wo = { w ^ W \ w V ' = X>'), Wj = [w e W\wx = X mod p' for all x e Z [F ]} . Let i := {/i e

z*) = 0 mod N). Show that

IV^ = {w ^ W\w\ = i}, W[ = [w ^ W\wii. = fi mod i for all

/j,

e P }.

Exercises

305

3.6 Consider a connected affine Dynkin diagram F with nodes / e { 0 ,..., and marks rii. We play a “game” on F as follows: Step 0: Pick a node (starting node). Step 1: Remove the last node j you picked, and let Fy be the diagram left over (y = if you are starting). Step 2: Compute the determinant of the root lattice with diagram Tj. If Dj = rij, you may continue playing the game. Otherwise, stop: You’ve lost the game. Step 3: Pick a node connected to the last node you removed. If you cannot do this, you have finished playing a winning game. Otherwise, return to Step 1 and keep playing. Show that in the only diagram all of whose games (24 of them) are winning games. 3.7 (J. Milnor and D. Husemoller, Symmetric Bilinear Forms, SpringerVerlag, 1973). In this exercise we construct the famous Leech lattice: the unique positive-definite even unimodular lattice of dimension 24 with no lattice points of square length 2. Let F2 = {0,1} be the field with two elements. For N define §0 := (1 < i < N\Si = 0} = {1 < i < N \S i = 1}. Let V = (i^i)o^i^io = (1, h 1,0,1,1,0,1,0,0,0) e 11 square matrix A = (a^j) with entries in F2 by aij := i^(/+y-2)modll

for all 1 <

Define an 11 X

j < 11.

The 11 rows of this matrix we will denote by a^ ,. . . , Let |5| denote the cardinality of an arbitrary set S, (a) Show that \a] n a]\ = 3 for all 1 < i < j < 11. (b) Fix S c { 1 ,..., 11}. Let s(5) = s = ^ F2^ where by con­ vention s = 0 if 5 = 0 . Show that |s^| = 0 mod 2 and that for all j € S, |s^ n aj\ - |s^ n aj\ = 0, ± 4 if |5| is odd and = ±2, ± 6 if |5| is even.

306

Lattices and Finite Root Systems

(c)

Let B = (bn) be the 12 X 12 square matrix defined by 0 1 B ■■= 1

1 1

• •

1

A

1 Show that any two distinct rows of B are orthogonal and that B^ = I. (d) Let C be 12 X 24 matrix obtained by gluing together I and B

C ■■=

/1 0

1

0 0 B 1

,0

t

and let 7 1 , , 712 ^ be the rows of C. Show that I7/I = 8,12 for all 1 < I < 12. Show that any two distinct rows of C are orthogonal. (e) Let S c F|‘* be the span of the rows of C. Show that (i) (1 ,1 ,...,1 ) g 5, (ii) Is^l = 0 mod 4 for all s G S, (iii) |s^| > 8 for all s G 5 \ {0}, (iv) dim,:^ 5 = 12. (f) Let L q c be a lattice with an orthogonal basis (b,)i^is24 satisfying b, • b, = i- Define two subsets E and I of L q as follows. 24

^

{L U= i • i/ ^ 2Z,

such that for all 1 < / < 24,

24



= 0 mods, i=\ mod 2 , .. ., 1^24 niod 2) e S.

/ = I 51 tib}j such that for all 1 < / < 24, •

^ 2Z + 1, 24

• 51 ^ - 4 mods, /=1 • { j( t i + 1) m od2,. . . , ^(^24 + 1) mod2) e 5.

307

Exercises

We define the Leech lattice L by L = £ U / c L q.

Show that if jc = ^ L, then 'Ltf = 0 mod 16. Use this to show that L is an even integral lattice. (h) Show that [L qI L] = 2^^. (i) Let

(g)

M = {(^¿) e

= 0 mod 2 for all 1 < / < 24},

and let 0=

e

= OmodS^.

Show that [Mo: E] = 2^\ (j) Use (h) and (i) to show that L is unimodular. (k) Show that L has no vectors of square length 2. 3.8 Follow all the constructions of Section 3.7 to construct explicitly the Lie algebra of the root lattice of type Follow Section 3.8 to explicitly determine the cocycle needed for your construction. 3.9 Consider the root system of type Di A = [ ± s ^ ± sj\l < i, j < l , i ^ ;} and its base n

{a^,. . . ,

where —^2? • • • ?^ /- i ^ ^/-i ~ ^ ^i-i (a) Show that the automorphism cr: -> W which fixes 1
308

Lattices and Finite Root Systems

(d)

(e)

Show that the fixed points in of o- form a subalgebra I and that f is linearly spanned by the elements of S, the elements a = d, and the elements + X^, a ¥=a. For each define 6 ^ = 2 5 /(5 |5 ). Let a , /3,y e A , and suppose that a ^ a, ^ y = y. (0 Show that {X^ + X^, a d, -X _ ^ - X_^} is an ^l2-triplet. (ii) Show that [a + d,X^] = ( fla ^ )Z ^ , [y,\x,+x^] =

[a + d , X p + X^] =

+ x^).

(iii) Let fi

^ / —1 ^ /-1

^ a i_ i

=

^ /-1

^

f l —l

1, . . . , /

2,

a / _ i —a/ J

+

Prove that e^,. . . , ei_^, h^,. . . , hi_^, f ^ , . . . , fi_^ satisfy the relations (11) and (12) of Section 3.7 for the Cartan matrix

of the base [d^,. . . , a/_i) of 2. (f) Determine a triangular decomposition of I. (g) Let K be a field, and let = IK Show that the elements 10 1 0 h^, 1 0 /^ derived from (e) (iii) generate as a Lie algebra. 3.10 (This exercise will be used in the exercises of Ch. 6). Let T be a graph that is a forest with vertices /}. Suppose that G is a group and that

is a mapping with the property that whenever i and j are not joined, /(/) and / ( ; ) commute. We wish to show that for all permutations tt of { ! ,..., /}, := /(7 t(1)) *• • f(7r(l)) lies in the same conjugacy class. (a) Consider / points (also labeled 1 ,..., /) placed uniformly in some order on a circle. Allowing only the rule that adjacent points i and j on the circle may be interchanged if / and j are not joined by an edge of F, show that (up to cyclic permutation) any ordering of the points 1 ,..., / may be obtained from any other. (b) Use (a) to prove that the conjugacy class of is independent of 77. 3.11 Prove Proposition 3.4.1

Chapter Four

Contragredient Lie Algebras T h e o p in io n s e e m s to h a v e g o t a b r o a d t h a t in a f e w y e a r s a l l th e g r e a t p h y s ic a l c o n s t a n t s w i l l h a v e b e e n a p p r o x i m a t e l y e s t im a t e d , a n d

th a t th e o n ly o c c u p a t io n

w h ic h w il l t h e n b e l e f t t o m e n o f s c i e n c e w i l l b e t o c a r r y o n t h e s e m e a s u r e m e n t s to a n o th e r p la c e

of

d e c im a ls . . . .

But

we

have

no

r ig h t

to

t h in k

th u s

of

th e

u n s e a r c h a b le r ic h e s o f c r e a t io n , o r th e u n t r ie d f e r t ilit y o f th o s e f r e s h m in d s in t o w h ic h t h e s e r i c h e s w i l l c o n t i n u e t o b e p o u r e d .

—James Clerk Maxwell, 1871, quoted from Abraham Pais (Oxford: Clarendon, 1991).

N ie ls

B o h r 's

T im e s ,

A contragredient Lie Algebra is, roughly speaking, a Lie algebra g, with a triangular decomposition S^, that is generated by the diagonal algebra if and subalgebras ^ l 2\ j ^ J, each isomorphic to êl2(!K). The remaining chapters, beginning with this one, are devoted to the general structure of contragredi­ ent Lie Algebras and constitute the core of the book. Section 4.1 introduces the contragredient algebras and concentrates largely on the necessary and sufficient conditions for the subalgebras t>e “integrable” to actions of 5L2([K) as an automorphism of g. The concept of the Weyl group IV of a contragredient algebra arises naturally in this context, although a full discussion on the structure of W is the subject of Chapter 5. Every contragredient algebra has an associated structure matrix A = {A^jX i, j, e J that plays a similar role to the Cartan matrix of Chapter 3. Using a relaxed version of the conditions CM of Section 3.3, namely CM1-CM3, we prove the basic result that a radical free contragredient algebra is integrable if and only if its structure matrix is a Cartan matrix. Section 4.2 is devoted to the existence of contragredient algebras with a given structure matrix A. The construction proceeds by first constructing a suitable diagonal subalgebra i) (a realization of and then by constructing a universal contragredient algebra u around which has A as its structure matrix. If y4 is a Cartan matrix, then u/rad(u) is integrable, thereby proving the existence of integrable contragredient algebras. There are a number of things about embeddings, field extensions, radicals, and decomposability

309

Contragredient Lie Algebras

310

which are rather obvious but nonetheless need to be written down. These make up Section 4.3. A very important class of contragredient algebras consists of the invariant (or symmetrizable) contragredient algebras, those carrying a (proper) invari­ ant bilinear form. Such a form can exist only if the structure matrix of g is symmetrizable (a generalization of symmetric). After establishing this, the remainder of Section 4.4 is devoted to showing the converse of this result. This is a crucial fact since most of the subsequent development depends significantly on the existence of such forms. For instance, in this section we have the construction of Kac’s generalization of the (quadratic) Casimir operator. In reality this is a whole family of operators one for each module in the category ^ (g , ^ ) , with the property that and inter­ twine g-module maps from M to N, The construction of these operators is possible (as far as is known) only if g is radical free and invariant. The Casimir-Kac operator is used at critical points throughout the entire theory, mainly as a tool to keep track of the type of subquotient modules that can occur in modules from ^ (g , *^). Our first application of these operators appears in Section 4.6, where we prove the Gabber-Kac theorem. This gives information about the generators of rad(u), where u is the universal contragredient algebra of a symmetrizable structure matrix. An important consequence is that one obtains an explicit presentation for each integrable invariant contragredient algebra g (always assuming symmetrizability) and in fact concludes that integrable is equivalent to radical free. A slight modification of the Casimir-Kac operator gives us an operator F acting on g itself. In Section 4.7 we define F and use it to prove the remarkable fact that there exists a contragredient bilinear form on g, obtainable by a slight twist of the invariant bilinear form, that is positive definite on the nonzero root spaces of an integrable invariant contragredient algebra g over R. This leads to the existence of a hermitian contragredient form on g^, which is likewise positive definite on nonzero root spaces.

4.1

CONTRAGREDIENT L IE ALGEBRAS

Let g be a Lie algebra over a field K, We say that g is contragredient triangular or simply contragredient if there exists a triangular decomposition * ^ = (g + ,^ ,í2 + ,cr)o f g satisfying the following: CTl: If {«ylyej ^ is the given basis of according to the axiom of triangular decomposition TD4 of Section 2.1, then the Lie algebra 5/^^^ generated by g“^ and g““^ is isomorphic to ^12(1K). CT2: The elements of g“>, g"“^ j e J, and generate g (as a Lie algebra). CT3: The sum Eye 9“^] is direct.

4.1

311

Contragredíent Lie Algebras

If we wish to indicate the triangular decomposition relative to which g is contragredient, we refer to the contragredient Lie algebra or contragredient pair (g, S^). Let j G J. Using CTl and cr it is clear that dim g“> = dim g”“^ = 1. Let Ej G g“>, Fj G g~“/ be any nonzero elements. Then Hj ~ [Ej, Fj] ^ 0 (by CTl) and [Hj, Ej] = kjEj for some kj # 0. With Cj ■■=2 k J % , a/== I kJ^Hj, fj •■=Fj, we have an il2-triple for §1^^: ( 1)

[«;

2 e y , [tty , / y ]

2 / y , [^ y ,/ y ]

C ij •

There is no reason why aej should be /y, but we can easily alter a to have this happen. Indeed for each j e J, let crej = tjfj, tj e Then there exists an unique automorphism 0 of g such that Oej = iyey, = t-% e\if = id^. (see Section 2.1, Remark 2). Of course 0g“ = g" for all roots a. Set r = da. Then T is an antiautomorphism of g satisfying r\t) = id^. Furthermore T6j = 0iy/y = /y, r/y = = 6j. Thus by modifying the triangular decom­ position ^ by replacing a by r, we can assume at the outset that cr(ey) = fjJ e J. Note that = id from CT2. Henceforth we assume that for each j e J, Cy e g«^/y e g-->,

a /e i|

satisfy (1) and ( X l C j ^ f j .

We call such a choice of

Cp

a j, and /y a display of (g,

The display {cy, a j , /y}ye j is finite if J is finite. Remark 1 Let {cy, a / , /y}ye j and {e'p , //lye j Then there exists a family {^ylyej such that e '= t e

two displays of (g, S^).

f- =

Since a{e'j) = / / we obtain iy = ±1 for all j. In particular a / is unique, since it is the only element in [g“>, g““^] that has g“^ as a 2-eigenspace. We leave it as a simple exercise to show that if every element of IK has a square root then displays can always be found without altering a.

312

Contragredíent Lie Algebras

We define yej Remark 2 The assumption CT3 is extremely mild. In fact it is not used here at all. We retain it to avoid a certain awkwardness in the presentation, but it is straightforward to adjust the results appropriately in the case that the set {a/ly e J} is linearly dependent. In Chapter 5, when we consider general root systems, dependence relations are an important consideration. Proposition 1 Let (g, T) be contragredient, and let [ej, a j , Then

be a display.

(i) for all i e J, dim g“' = 1; (ii) g+ is generated by {ej\j e J} and g_ is generated by {fj\j e J} as Lie algebras; (iii) for all a ^ L \ {0}, dim g" is finite. Proof, (ii) Let g'+ denote the subalgebra of g generated by the e,, i e J, and g'_ the subalgebra of g generated by the /,, i e J. It suffices to show that 9' == g'_+ ^ + g'+ is a subalgebra of g. First, ad /i(g') c g' for all g is clear. Next it is easy to see that ad

, e ,J e ]^ + g'^.

for all A: > 1,

and hence ad /y(g'+) ^ il + 9'+the same way ad ey(g'_) c + g'_. This proves part (ii). Since [e,|,. . . , e,^] lies in gt^“o and g“' is spanned by e„ it is clear that dimgt^“' is finite. Using cr we complete part (iii). □ We next attach to (g,

a matrix A = (/1,^), An

by defining

= ( a ,- ,« / ) .

The matrix A is called the structure matrix corresponding to (g,T). The condition eJ = 2ei shows that An = 2

for all/.

Example 1 Let g be one of the Lie algebras of type A , £>, and E given in Section 3.7. Each of these is based on an even lattice L in which L(2) generates L and forms a finite root system. For each we have a base

4.1

n = {«1,. . . ,

Contragredient Lie Algebras

313

relative to which L(2) = L(2)+U L(2)_. We have g=

©

0 g“ = 0 g"“ © Í) © 0 g“, asU2) asi,(2)+ a^U2)^

the latter being a triangular decomposition of g. The spaces 9"“' + [9"''^ 9“^] + 9"^

j = 1, • • •, ^

are isomorphic to ^ Í 2ÍK) and collectively generate g as a Lie algebra. It follows that g is contragredient. The elements i^y>^y»/y}y=i,.defined in (3.7.10) form a display and the corresponding structure matrbc is the Cartan matrix A of L(2). Example 2 (§I2(IK)) (see the Appendix iT¡(lK) = < /o,/i> e $ ® <eo,ei> determines a triangular decomposition of ^l2(IK). The subalgebras = Kf¡ + Kh¡ + Ke¡,

j = 0,1,

are isomorphic to §I2(IK), from which we see that §I2(IK) is contragredient. The corresponding matrix is (-^

1

)'

We now define a very important group W (called the Weyl group) of linear automorphisms of As we will see, the Weyl group is closely related to the group Aut(g, ]^) of elementary automorphisms of g that stabilize if. Initially we use W to get a better idea of what the root system A looks like. Let j e J. Define 0: r by rji p ^ P - <j8, a ^ ) a j

for all P

and

by rjy : h ^ h — (aj, h ) a j

for all /2 e

It is easy to see that r,(ay) = - a ^ and that Vj pointwise fixes the hyperplane = {j8 e ]^*|<j8, = 0} of Thus rj is a reflection of f)* in aj

314

Contragredíent Líe Algebras

(Section 3.2). Similarly ry is a reflection of ^ in a / . In particular r / = id^*,

r / ^ = id^,

rj^G L ir),

r/e G L (^ ).

Notice that 0(

^ u



Thus rj stabilizes Q stabilizes

A^j ^ Z

for all / g J,

A

for all / g J.

e Z

The group W c GL(ij*) generated by those r, for which ad Cj is a locally nilpotent transformation of g is called the Weyl group of (g, T): W = (rj\j G J, ad Cj is locally nilpotent). Similarly we define the dual Weyl group GL{^),

W ^= {r^ I ;

G

J, ad

is locally nilpotent).

If none of the ad ej are locally nilpotent, then by convention W = {1} and W ^= {!}, where 1 denotes the identity map of the appropriate space. Remark 3 Both W and depend on (g, but not on the chosen display. The reason for asking that ad ej be nilpotent will become apparent as we move along. In the end we are going to be interested in the case when ad 6j is locally nilpotent for every j g J. Readers seeing this for the first time might like to assume this from the outset. Proposition 2 (i) W ^ and W are isomorphic groups, an explicit isomorphism being given by r,, j G J. (ii) I f these two groups are identified by the isomorphism in part (/), then (a , h) = { w{ a ),w { h) )

for all a

G

1^*,

G

1^, and w E:W.

4.1

Proof. Let ^ e 3.2.6). We have

315

Contragredient Lie Algebras

and /i e

Recall the inverse transpose (Proposition

= { ^ ,h ~ { a j,h )a f) = {l3 ~ { l 3 ,a ^ ) a j , h ) = { r j( ^ ) ,h )

fo r a ll/3 G f)*,

G f).

This shows that (ry^)* = rj and also shows that (2)

{ ^ , r / ( h ) ) = { r j ( p ) ,h )

fo ra ll^

Now it follows that fr/

V

Jk

J

= r,j \ . .. r ,Jk

and hence that (3)

(■ )* :W ''^W

is a (surjective) group homomorphism. Now consider the inverse transpose r* of rj, y

^^

Then for all t e 1^** and for all /3 e 1^*, (4)

{ P , r * i t ) ) ={ rj(P),t) ={l3,t-{aj,t)a^).

Here we have written the pairing of 1^* and 1^** as < • , • > : f|* X

^

IK

and have identified a f g 1^ as an element of 1^** via the canonical identifi­ cation of 1^ in 1^**. Thus (4) reads rr If. = r / , and we have a homomorphism (5)

W ^ W '^

Contragredíent Líe Algebras

316

given by VT

w* 1^

which is evidently the inverse of the homomorphism (3). (ii) This follows immediately from part (i) and equation (2). Proposition 3 Let t ^ K^, and let j e J. Assume that ad ej is a locally nilpotent endomor­ phism of g. Then (i) n^U) '= expad(iey)expad( —i~ypexpad(iey) is an {elementary) auto­ morphism of g stabilizing f); (ii) ny(i)li, = r /. Proof Since ad e^ is locally nilpotent so is ad aiej) = ad fj. Thus nj(t) is an automorphism of g (Proposition 1.5.3). Let Hj = { h ^ f i \ ( a j , h y = 0}. Since (oij, a j ) = 2,

and since [h, ej] = 0 = [/i, fj]

for all h e Hj,

we have \h ¡ =

1-

On the other hand, 0 (« /) =

ad(tey)exp ad( - 1~‘/ y ) ( a / - 2ie^)

= exp ad(ie^) ( - « / - 2iey) = —a¡ This shows that n^it) stabilizes 1^. Moreover let with W e H:. Then

e 1^, and write h = ka^ + h!

nj{t){h) = k a j h ! = h — { a j , h ) a j = r]'{h).

4.1

317

Contragredíent Lie Algebras

Proposition 4 Let w

and write w = rj . . . r j . Let

...,

e

be arbitrary. Then

(0 n = n{w) •= is an elementary automorphism o f g such that ng“ = g^“ for all a e A. Moreover n\\^ = w under the identification o f W with W ^\ (ii) ivA = A and dim g“ = dim g"^" for all o: e A; (iii) for j ^ J with ad Cj locally nilpotent and for all w El W, the elements of g"^“^ are diddocally nilpotent. Proof (i) We see that n stabilizes by Proposition 3, and hence by Propositions 2.1.3 and 2 above we obtain ng“ = g'^/i o*« = with n |^ = w, as desired. (ii) This follows from part (i). (iii) «(g“0 = g'^“^ and n is an automorphism. Since g“>= Ke^, g"^"> = IK/ie , and part (iii) is immediate. □ Of course the n{w) of Proposition 4 is far from unique for a given w. We come back to this point in detail in Chapter 6. Notice, however, that if n{w) and ri{w) are as above, then n{w\n'{w))~^ e K, where K c Aut(g, 1^) is as in the discussion following Proposition 2.1.3. Let (g, ^ ) be contragredient. A root « e A is said to be real if a = wa^ for some w EiW and some ; e J for which ad e^ is locally nilpotent. If a root is not real, then it is said to be imaginary. Set '’^A := (a e A I a is real}, '^A := A V"A, '■"A^:= A+n""A, '■"A_:= A_n''^A, ^■'”A^:= A+n^'”A, "'”A_:= A.n'^^A, n =={«;!;• e j } ,

n'^== { a / l / e J},

:= {«y I y G J, ad €j is locally nilpotent}, ‘11'^:=

I y G J, ad Cj is locally nilpotent}.

318

Contragredient Lie Algebras

Thus "A = w r W . We have

g= © 9“ ae A

0

9“ ©

0 g"" 0 ae"A_

0

0 g"" ® 0 9"* ae"^A+ aG''”A+

The root spaces g", a are relatively easy to understand. This is not so for the imaginary root spaces. Proposition 5 Let (g, r ) be contragredient, and let Wbe its Weyl group. Then with the above notation we have (i) (ii) (hi) (iv) (v) (vi)

Q a n A = {a, 0, —a) for all a e'^^A; dim g“ = 1 for all a e'^^A; ^"A = -""A ««¿"'"A = -"'"A; Wstabilizes '^^A/'”A^_, and ""A^= -""A_ and"'”A^= -'^A _; ^"n = nn^"A.

Proof (i) Let a e^'^A, and suppose that na ^ A for some n e Q^.. By assumption there exists aj and w ^ W such that w{na) = naj. Since W{A) = A, it follows that naj e A. Assume that nuj e A+c Q_^. Then by TD4 of Section 2.1, n e Z+. The space g"“> is generated by all expres­ sions of the form [ej^,...,ej^] with 0 J, A: 0 Z^_, and «y. + • • • +ay^ = noj (Proposition 1). It follows that k = n and that j) = j for all 1 < / < A:. Thus g"“>= (0) unless n = 1. If naj e A_ or if n e Q_, we reason in the same fashion. This proves (i). (ii) We know that dim g“>= 1 for all ; e J (Proposition 1). Since dim g“ = dim g"^“ for all a 0 A and w ^ W (Proposition 4) (ii) follows. (hi) Let a e'^^A. Choose w ^ W and aj e'^^II such that a = waj. Then - a = wrjOj e'^^A, showing that '^^A = -'^^A and hence that "'"A = - " ”A (since A = -A ).

4.1

Contragredient Lie Algebras

(iv) We have W C ^ ) Let us show that (6)

if aj

and hence that

319

='"’A, since M A ) = A.

^ n ,th e n rX A A { a;} ) = AA{«y}.

Indeed, since for all n e Q^, naj ^ A+\{ay}, we can establish (6) by reason­ ing as in (3.3.14). Now we want to show that +) Let a and let aj e '’^n. Then rja e'^'A and by (4.6) Vja e A+. Thus Vja e A^_n^'”A. It follows that ITa c (A +n^'”A) c^'^A^ which is what we want. Finally, WCA_) = 1^(-^‘'”A+) = -1TC'”A+) = -^■'”A^ = ''”A_. (v) The proof is obvious. (vi) Clear from part (iii) of Proposition 4. □ Example 3 {A, D, E) This continues Example 1. We have A = L(2) U {0}. Since A is finite, the set jo: + kaj I A: e Zj n A is finite for all a e A, ; e J. Thus ad and ad /y are nilpotent. Thus the Weyl group W (in the current context) is

and from the definition of each rj and Proposition 3.3.4, it is clear that W is precisely the Weyl group of the finite root system L(2). The same proposition shows that L(2) = ITIl ='^^A, and hence that "'"A = {0}. The action of W on = LK a^ = (]^*)* is precisely the transpose action discussed in Proposition 3.2.6. The role of the dual root system A^= {Wa^ | ; = 1 ,...,/} is made apparent below. Fix ay Then ad ey and ad/y are locally nilpotent, and we have already had occasion to see, exp(ad te^) and exp(ad i/y), i e IK are welldefined automorphisms of g. By Proposition 2.4.7 the representation == ^I2(IK) Ql(g) given by :X

ad X

gives rise to a representation ^<^>:5L2(IK) ^ A ut(g), satisfying ^ exp(adtó^),

(o

(]

?)

320

Contragredient Lie Algebras

We can interpret this as “integrating” the representation of representation. It is interesting to see that under 7t^^\ 0 - t -1

" ( ( ;

= nj(t)

to a group

:i(;

:il

fo ra lli e K ''

(see Proposition 2.4.7). We denote the group 7r^^^5L2(lK)) by that is,

or SL^{\

:= (exp ad tej,exp ad tfj U e 1K>. According to the way in which g decomposes into irreducible §I^2^^‘niodules under ad, S L f - 5L2(K) or - SL2(K)/{t ± 1} (see Proposition 2.4.9). The group generated by those exp ad te^ and exp ad tf¿, i e K, / e J for which ad and ad are locally nilpotent is called the adjoint group of g and is denoted by ^ad- There is much more to come on <Jad in Chapters 6 and 7. Proposition 6 Let (g, ^ ) be contragredient as above, and let a aj be such U that a = waj. Then

Let w

and

(i) the space := g“ 0 [g“,g "] 0 g “ is a three-dimensional subalgebra o f g isomorphic to ^I2(1K). (ii) The elements of and g~“ are locally ad-nilpotent, and the group SL^2 ^ := (exp ad e, exp ad / | e e g", / e g~“> is a subgroup o f isomorphic to SL2(K) or 5L2(IK)/ {± 1}. (iii) Either of the following properties characterizes the same unique ele­ ment ]^: (iiia) belongs to an 2-triplet of in other words, there exist ^a’fa ^ [ a ^ ,e „ ] = 2 e „ ,

[a'",/« ] = - 2 / ^ ,

[e^,fj= a'^;

(iiib) a ^ = wa^ {under the identification o f W with W ^). Proof By Proposition 4.1.4 there exists n = n{w) «9^ = 9*^^

for all /3 e A.

such that

4.1

Contragredient Lie Algebras

321

Thus 0 [g«y, g-«y] 0 g"«y)

which establishes part (i). Moreover, since n(g“>) = g", it follows that g" (and hence g““) consists of locally ad-nilpotent elements. This shows that is a well-defined subgroup of Aut(g). It is easy to verify that n(expad

= expad(njc)

wherever n e Aut(g) and x e g is locally ad-nilpotent. Thus = SL^^\ whence we have part (ii). From part (i) it follows that {ncj, n a j , n/y} is an ^l2-triplet for Since n\^ = w, the existence of having properties (iiia) and (iiib) follows by setting a^:= As for the uniqueness of we recall that g", g““, Ka ^ are the 1^-eigenspaces of 5/^"^ and that the space [g“, g““] has a unique element that can be extended to an ^ 12-triplet of ^ Remark 4 Let a and let w e IF and be such that a = waj. Let be the (unique) element defined in part (iii) of Proposition 6. Then a ^ = wa^, and this identity holds independently of the choice of w and aj above. We call the coroot of a. The set of coroots is denoted by Notice that from the definition it follows immediately that for all a e ""A and w e IF, {waY=w{a^) and that '’^A^c 2 ^ From [a^, e^] = 2e^ we clearly have = 2. Proposition 7 Let a e '^^A, and let

be its coroot. Then

(i) the reflection r^ E GL(i)*) deflned by

belongs to W: (ii) I f w ^ W and aj

are such that a = waj, then r^ = wrjW~^.

In particular r . = r,;

322

Contragredient Líe Algebras

(iii)

under the identification o f W with h

we have

= r^v, where for all

r^w :h ^ h — {a, h )a ^ . Proof Let w ^ W and Uj way. If e ]^*, we have

be such that a = waj. By Proposition 6,

wrjW~^p = w(^w~^fi - (w~^P,ay)aj^

= )8 - ( p , w a ^ ) a

(by part (ii) of Proposition 2)

= fi - <)8,a^>a which shows that r^ = wrjw~^. This establishes part (ii), and also part (i), since wrjw~^ e W. Finally, part (iii) follows from Proposition 2 (ii). □ We continue to assume that g is a contragredient Lie algebra. Proposition 8 Let A be the structure matrix o f g. Fix j e J. (i)

ad Cy is locally nilpotent if and only if for all i e J, / ^ ;, we have (ia) ^ , y e Z < o , (ib) dfj := (ad Cy)"^'^^e¿ = 0. (ii) I f ad Cy is locally nilpotent, then for all i ^ j, Aij = 0<=^ [e„ey] = 0, ^ , y = 0 = > ^ y , = 0.

(O f course, if ad e^ is also locally nilpotent, we obtain A^j = 0 - ^ y , = 0.) (iii) Properties (i) and (ii) hold if ej and c, are replaced by f andfi. Proof (i) Suppose that ad e^ is locally nilpotent. Since for each i e J, rja^ = —A^jUj e A, and since no root can have ‘'mixed signs,” ^¿y ^ whenever i ^ j. Furthermore + (1 “ ^ i j ) ^ j ) = «<• - «y Í A which shows that

4.1

Contragredient Lie Algebras

323

Conversely suppose that for all i ¥=j, e Z < q and (ad = 0. Note that (ad = 0 for all i and (ad ejYh = 0 for all /z e 1^. Now set a = |jc G g I(ad

= 0 for some rij{x) e l\l|.

It is straightforward to prove that a is a subalgebra of g. Since a contains a set of generators of g (see CT2) we have a = g. (ii) Suppose that ad ej is locally nilpotent and that A¿j = 0. Then (ad ej)e¿ = 0 by part (ib), and we have ^ji^J = [«."'>«;■] =

= 0

by the Jacobi identity. Thus Aj¿ = 0. This last argument works equally well to show that [e¿, ej] = 0 =>A¿j = 0, thus finishing the proof of part (ii). □ A contragredient Lie algebra (g, y ) is called integrable (relative to if for some (hence any) display {ej, a^, ad 6j (hence, using the involution (7, also ad fj) is locally nilpotentfor every j g J. Example 4 The Lie algebras A, D, E and §I2(IK) are integrable.For an integrable contragredient Lie algebra the Weyl group W is generated by the set of all rj, j G J. Proposition 9 The structure matrix o f an integrable contragredient Lie algebra g satisfies three of the conditions CM o f Section 3.3: CMl: All = 2 for all i g J; CM2: Aij G —N for all z, j CM3: A^j = 0 <=>Aji = 0.

g

J, z

;;

Using the notation established above, we have the relations

R l:

i[ar,f,] = -AjJj, for all i, j G J. ■■= ( ade¡ )

R2:

I d~j ■■= (ad f¡)

= 0,

=0

for all i # j.

324

Contragredíent Lie Algebras

A matrix A ^ satisfying CMl-3 is called a Caitan matrix. In the literature the expression “generalized Cartan matrix” is often used instead. We refer to a Cartan matrix satisfying CM l-5 of 3.3 as a Cartan matrix of finite type. The relations R1 and R2 are familiar from Section 3.7. However, the situation here is far more general. In Section 4.2 and subse­ quent sections we will show that a contragredient Lie algebra g can be constructed whose structure matrix is any prescribed matrix A for which CMl holds. If A satisfies CM l-3, then g can be constructed to be inte­ grable. In the exercises we outline a generalization of integrable contragredi­ ent Lie algebras that relaxes CMl. The terminology “integrable” comes from the fact that each representa­ tion of j e J, in g (given by the adjoint action) can be integrated to a group representation : 5L2(K) ^ A ut(g), as we have seen above. A contragredient Lie algebra (g, is called a Kac-Moody algebra if it is integrable. We say that g is of finite type if A is of finite type and of affine type if A is of affine type. Otherwise, it is said to be of índefiníte type. These Lie algebras were introduced in [Kal, Mol]. Let (g, be contragredient. We recall (Proposition 2.7.5) that the radical r = rad(g) of g can be characterized as the maximal ideal of g intersecting trivially. Since [e,, /¿] = e \ {0}, we see that r n

( 0 »
Let ~ : g g /r denote the natural mapping. By the Remark 1 of Section 2.7, g /r has a triangular decomposition ^ = (1^, g+, Q^, cr), where we have identified and and written a for the anti-involution induced by cr on g. Furthermore the display {e¿, , /J /e j rise to a display {é¿, a'^, of g, showing that g /r is contragredient. If ad is locally nilpotent, so are ad and ad /^. Thus we have a natural homomorphism ^:<^ad(s) ^ Gad(g) given by exp ad

exp ad

,

exp ad í/¿

exp ad í/¿,

4.1

Contragredient Lie Algebras

325

whenever ad (and hence ad f¿) is locally nilpotent. Note, however, that it can easily happen that ad é¿ is locally nilpotent, although ad is not; in particular 6 need not be surjective. Likewise we evidently have a homomor­ phism of Weyl groups, W{Q) ^ W(Q), which need not be surjective. However, this map is injective^ since W( q) can be viewed as a group of linear maps on Í) and i) and can be identified. Thus we can simply identify W( q) as a subgroup of W^(§). Similar considera­ tions apply to the algebra § •= 9 /t if t is any ideal of 9 such that t e r . More precisely Proposition 10 Let (g, be a contragredient Lie algebra, and let § = g /t, where t is an ideal of g contained in rad{%) such that o-(t) = t. Then the natural mapping “ : g ^ g is injective on th^subspace ®^ ® Identify­ ing 5 and ^j_we have that ^ = (^, g+, cr) is a triangular decomposition of g and (g, is contragredient. Furthermore (g, and (g, have the same structure matrix, and g is integrable if g is integrable. We have ^^A(g) c^^A(g),

PL(g) c iy(g)

with equalities if g is integrable. Proof. After the remarks above it only remains to prove the statements of the last sentence. If a e'^^A(g), then a = waj for some «y e '‘^n. Under the identification of IF(g) inside W{%), the same equality holds relative to g, so a e '’^A(g). If g is integrable, then = < r/ | ; e J> = W{%) and ^^A(g) = =^^A(g). □ Proposition 11 Let ( g , r ) be contragredient with structure matrix Л = g = g/rad(g), and let ~ ^ q be the canonical map. Then

y^j* Define

(i) I f A¿: e Z_ or if A¿: =Aj¿ = О for some i Ф j, then (adey) and d¿j = ( a d / y ) belong to rad(g); (ii) For ad éy {and hence ad /y) to be locally nilpotent, it is necessary and sufficient that for all i ¥=j, A¿j e Z Aj¿ = 0; (iii) g is integrable if and only if A is a Cartan matrix. Proof, (i) Suppose that A^j e Z < q for some i ¥-j. Consider the §1^2^^-sub­ module M of g (under the adjoint representation) generated by /¿. We have [ej,f] = 0 and [af,f¿] = - A ^ j f . By part (ii) of Proposition 2.4.2 (with f

Contragredíent Lie Algebras

326

replacing z;+, - a , replacing A, etc.), either d~j = (ad = 0 or M is a Verma module and dj] generates a maximal proper submodule. In either case ad ej{d¡j) = 0. Also (a d e ,)(a d /,)"^ '^ " 7 , = (

a

d

= 0.

Indeed, If A¿j < 0, this is clear, and if A¿j = 0, then also Aj¿ = 0 and [fj, h¿] = Aj¿f¿ = 0. Finally, it is obvious that ad ( a d = 0 if k ^ i, j. Thus d'j is a highest weight vector for g in the adjoint represen­ tation. We know then that the module M' that it generates is ad(U(g_))(ad 9_, and hence M' is an ideal of g whose intersec­ tion with is trivial. Thus M' c rad g, and we conclude that d~ e rad g. Since rad g is cr-invariant, d~^j e rad g proving part (i). (ii) If ad éj is locally nilpotent, then the A¿j are as desired by Proposition 8. (Recall that g and g have the same structure matrix, see Proposition 10). Conversely if ^4^y e Z A^ - = 0 => Aj¿ = 0, then (ad ij)

- A a + 1

e¿ = 0

for all i

j

by part (i). Thus ad Cj is locally nilpotent (part (i) of Proposition 8). (iii) The proof follows from part (ii). Proposition 12 Let (g, r ) be a contragredient algebra, and let Dg = g_e

=

Then

e g^..

Proof. For any a e A\{0}, [1^, g“] = g“, which together with [e„/;] = shows that Dg = g_+(^ n Dg) + g+D g_+ + g^. It remains to show that n Dg c . To prove this, we need only to show that [g_ , 9 + ] n ^ c Q ^, which we can reduce to looking at a single product [ j:, y], where X e g““ and y e g", a e A+. We use induction on ht a. If ht a = 1, then a = a,, X = c/„ y = de^ for some c, d e i e J, and [x, y] e Oth­ erwise, ht a > 1, and since g_ is generated by the /y, j e J, we may assume that X has the simple form [/ y, z], z e g“^, ¡3 e A+, ht = ht a — 1. Then [jc, y] = [[/;, z], y] = [fjiz, y]] - [z,[fj, y]]. Now [z, y] € g“', and [fj, y] e g^, so the proof is finished by the induction. □

4.1

Contragredíent Lie Algebras

327

Corollary ¡f ^ = Qk ^ ihen g is perfect.



Remark 6 The decomposition Dg = g_0 !2k ® 9+ (or more precisely (g+, Q^, o-log)) is not in general a triangular decom­ position. The problem is that it is possible (and always happens in affine algebras) that there are roots 5 0 for which g^] = 0. Thus is not in general large enough to serve as a diagonal algebra. This phenomenon, which can occur only if the structure matrix is singular, is largely responsible for the necessity in Section 4.2 of defining a realization of the matrix as a preliminary to constructing contragredient algebras with a given structure matrix. Let (g, Let a

be a Kac-Moody algebra with root system A. and let

0 A. The a-root string through ^ is 5(j8,a) = A n (/3 + Za).

The next result is the fundamental fact about root strings. Proposition 13 Let ( q, be a Kac-Moody algebra. Let a 0 '^^A. Then for any /3 e A there are nonnegative integers d, u so that 5(/3, a) is an unbroken sequence RSI

p - d a , . . . , p , . . . , p + ua,

and furthermore RS2

d - u = .

Proof Since a g“ + [g“, g““] + g”“ = ^1^2^ is isomorphic to ^l2(IK). Furthermore g affords an integrable representation of (Proposition 6). Let N ‘= E^ez9^^^“- Then N is an integrable submodule, and its weight system P(N) is precisely S(p, a). From Proposition 2.4.7, N decomposes into finite-dimensional irreducible submodules, each of which has the form K= where dim = 1 and ad is scalar multiplica­ tion by 5 - 2/, / = 0 , .. ., 5. Since ad a is multiplication by <j3, + 2k, we have K S —2Í

C

+

0 , o : ' ' » /2 ] - i } a

328

Contragredíent Líe Algebras

This implies that s = <)8, (mod 2). Now we use the Freudenthal mid­ point argument [FdV]. The midpoint of the set of roots ¡3 + {^(5 — (¡3, a'^)) - ¿}a as i runs from 0 to 5 is 1/ (

2

\ is-(p,a^y ^ l« + ^ + ( ^ )“ —

= /3 - -a, which is independent of s. Actually /n is a root of the string only if <13, a^> e 2Z, but the point is that all the irreducible submodules K of N share the same midpoint and they all involve fi or fi j a according to the parity of . □ We finish with a prescription to inductively compute the entire set of positive roots of a Kac-Moody Lie algebra: Proposition 14 Let ( q,

be a Kac-Moody algebra with root system A. Let

Q+{n) = (a e ¡2+ lht(a) = «}, A+(n) = A+n Q ^{n), n ^ l . {For n < 0, Q^{n) = A+(n) = 0.) Then (i) 0 ^ ( l ) = { a j / e J} = A^(l); (ii) for a e Q^{n), n > 1, we have a e A+(n) if and only if one of the following two conditions hold: (iia) there is an / e J such that (a, a f ) > 0 and r¿a s A+(n - ( a , a f ) ) , (iib) for all i e J, (a, < 0 and for some / G J, a —a¿ G (n - 1). The roots that occur in (iib) are imaginary, and a root a occurring in (iia) is imaginary if and only if the corresponding root r^a is imaginary.

4.1

Contragredient Líe Algebras

329

Proof, (i) Clear. (ii) Let a e Q^(n); n > 1. First, we show the conditions are necessary. Assume that a e A+(/t). If condition (iia) fails to be the case, then from (4.6) we see that 0 and hence by Proposition 13, a e A. Finally if the root a occurring in condition (iia) is imaginary, then so is r^a [Proposition 5(iv)]. If a occurs in condition (iib), then to show that a e'^'A, we must anticipate Proposition 5.2.6. Indeed, if a then In particular a ^ = ^ 0? and hence ( a , a ' ' ) = E y e j c / a ,a / > < 0, contrary to
rel="nofollow"> = 2.



Corollary Let t be any ideal contained in rad(g) such that or(t) = t. Then A (g/t) = A(g) {see also Proposition 10). Proof The algorithm of the proposition determines the same subset of 2 ^ for g and g /t. □ We finish this section with a description of the Lie algebra of derivations of a contragredient Lie algebra g. Any linear mapping e : g/D g Z(g) lifts to a linear map e : g Z(g) g annihilating Dg, and s is clearly a derivation. Identify the space of these derivations with Hom|,^(g/Dg,Z(g)) Proposition 15 Let Q be a finitely displayed contragredient Lie algebra with dim Then D erg = H om K (g/D g,Z (g)) + a d g . In particular, if Q is perfect or Z(g) = (0), then Der g = ad g.

< dim g+.

330

Contragredient Lie Algebras

Proof. Using Proposition 2.1.4 it will suffice to show that a derivation 5 e Dq belongs to Honi(|^(g/Dg,Z(g)) + ad g. Let a : / , j be a finite display. Then 8a^= d([ej, fj]) c K a / and 28ej = Cj]) = [5 a /, ej] + [a /, Scj] shows that 5 a / = 0. It follows that if 8ej = XjCj, then 8fj = -Ay/y for some Ay ^ IK. Choose /i e so that aj(h) = Ay for each j. Then 8 — aid h kills Dg. Also for any h' ^ ij and any x e Dg, we have 0 = (5 — ad h)[h', x] = [(5 - ad h)h', x] showing that (5 - ad h)(h') centralizes Dg. Since it lies in 1^, it also centralizes ij, hence g. Thus (5 - ad /z)g c (6 - ad AXi) + Dg) c Zg, and finally 5 e Hom(g/Dg, Zg) + ad g. □ 4.2

REALIZATIONS OF CONTRAGREDIENT LIE ALGEBRAS

In Section 4.1 we saw how every contragredient Lie algebra gives rise to a structure matrix. In this section we reverse the process and show how to construct a contragredient Lie algebra with a given structure matrix A. When A is ai Cartan matrix, this leads to the construction of a Kac-Moody algebra with structure matrix A. As a preliminary step it is necessary to construct from A a space 1^, which will eventually be the diagonal subalgebra of our Lie algebra. This involves the idea of a realization of A. Let J be a nonempty set, and let A = (A¿J), ¿,j e J, be a matrix with coefficients in IK(more properly A is an element of I K By a realization of A over IK, we understand a triple /? = ( 5 , n , n ^ ) consisting of a vector space over IK together with two subsets II = {a, | i e J} c ij* (the dual space of 1&) and II^= { a/ | / g J} c such that Rl: each of the sets II and II ^ consists of linearly independent elements; and if we denote the natural pairing of 1^* and l^by<*,->:l^*xf)-^IK, then R2: = A,j for all /, j g J. The realization is finite dimensional (of dimension dim 1^) if 1^, and hence is finite dimensional. Example 1 Consider A = ^

a,b, ^ K . We distinguish two cases:

1. ab ¥= A. We may take to be a two-dimensional IK-space with basis n ^ = {aj^, a /} and then define II = {a^, a2) c if* in the only possible way, namely (a¿, a /> =-^4¿y; 1 < /, j < 2. That H is linearly indepen­ dent follows from the fact that det(^) = A — ab 0.

4.2

Realizations of Contragredient Lie Algebras

331

2. ab = 4. Introduce a third symbol d, and define = Let n

Ka^,

[a^, «2 }, and II = {a^, «2} c 1^* be defined by a /> =Aij,

1 < i, j < 2,

( a i , d ) = i. Then R '= (]^, n , n ^ ) is a realization of A. Example 2 Let J = Z, and define A e

by

An = 2, A^j= Aij = 0, Let ]^ = ®

and

| / - ; | = 1,

otherwise.

and define

e 1^* for all i e Z by

=A^ j , By setting n = {a, I / ^ Z} and 11^ = yl.

i , j e Z. | i e Z}, we obtain a realization of

Proposition 1 Suppose that card(J) = / is finite. Let 1 = I -\- corank(y4). Given nonzero elements , S/ o f IK, we claim that there exists an I X l-matrix A with the following properties : mini: min2: min3: min4:

Aij = Aij for all 1 < i, j < 1. det(^) 0. A^j = AjiS^ for a l l \ < i < l < j < l andA^j = Aji for all I < i, j < L If A is a Cartan matrix and all belong to then A is a Cartan matrix.

Proof. To see that A exists, first observe that if corank(^) = 0, then A = A, and we are done. Otherwise, we construct A in corank(^)-steps as follows: Consider an (/ + 1) x (Z + l)-matrix A^ of the form

^1 =

SiOi 2

Contragredient Lie Algebras

332

Let S := { ( c j , e = 0 for all j}. This is a nontrivial subspace o f Thus, if H — {(a^ . . . , aj) | Ej^iCjCjaj = 0 for all (c^,..., Cj) e S}, then H is a proper subspace of Let R be the row space o f A. Then R is a proper subspace o f IK^ Hence there exists (a^,. . . , a|) e ZL\{R U H}. By construction the matrix defined by this choice o f a^ satisfies corank{Af) = corank(A) — 1. Indeed its first I rows have row rank = rank(A) + 1, and the last row is evidently independent of these first I rows. We now repeat this argument for A ^ with respect to e\ , , . ., where e\ = and = 1- After corankiAysteps we obtain a matrix A satisfying min(l)-(3). Suppose that the hypotheses of min(4) holds. Then A is a Cartan matrix provided that each Eia^ e Z. Thus must be chosen to cancel the denominator o f which is easily arranged. □ Remark 1 Condition min(l) states that ^ is a submatrix of A. Condition min(2) will be used to explicitly construct the realization of A. Condition min (4) allows us to assume that ^ is a Cartan matrix whenever A is. (We just make a suitable choice of Condition minO) is important later on when we define symmetrizable matrices (Section 4.4). It says that if A is symmetrizable by (e^,. . . , then A is symmetrizable by (e^,. . . , 1, . . . , 1). Proposition 2 Let A G

be a matrix. Then

(i) a realization of A exists', (ii) if card(J) = I is finite, then ij can be taken to be o f dimension I + corank(^), and this is the smallest dimension possible. Proof (i) Define to be a C-space admitting the set {af, basis. For each i e J, let =f|* be defined by

| / e J} as a

=Aij, Then I I : = { a J / e J } is clearly linearly independent, and with II {af \i ^ J}, R — (]^, n , n ^ ) is a realization of A. (ii) Using Proposition 1, let ^ be a Cartan matrix which is 1 X 1, where / = / + corank A, which contains A as the submatrix (A¿J)l^¿ J^l, and which satisfies d e t (^ ) ¥= 0. Let f) be an /-dimensional (K-space. Fix a basis a^, . . . , ai of Define « i , . . . , ^ if* by a / > = A^j. Then the a¿ are linearly independent because d et(^) ¥= 0. It is clear that if II — {a^,..., a/} and { a^ , . . . , af}, then (]&, II, 11^) is a realization of A of dimension I Finally, let R = 0),YI,U^) he any finite-dimensional realization of A. Choose bases B and B* of f) and 1^* so that they begin with a f , . . . , a / and ai , . . . , a i , respectively. Since the matrix M = has

4.2

Realizations of Contragredient Lie Algebras

333

linearly independent rows, in particular its first / rows are linearly indepen­ dent. Now, if S is any k X k matrix of rank s and S' is any (k) X (k 1)matrix of the form 5' = [5 I *], then S' has rank < 5 + 1. Applying this to the submatrix A which occupies the top left corner of M, we see that for its first / rows to be linearly independent, the number of columns must be at least / + (/ —rank(^)) = / + corank(^). Thus / + corank(>l) is the mini­ mum dimension for if in any realization of ^4. □ If J is finite and R •= ( / z , n , n ^ ) is a realization of A ^ with diml^ = / + corank(y4) then we say that R is a minimal realization of A. Let A and = (f), 11,11^) be as above. We construct a realization R^ of the transpose of A. Set R^ = ( f ) *, n" ',n ) where II^c]^

]^** under the canonical identification of f) inside 1^**. Let < • , • > : f)* X f)** ^

K

be the canonical pairing. (Note that this pairing is written with the factors in the reverse order that one might expect. We do this so that we may think of the new < * , • > as being an extension of the original pairing under the canonical identification of i) in 1^**), Then (aj,ar)=A,=Ajj. Since both n ^ c f)** and II c 1^* are linearly independent, it follows that is indeed a realization of A^. We say that is the realization dual to R. We now begin to construct Lie algebras out of matrices. Let A ^ be a matrix and R = (1^, I I ,11'^) be a realization of A. View as an abelian Lie algebra, and let X = {e^, | / e J} be a set of symbols. We let g = be the free Lie algebra on X and define f

^*g

to be the free product of f) and g. Let R be the subset of f , consisting of the following elements for all ¿,j e J and e 1^:

(1) [h,fj] + (aj , h) f j . The first Lie algebra that is of interest for us is then defined by

334

Contragredient Lie Algebras

where I(R) is the ideal of f generated by R. We call u(A, R) the universal algebra of the realization R of A. Remark 2 Let {h^ I i e 1} be any basis of Then u (^ , /?) can be described as the Lie algebra generated by the set ej, fj | i e / , ; g J} subject to the relations [ e j , f J - 8j^a]',[hi,ej] - ( a ^ , [ / i „ / ^ ] + (aj,hi)fj, where i , k ^ I and j, m g J. We now look more closely at the Lie algebra u = n(A, R), For conve­ nience the notation for the canonical map f ^ u will be suppressed when­ ever no confusion is possible. Thus we will use expressions of the form “ Cy G u ” where, strictly speaking, this is to be understood as meaning €j H- I(R) G u. For the time being, we will denote the image of fj under the canonical map by that is, + I(R) c u. Later we will see that is actually an injection, and we will be able to identify i) and Via the adjoint representation acts on u. Combining this fact with the canonical map ^ 1^^, we see that u has a natural 1^-module structure, and under this action h • Cj = a j ( h ) e j , h • f j = —a j ( h ) f j , and h • if ^ = (ff) for all /z G ]^. In other words, each ej and fj and all the elements of are weight vectors of the l^-module u. Their weights are aj, -Uj and 0, respectively. Since u is generated by these elements it follows from Proposition 2.1.2(ii), that u admits a weight space decomposition relative to 1^. The weights all lie in the group Q := 0

l a j c i)=*

and u = 0 u “, a^Q where u" := (jc e u I[h, x] = ( a, h ) x for all h We define

e+==(V;e0j

/

\{o},

Q- = -Q ^,

£tnd the corresponding subalgebras u+=

0

u “.

We also define, in the usual way, the height function h t : 0 ^ Z, ht: £ c ,a ,.

L c, .

g

4.2

Realizations of Contragredient Lie Algebras

335

Finally, set Qk

•= Ф

the K-span of П in 1^*.

In the same way we define QX, QX, and giK inside 1&. Our intention now is to show that u = u _ 0 ^ ® u + and that u admits a regular triangular decomposition. We begin by establishing the following proposition: Proposition 3 There exists a unique anti-involution a o f n satisfying cr(cy) = fj, o-(fj) = and c r I = 1. Proof The uniqueness is clear since u is generated by together with the e/s and f/s. The map e^ -e^ extends to an automorphism of the free Lie algebra Since is abelian, the map x —jc is an automor­ phism of ]^. By Proposition 1.10.4(ii) there exists an automorphism (o of f = ]^ * g satisfying (o(e^) = - f , caifi) = and
e I(R).

Hence (o induces an automorphism (also denoted) co of u. It follows that (T '= -0) is our desired anti-involution. □ Proposition 4 Let the notation be as above. Then (i)

is generated by {ej I y e J} and n_ is generated by {fj I ; ^ J} (as Lie algebras); (ii) u = u_® ® u+. Proof The argument is precisely the same as that in Proposition 4.1.1.



Proposition 5 Let the notation be as above. Then (i) The sum YKf j + + ElKcy is direct and the restriction to it o f the canonical map f u й injective; (ii) and u_ are free Lie algebras, freely generated by {ej I ; ^ J} and {fj I j ^ J}) respectively.

Contragredient Líe Algebras

336

Proof, Let A be the free associative algebra on the set X = {xj \ j e J}. Let A e ]^* be arbitrary. We proceed to show that A can be made into a highest weight u-module with highest weight A and highest weight vector 1 ^ A, Define a representation of ]&on rel="nofollow">1 by h ' 1=

h-Xj^

Jk

for a l l ; i , . . . , ^ G J,/i el^. Next we make A into an g-module as follows. Since S is freely generated by {ej, fj I j e J}, it suffices to define the action of each Cj and fj in A. (Recall the correspondence between ^-modules and left U(g)-modules and the fact that U(3) is the free associative algebra on {ej,fj\j e J}. See Proposition 1.10.2). We define f j ' X = XjX

for all y e J, jc e y4.

The action of the e/s is defined recursively on each monomial Xj^... Xj^ as follows: ey • 1 = 0, Xf

Jk

=

X:(e:

Jl^ J

• JC,

Jl

. . .

X: ) Jk'

+ djj^X - aj^

---- ''Jk'

[The action of e, is defined in such a way as to be compatible with = fjl ■ ^ifj = fi^ + We have given A both an and an g module structure. Thus there is a unique f = * ^-module structure for A compatible with the above (part (ii) of Proposition 1.10.4). Straightforward computation shows that the ideal I{R) of f lies in the annhilator of this module and hence that A inherits a u := f//(jR)-module structure. For instance, consider /y] [e,,/;] • 1 = C,- •/; • 1 - fj • = C,. • Xj

•1

= Xj{e^ ■1) + 5,/A,a>'>l = 5,/A,a,y>l = 5,,ar- 1. Similarly [e,, fj\

■Xj ^... Xj^

= e, •

...

x¡^

-

x ¡ ■ e,



...

x¡^

= 5„

Jk

4.2

Now let

Realizations of Contragredient Lie Algebras

337

e ]^ \ {0}. Then for the u-module A we have (h + I { R ) ) • 1 = /i • 1 = l.

Hence h + I(R) = 0 (in u) only if (A, /z> = 0. Since we are free to choose A arbitrarily, we may assume that ^ 0. It follows that +/ (/? ) ^ 0. In other words, the canonical map i) ^ is injective. The representation of u_ on is just the left regular representation of A on itself; that is, each fj acts on A as left multiplication by Xj, This gives us a homomorphism U(u_) A with fj Xj. Since A is free, the inverse map with Xj ^ fj exists, and U(u_) —A. Thus the Lie subalgebras of Lie (U(u_)) and Lie {A) generated by the fj and Xj, respectively, are also isomorphic. But the latter is free on the [xj] (Proposition 1.10.1). Thus u_ is freely generated by the set [fj | j e J}. Finally, a interchanges u_ and u+, and hence part (ii) is proved. From part (ii) of Proposition 4 and the freeness of u the sum ElK/y + + LKcj is direct. □ Remark 3 The u-module A described above is evidently the Verma module of type (1, A) for u. Remark 4 Part (i) of Proposition 5 allows us to identify in u. We assume this identification henceforth.

with its image

Proposition 6 Let the notation be as above. Then (i) for all a ^ Q \ {0}, dim u “ < oo; (ii) for all i e J, dim u “' = dim u " “' = 1; (iii) if J is countable and ^ is of countable dimension, then u is of countable dimension. Proof. We know that u “ = (0) unless a e ± 0 + or a = 0. Take a e Q^. By part (i) of Proposition 4, u “ is spanned by the products ej^ ...]], where + ••• = a, of which there are only a finite number. For the special case a = u “' is spanned by e^. Using a, parts (i) and (ii) now follow. Part (iii) is immediate from part (i). □ Putting everything together, we have Proposition 7 Let u = Vi{A, R) be the Lie algebra defined by a matrix A and a realization R. In the notation established above. (i) ,5^ := (]^, u+, 0+, O') is a regular triangular decomposition o f the Lie algebra u; (ii) if An # 0 for all i e J, then (u, ^ ) is contragredient.

Contragredient Lie Algebras

338

Remark 5 The structure matrix S of the contragredient algebra (u, *9") above need not equal A, In fact, assuming all ¥= 0, S = A if and and only if all ¿, Aii = 2. Example 3 Let A = {d) be a 1 X 1 matrix, a 0. Then with — Kh and a e ]^* defined by (a , h) = a, we obtain a realization R = (^,{o:},{M) of A and u = u(A, R) = K f 0 K/z 0 Ke with [e, f ] = h, [h, e] = ae, [h, /] = -af. It is easy to replace / , h, and e by suitable multiples (see Section 4.1) and obtain the standard §l2(IK)-triplet [e,f]=h,

[h,e] = 2e,

[A,/] = - 2 / ,

from which we conclude that u = ^I2(1K). The structure matrix of u is (2) and of course any minimal realization R' = (]^',{a},{a^}) of this matrix (i.e., (a, a ^ } = 2) yields u((2), R') = n(A, R). Let (g, be contragredient. Since later we will work extensively with such algebras, we will set once and for all the notation to be employed in this context. •^ = (^, Q+, Q+, o-) n =

Triangular decomposition Fundamental roots

n '-

Fundamental coroots

< 2 = 0 Zaj jsj

Root lattice

0 Za/

Coroot lattice

;s j <2k = 0

IK«; c

= 0 yeje += 0 yej

0 _= - Q ^ The structure matrix of ( g , ^ )

< -.-> :rx 5 ^ K J /jr}yej

The natural paring A display of (g ,

(in particular

cr(ej) = fj for all j e j ) Consider the triple R == (1^, II, 11^) arising from (g, 3^). It is immediate that R is a realization of the structure matrix ^ of (g, (note that we

4.2

Realizations of Contragredient Lie Algebras

339

need CT3 for this). We call R the natural realization of A in the context of (g, ^ ) . Let us now construct the universal Lie algebra u = \i(A, R) as above. Set

and f=

Then u = f//(i^),

where I(R) is the ideal of f generated by the elements of the set R defined in (1). Recall (Proposition 5(i)) that

(2 )

I 0 K/,.j ® ^ e I ©

cf

can be identified with a subspace of u. Accordingly we henceforth identify with a subalgebra of both u and g and think of ej and fj as elements of both of these algebras. (It will always be clear to which algebra we are making reference.) As we have seen above the algebra u admits <5^ as a triangular decompo­ sition, where = (f |,u^ ,G^ ,o-). Moreover (u, ^ ) is contragredient (Proposition 7(ii)). Because of the way in which f is defined (i.e., as a free product), there exists a (unique) Lie algebra epimorphism

satisfying

Hfj) =fj’ (¡/(h) = h

for all

e ]^, 7 G J.

Since i/r(/(i?)) = (0), there exists an induced epimorphism q. This allows us to realize g as a homomorphic image of u. We refer to

340

Contragredient Lie Algebras

(u, Ty, if/) above as the universal covering of (g, «^). Evidently (3)

^(u^)=g«

for all a e g .

Proposition 8

Let ( g , Then

be contragredient, and let

(u ,

, i/r) be its universal covering.

(i) ker((/r) c rad(u), (ii) (/i(rad(u)) = rad(g). Proof. In view of Proposition 2.7.5, we have t ^ ( u ) = m^^(u) = rad(u) and = my^Cg) = rad(g). Since is an isomorphism, it follows that ker(i/i) n ]^ = (0), whence we have part (i). Similarly (/r(rad(u)) is an ideal of g which intersects trivially, while i/i”Krad(g)) is an ideal of u which intersects trivially. This establishes part (ii). □ Let A G

and let R he a realization of A. Define Q= q ( A , R ) := u (^ ,i^ )/ra d (u ).

By (2.7(i)), rad(g) = (0). We call g (^ , /?) the radical free algebra of the pair (A, R). Note that if A^^ ¥= 0 for all i e J, then g is contragredient, and in this case we call q(A, R) the radical free contragredient algebra of the pair (A,R\ We have seen that any contragredient algebra (e, with the natural realization R has a universal covering (u, i/r). If furthermore e is radical free, then by Proposition 8 ker if/ = rad(u), and it follows at once that e is canonically isomorphic to g (^ , jR). Proposition 9

If e is a radical free contragredient algebra with structure matrix A and realization R, then there is a canonical isomorphism e g (^ , i?). Our interest is primarily in the case that ^ is a Cartan matrix. In that case = u (^ ,/? )/ra d (u ) is integrable, and hence, a Kac-Moody algebra, by Proposition 4.1.11. However, there may be intermediate Kac-Moody algebras, between n(A, R) and g(v4, R). q( A , R )

Proposition 10

Let A be a Cartan matrix with realization R, and let n{A, R) be the corre­ sponding contragredient algebra. Let J{R) be the ideal o f vl{A, R) generated by

4.2

Realizations of Contragredient Lie Algebras

341

the elements \dtj = {&áe¡)

i*j

1^.7 =

i* i

(R2)

Then R) •= u(yl, R)/ J{R) is a Kac-Moody Lie algebra. Furthermore for any Kac-Moody algebra % with realization R, there exist surjective homomorphisms q\ A

, R ) ^ q ^ q( A , R )

{with the obvious effects on their displays) under which ra d g ^ ( ^ , i? )

rad(g) ^ r a d g ( ^ , i ? ) = (0).

Proof. That g^(^, R) is integrable follows from Propositions 4.1.8 and 4.1.10. The existence of the map q^{A, i?) g follows from factoring the covering homomorphism u{A, R) ^ % through q^(A, R) by Proposition 4.1.9. The rest follows from Proposition 8. □ This proposition is a natural complement to Proposition 4.1.9. In the sequel (Section 4.6) we will find that for the cases of most interest Q^(A, R) = %{A, R). Example 1 A =

bring the notation in line with our usual

notation for §Í2(IK) in the Appendix on A^^\ we will take II = {«(„«1}, n'^= a^} with <«,-,«/> =A¡j and set h = IKif +

+ IKa^.

Using R = {§, n , n ''} , we define u(A, R). It consists of two free Lie algebras ^ +~

u _ —( / o , / i ) ,

and the abelian subalgebra h: u

=

< /o> /i>

®

< eo,C i> .

342

Contragredient Lie Algebras

The algebra u is contragredient and simple considerations with free Lie algebras show that its root system is A(u) = A(u)_u{0}

U

A(u) + ,

where A(u) + = [ka^ 4- ma^ | f c , m > 0 , A: + m > 0 , and fc(resp. m) = 1 if m (resp. k) = 0} A ( u ) _ = “ A(u) + . The root space multiplicities (dim u “, a e A(u)) can be computed by Witt’s formula (Proposition 2.5.5). Since ^l2(IK) is contragredient with structure matrix A there is homomor­ phism i/i : u

êl2(IK)

with e, ar^h„

I = 0,1 (the fact that corresponding elements u and § 12(11^) have the same name should not cause confusion). This example continues in the Appendix on

4.3

(see Section A.3.)

EMBEDDINGS, FIELD EXTENSIONS, AND DECOMPOSABILITY

Let J c J', and let A g be a submatrix of A g Suppose that R = (1^, n , n'^) and R' = (^', II', 11'^) are realizations of A and A , respec­ tively, where II = II'^= n' = and 11'''= ej-. An embedding of i? in i?' consists of an ordered pair 17 = (•>7^, 77^), where 77^ (resp. is an injective linear map (resp.

-» 1^')

4.3

Embeddings, Field Extensions, and Decomposability

343

such that (i) 77^:11^11' with 7]^a^) = a- for all i e J; (ii) n'"" with for all i e J; (iii) for all a e f)*, for all f| e i|, t7^(/z)>' = (a, h); where ( • , • ) pairings.

X ij

and <•, •>' : f)'* X i)'

are the canonical

Note that since <«;, = A]j = A^j = (a^, a j ) for all /,; e J the con­ ditions (i) and (ii) are compatible with condition (iii). At the lattice level there exists induced Z-linear maps Vl ‘ Q ^ Q' • Note that for ¡L e

( 1)

^

V

l

( Q )

if and only if supp(/i') c J.

Remark 1 The most obvious and usual example of an embedding occurs when one takes f) to be any subspace of 1^' containing such that {a-lygj, if restricted to functions on 1^, is a linearly independent set of 1^* (e.g., 'tj = 1^'). Define re s: 1^'* -> 1^* to be the restriction map arising in a natural way from the inclusion c 1^'. Then with II — [a\ I / ^ J} and n^:= {a'^ I i e J}, we see that /? = (1^, II, n ^ ) is a realization of A. Fur­ thermore, with the maps inclusion map, ^ any linear map that lifts the elements of 1^* to linear functions on ij' (i.e., res • rjj^ = id) and such that T7^(res(a^)) = for all i e J, we have that 17 == (17^, is an embedding of R in R \ We call R a natural realization of A in the context of R \ Remark 2 We have assumed in our definition that J c J' and that ^ is a submatrix of A'. It is rather easy to extend the definition to an embedding (p: J -> J', and matrices A and A' indexed by J X J and J' x J', respectively, satisfying = ^ ij for all i , j e J. Results involving 17 have obvious generalizations to this case. Proposition 1 With the notation as above let rj = ( v l ^Vr ^ tm embedding o f the realization R of A in the realization R! o f A . Then there is a canonical embedding {also denoted 77) 77

: u := n ( A , R)

u' := n { A , R')

344

Contragredient Lie Algebras

such that (0

7j(]^) = ■njiiif)

C

1^';

(ii) T7(e,) = e'i and rjifi) = for all i e J; (iii) T7U" = for all a ^ Q \ {0}; (iv) a'(rix) = riicrx) for allx e u, where a and a' are the anti-involutions on u and u', respectively. Proof Let X ■■=[ej, fj}j ^ j and X' ~ {e'j, fJ}j ^ j. and define f and f' to be the free products ii * and 1^' * that are used to define u and u', respectively. We define a Lie algebra homomorphism i/i: f ^ f'

i

by = Vr , il>(e¡)=e’¡, , ¡ , { f ) = f ¡ .

for all i e J,

and observe that the relations R involved in the definition of u are annihi­ lated by ip. For example, - «0«") = [<’ fj] -

0-

Thus ip factors through the ideal /(R) to give 77: u u'. Since 17(6^) = e) and and are freely generated by the {e^} and {e'¿}, respectively, we see that 7] embeds u+ into u+. The same applies to u_ and u'_. All the statements of the Proposition are now obvious except perhaps for the equality in part (iii). For that, observe first that for all a ^ Q \ {0} we have u “ = (0) = unless a ^ Q+. Assume then that a ^ (the Q_ case is similar). Then u" is spanned by products [Cj^,. . . , CjJ with j) in J and aj^ + • • • +ay^ = a e Q+. Next ^rvLM jg spanned by products [e'y,. . . , e'j^] with in J' and a'j^ + • • • = i7^(a). By (1) {j\ , . . . , ^} c J, and hence each of these products lies in t7(u"). □

Remark 3 The most common situation in which the last proposition arises is the one in which A is some submatrix, say, of some matrix ij-'l i,j < kl A = that has some realization R! = (f)', II', 11'^). For the real­ ization R one may take (f)', II, 11^), where II — [a\ , . . . , a'j^} c II' and — . . . , a '/ ) c (see Remark 1). Then u = u(yl, R) embeds into u' = Vi{A, R ) by ^ fi ^ fi, a\^ so that u may be identified with a subalgebra of u' in the most obvious way imaginable.

43

Embeddings, Field Extensions, and Decomposability

345

Another common and equally obvious embedding occurs when A, as above, is nonsingular (even though A' may be singular). Then we may use the realization R = ((2k >n , n'^), where 2 ^ == 0 <=i * '' Example 1 Let be a realization of A g and let 7 g J be fixed with Ajj # 0. Let = (Ka/,{a^},{a/}). Then, as above, is a realiza­ tion of ( A j j ), and we have the canonical embedding u((Ajj), R^^'>) -» u(^4, R). As we see in Example 4.2.3, u ( ( > l ^ . p , = gljClK). Now u((y4^.p, is isomorphic to the subalgebra of \i(A, R) generated by Cj, fj, a / , which we know also to be isomorphic to SljiK). Proposition 2 Let Tj be an embedding o f a realization R in realization R’. Let 17: u(A, R) -» \i(A, R') be the corresponding embedding o f Lie algebras. Then (i) 77(rad(u)) = rad(u') n tj( u ); (ii) the induced homomorphism q(A, R) g(A', R') is injective-, (iii) 77^ A = A' n t]j(Q), where A and A' denote the root systems o f q(A, R) andgiA', R'Xrespectively.Moreoverforalla G A \ {0},77(g(y4, i?)“) = g(A', (iv) if g(A, R) and g(A', R') are Kac-Moody algebras, then -nr.C^A) =^^A' n 7,^(2), 77^(""A) =""A' n 77^(2). Proof Let J and J' denote the indexing sets for A and A', respectively. Let a' ■■=Ttifa) G 2'+. where a g A+, and let x g u “. Assume x g rad(u). To show that y ~ t](x ) g rad(u'), we must verify that given y^ g g ' " ' ..., ^ 2'+ and -I- • • • +iS'* = a', then Vk ^ S -Pi where

[yi. • • •, y*. y] = 0. Since supp(a') = U f=i supp(j8-) it follows from (1) that supp(j8p c J for all 1 < i < A:. Thus = t7^(/3,) for some /3, G 2+ , and hence y, = t7^(x,) for some x, g u “^' (part (iii) of Proposition 1). Thus 0 = 77(0) = T7([x i,. . . , X*, x]) = [yj,. . . , y*., y]. In the same way 77(rad u)“ c radu' if a G A_. On the other hand, if x i rad(u), then it is evident that y € rad(u'). Thus 77(rad(u)“) = rad(u')’’i-(“) n t7( u ). Now parts (i) and (ii) follow at once. It is clear from (ii) and Proposition 1 that TjjfA) c A' n rjjfQ). For the reverse inclusion it suffices to take a' g A'+n r]j(Q). Then a' g -q^fQ^), and so a' = ■ +a-^ for some i j , . . . , G J. Since a' g A'+, for some permutation of i j , . . . , say, the trivial one, [e^, ■■■, e^] * 0. Thus [e,y...,e,^] # 0 and 6' ■= T7^(a,^ -!-••• +a,^) ^ t7^(A). Furthermore, since

346

Contragredient Lie Algebras

q(A', R')“' is spanned by the products of the form [e\^,. . . , eJJ, riiqiA, i?)“) = q(A', R')“'. This proves part (iii). According to Proposition 4.1.14, for n e Z+, n > 1,

(2)

a e" A +( n ) => 3; e J,

such that (a , a j ) > 0,

a - { a, a' j ) aj

- < a ,a / > ) .

Similarly (3)

e"A '+(n) ^ 3; e J', rtL*^ -

such that <7,^«, < > > 0,

e''^A'+(n - <17^«, a}'")).

Now supp(i7^(a)) e {a -1 i e J}, and hence a!^) > 0 is possible only if j e J. Thus in (3), J' can be replaced by J. Now part (iv) follows by induction on n, starting from the obvious fact that ry^C^Ad)) = t7^(A(1)) = A'(l) n 71¿ Q ) =^"A'(1) n 71¿ Q l □ Remark 4 If we are in the cases described in Remark 3, then part (iii) of Proposition 2 assumes the simple form (4)

A = A' n E

Remark 5 In this proposition q(A, R) and q(A', R') can be replaced by and q \A ',R ').

q\ A , R )

We now look more closely at derived algebras. Let g = q(A, R) be the radical free Lie algebra defined by a matrix A and realization R. The proof of Proposition 4.1.12 (which is for contragredient algebras) carries over directly to show that (5)

Dg = g_0

0 g+.

Here we will give an entirely different description of Dg that shows that it is dependent only on A (not on R). Let Л be arbitrary, and let b be the Lie algebra defined by the generators e^, (/ e J), together with the relations

(R')

43

Embeddings, Field Extensions, and Decomposability

347

where h¡ ■= [e,, /,]. We begin by noting that [ht,hj] = [ hi , [ e j J j ] \ = [Aj^ejJj] + [cj, - A j J j ] = 0 ,

which shows that a == is an abelian subalgebra of b. We can grade b by (the set of mappings of J into Z). Let be defined by «/(;) = ^¿j, and set deg

= a^,

deg/, = -a,., deg hi = 0. Then the relations (R') are homogeneous, which suffices to determine the grading on b. We have need only of the subgroup Q' of consisting of functions a with finite support. Let Q'+ = {En,o:, e Q' \ > 0} \ {0}, and let Q'_ = Then with b+:= we have by a trivial adaptation of Proposition 4.1.1, b = b_0 a © b , and b +=

e J>,

b_= . Evidently there is a surjective homomorphism (/) = / , and hence with (f>(hi) = a / , since the corresponding elements in u satisfy the relations (R'). Since u+ is freely generated by 1/ e J}, :b+ —^ u+. Likewise (j>: b_ —^ u_. Since { a/ | / g J} c c u are linearly independent, we have (f>: a , and we conclude that is a Lie algebra isomorphism. Furthermore there is an isomorphism : Q' —^ Q with a, and Define (R'')

r := maximal homogeneous ideal of b intersecting a trivially.

Since r is graded, (x) = n u “) from which it is clear that (j>(x) is invariant by ad 1^. Thus <^(r) is an ideal of u (not just Du), and hence (/)(r) c rad(u). On the other hand, rad(u) c D(u), and <^"^rad(u)) is a graded ideal of u intersecting a trivially. Thus r = <^“ Krad(u)), and we have

Contragredient Lie Algebras

348

finally b /r = Dg. This gives the alternative description of Dg by (R') and (R"). Proposition 3 Let A e

be a matrix, and let R b e a realization o f A,

(i) Dg(yl, R) —b /r , where b is the Lie algebra defined by the presenta­ tion (RO and r is the ideal defined by (R"). In particular Dq(A,R) depends only A. (ii) Dg w perfect if and only if A has no row consisting entirely of zeros. (iii) I f A is a Cartan matrix then Dg^(^, R) (see Proposition 4.2.10) has the presentation with generators e^, /¿, h^, i e J, and the relations

(R l) [e¿,fj]

=

8¿j hj

for all

i j ;

i(adc,)'^'^"^e, = 0, (R2) \

fj)

V/ = 0

for

ii^j.

Proof (i) The proof has already been established. (ii) and (iii) The proofs are left as exercises.



Corollary Let (t, and (c', ^ ' ) be radical free contragredient Lie algebras admitting the same structure matrix. Then De = Dc'. Proposition 4 Let A e and let R be a realization o f A. Let g = g(yl, R). Then the centers of g and Dg are given by Zg = (/i e

I

h) = 0 for all i e j},

ZDg = {A e G k K«/, A> = 0 for alii e j).

43

Embeddings, Field Extensions, and Decomposability

349

Proof, Let z be central in g or Dg. Then writing z = ^ 9“? see immediately that each z" is central. Proposition 2.7.3 shows that z “ = 0 if a e A+U A_. Thus z e ]^, and the result is immediate. □ Let (g, be contragredient, and let {e^,ay,f^} be a display of g and R = {]^,n, n^} the natural realization of the structure matrix A of g. The situation when J is finite and i? is a minimal realization is the most common and most important. Assuming that J is finite, we put together a number of conditions which are equivalent to R being a minimal realization. Write ^ = i2iK ® ^ for some subspace t of i). Then each f e e t induces a linear functional on <2iK by a , and we obtain a linear mapping i \ i ^ Q\IK-

Proposition 5 Let ( g , r ) be contragredient with natural realization R and structure matrix A= Assume that J is finite. Then the following are equivalent. (i) (ii) (iii) (iv)

R is a minimal realization o f A. Zg c Dg. Zgce„^. For every supplement t o f in 1^, the corresponding map i : t is injective.

Qt

Proof. Since Zg c and Dg n = 0ii< >it is clear that parts (ii) and (iii) are equivalent. (i) => (iii) We have dim finite by Proposition 4.2.2. Suppose that z e ( ^ \ G k ) Zg. Then {ai , z } = 0 for all i e J, and II induces a srt II of line^ly independent functionals on 'ii/Kz. The realization R •= {i)/Kz, n , n'^(mod Kz)) contradicts the assumption of (i). in f). Then (iii) (iv) Let t be a supplement of ker t = {z e 11 (a,, x) = 0 for all / G j}

= t n Z g c t n ( 2 K = (0)(iv) ^ (i) Let t be a supplement of in f). Since i : t -» <2k is injective and dim 0 k is finite, dim (| = dim + dim t is finite. Thus through the pairing <• , • >, induces all of ^**; in particular ii induces all the functionals of 0K- Thus we have the exact sequence Zg

^ ^ 0K

0.

350

Contragredient Lie Algebras

Now, by assumption, t n Zg = (0). Since t was arbitrary, Zg c Q'^. Thus Zg = {/z e |
is minimally realized if

MRl: it has a finite display (i.e., J is finite) MR2: any one of the conditions i-iv of Proposition 5 hold. Proposition 6 If (ind (g', ^ ' ) are minimally realized radical free contragredient Lie algebras with displays S ' = a / , j and S) = , fj)j^j tmd with the same structure matrix A, then g and g' are isomorphic by a (noncanonical) isomorphism


4.3

Embeddings, Field Extensions, and Decomposability

351

about representations that are not available in the finite-dimensional theory. For our purposes the following result will be sufficient. Proposition 7 Let be a minimally realized radical free contragredient Lie algebra, and let R be the natural realization o f its structure matrix A = [so that g = of A, i?)]. Let J' be a finite set with J c J', and let A' be any Cartan matrix indexed by J' X J' with A as a submatrix o f A' in the obvious way. Let R' be a minimal realization o f A'. Then R embeds into R' compatibly with the set inclusion J c J' and q(A, R) embeds into (¿{A', R') so that e^ e', a/ ^ / / for all i e J. Moreover, if A and A' denote the root systems of <^{A, R) and of A', R ), respectively, and we view L as a subset o f Q then A = A' n Proof Let R = be a minimal realization of A'. Set IIi — {a-ji e J} and ^ {a\^ \i e J}. It is easy to find a subspace of 1^' containing so that R^ = (l^j, IIi^) is a minimal realization of A. Then R^ embeds in R trivially, and our result follows from Propositions 2 and 6. □ Let jR = ( ] ^ , n , n ^ ) b e a realization of a matrix A over a field K, and let u(A, R) and ^(A, R) be the universal and radical free Lie algebras of (A, R), respectively. Suppose that K' is a field extension of K. Replacing by := K' and identifying 1^* inside in the obvious way, we obtain a realization R^, := ( ^ ^ , , n , n ^ ) of A over K'. We then form the Lie algebra u(A, R^ rel="nofollow">) over K'. It is routine to verify that (6) the isomorphism being canonical: i)K' ^ K' ® ^ e,

(identity m ap),

1 ® e¡,

fi ^ 1 ®/iIn addition by Proposition 2.7.4, rad(K' ®|)^u(/l, i?)) = IK' ®||^ rad u ( A , R),

352

Contragredient Lie Algebras

and hence through the isomorphism (6), rad(u(^,i?K')) = K'

radu(/l,i?),

which leads to q{A,

(7)

= IK'

i?),

with IK- ^ IK' ®K

( identity m ap),

1 ® e¡, ^ 1 ®/iIf a contragredient Lie algebra q(A, R') over the field IK' has a subalgebra g (^ , R) over IKsuch that q(A, R') = IK' ® R), then we say that q(A, R) is a IK-rational form of g(yl, R'). Given a square matrix A e IK^^'*, we define the skeletal graph of A to be the graph F whose nodes are indexed by J and in which the nodes i and j are joined by an edge from i to j iff A¡j 0 oi Aj¡ ^ 0. (In Chapter 5 we define the Coxeter-Dynkin diagram, which is a more elaborate version of this; see also Section 3.4.) The connected components of F correspond to the minimal nonempty subsets of J such that A¡j = A¡¡ = 0 whenever i e j e p ^ q. The submatrices A^^^ defined by the subsets of J are called the indecomposable blocks of A. A is indecomposable if F is connected (so that there is only one block). In all cases of any importance to us we will find that A¡j =/= 0 <=»Aj¡ ^ 0, and these simple notions of connectivity are sufficient. Proposition 8 Let R b e a realization o f a matrix A e IK-*^-*, let F be the skeletal graph of A, and let g = g(yl,f?). Let J = be a partition of J so that the subgraphs F^^^ corresponding to the subsets are mutually disconnected (i.e., A¡j = 0 = Aj¡ whenever i e j e p q). For each p ^ P, let R*'”^ be a realization o f the submatrix A^‘’^ ■■=(A¡j)¡ yej«’» so that R^'’^ is a natural realization o f A^'’'>in the context o f R {see Remark 1). Identify the radical free Lie algebra g^^> == q(A^’’\ R^>’'>) as a subalgebra o f g by Proposi­ tion 2. Then (0

9^= X ^ ^ ^ g V ’), g_=

(ii) D g = X^^^Dg<^>, (iii) g = Eg^^^ + where

is the diagonal subalgebra o f g.

43

Embeddings, Field Extensions, and Decomposability

353

Proof. Let p, q e P, p ^ q, and let i e j e Then [/„[e,., effi = -[«y, Cj] = -AjiCj = 0. Similarly [fj, [e„ Cj] = 0, and it follows at once that [e,,Cy] e rad(g) = (0). Since the a„ i e J, are linearly independent in we see that [g(f> n = (0). We have just seen that [g^/\ = (0) if p ^ q, so we have proved the first part of (i). The other follows in the same way (or one may use cr). Since Dg^^^ n = 0 and since Dg n i) = <2k = we may use Dg g"©(Dg n 1^) © g"^ to see that part (ii) follows from part (i). Now part (iii) is immediate. We call a square matrix A combinatorially symmetric if for all i and j in J we have A:: ¥= 0

(8) and

(9)

Aji = 0

whenever

= 0.

Proposition 9 Let A be combinatorially symmetric, and let R = of A.

be any realization

(i)

I f A is indecomposable, then any ideal o f q(A, R) is either inside ij or contains Dg. (i) If J is finite and f) = Q ^, then the decomposition o f ^ = ^ defined by the indecomposable components o f A is a decomposition of g into simple ideals. In particular g is simple whenever A is indecom­ posable. Proof (i) Let a be an ideal of g. Then a = ea", where a“ = a n g" c a and a" ¥= 0 for some nonzero root. Without loss of generality we can assume that there is an jc e a" with a e A+, x ¥= 0. Since rad(g) = 0, there is a sequence of elements ..., where fj. e g~“'j, i^,. . . , i^ ^ J, such that 0 [fi^,. . . , fi^, x] e i). Then [f^^,, , , , f- x] e (IK \ {0})ei^ e a. Let Jq := {j e J |ej G a). Since [ej,[fj,ej]] = [aj'^jeJ = A^ej it is evident that J q indexes a union of connected components of r ( ^ ) . Thus J q = J. From ej e a we obtain [fj, ej] = - ci f , and [fj, = Ajjfj are both in a. Thus fj e a for all j e J, and hence a d Dg. (ii) Since ^ = Q k , we have g = Dg. Assume first that A is indecompos­ able. Since J is finite, dim(0K*) = card(J), and evidently II is a basis for

354

Contragredient Lie Algebras

0IK* = 5*- Then, given e f), h 0, there exists an i e J, for which [h,e¿] = ce^ 0. Thus any ideal of g containing h contains some root space g“‘ and with what we have proved in (i), this shows that g is simple. In general let J = t>e the decomposition of J into subsets labeling the connected components of the skeletal graph of A, For each p e P we have Kaj

and := (a e r I a

= 0 for all q ^ p) =

.

Set = {i>:y};sj(p) c There is a natural em­ bedding of == ( 2 k n<^>, into R. With Q^P'> ■■= g((^,y), ye we have = Dg^^\ which is simple by part (i). Now by part GO of Proposition 8, g=xg<^>. □ We finish this section by relating Kac-Moody algebras to the finite-dimen­ sional semisimple Lie theory. Proposition 10 Let A be a Cartan matrix o f finite type, and let Rbe a minimal realization of A, Then (i) the Lie algebra g = %{A, R) is, up to isomorphism, independent ofR; (ii) g is finite dimensional', (iii) g is semisimple with simple ideals corresponding to the indecomposable blocks o f A; in particular g is simple if A is indecomposable. Proof See Exercise 4.1.



Let A be an indecomposable (resp. decomposable) Cartan matrix of finite type. Let jR be a minimal realization of A. Then g = g(-^4, R) is called the split simple (resp. semisimple) finite-dimensional Lie algebra over K with Cartan matrix A. Remark 6 It is a fact that if IK is algebraically closed then every finite­ dimensional simple Lie algebra over IK is of the form g(-^4, R) A indecom­ posable, as above. Over nonalgebraically closed fields there are (in general, many) other possibilities.

4.4

4 .4

Invariant Bilinear Forms

355

INVABIANT BILIN E AR FORM S

We wish to find necessary and sufficient conditions for a contragredient Lie algebra to carry a nontrivial symmetric invariant bilinear form. We formulate an existence theorem in the general context of Z-graded Lie algebras. Let 9 be a Lie algebra over IK graded by Z, g = ® * ^ k eN define q{k) = 0 9'. Uls/t A bilinear form (• 1•) : 8 (* ) X g(*) ^ IK will be called locally invariant if ( [ y , ^ ] U ) + ( x | [ y , z ] ) = 0,

or equivalently ([^ ,y ]U ) = (xl[y ,z])

for all x , y , z ^ g(fc) for which [x, y] , [ y, z] e g(fc).

Proposition 1 Let g = exists h ^

^ Z~graded Lie algebra over IK, and suppose that there such that for both e = 1 and e = —1, ^ generated by Suppose that

(1)

Xg(/i)

is a symmetric locally invariant bilinear form satisfying (2)

( qM qO "" (^)

^ j ^ Q for alii J with 1/|,|;| < h.

Then (* I *) extends uniquely to a symmetric invariant bilinear form on g satisfying (2) for all i, j e Z. Proof We extend (• | • ) to g(n) X g(n) for all n e Kl, az > /z by induction on n. Assume that (• | • ) is defined on g(n - 1) and is symmetric and locally invariant. We have to define ( I*) on g(n). In view of (2) we define (g"*"" I gO = (0) and (g* I g^") = (0) unless i = +«. It remains to define

Contragredient Lie Algebras

356

(• I *) on g - " X following

At this point we interrupt the proof to establish the

Claim Let / , k, I be integers satisfying 0<

(3)

i + / = ±n,

(4)

< n,

|i|,l;U A :U /l

k + I = +n.

Let u‘, v \ w*, z ‘ be elements of g', g^, g*, g^ respectively. Then (5)

I z ') = ( m‘ | [ u^ [ h'* , z ']]).

Proof (of Claim). Notice that i + j + k + I = 0, and hence |i + j + A:| = 1/| < n and \J + k + l\ = III < n. Thus both sides of (5) make sense. Also notice that |i + ¿1 = I; + /| < n and that \j + k| < n. We have

([[«',

|z') = ([[u‘,H'*],y']

\z‘ ) +

([«', [u^,vv*]] |z')

= ([[u',H'*^]|i;^z']) + (M'|[[i;^w*],z']) = {u‘ \ [ w \ [ v f z ‘]]) + {u‘ \ [ [ vf w' ^ ] , z ‘]) = (^г‘ |[ t^ ^ [ н '^ z '] ] ) . This establishes the claim.



Now let X e g^", y e g“®", where e = ± 1. We want to define (jc | y). By assumption for some k , m ^ Nv/e can write

x=

T , [ x ' j , x ' ; ] , y = H[ y ' j , y " ] ,

;=i

;=i

where the x), x] e ©"^j g^‘ and the y], y'J Define ( 6)

( x \ y ) ■■= Z { [ x , y ' j ] \ y j ) .

y=l To see that (6) does not depend on the way in which y is decomposed, we

4.4

Invariant Bilinear Forms

357

observe that

(7) k

\

m

k,m

E { x' i , x'l]\y ( j: I y ) = E ([x, y'j] I yj) = E /=1 ; =1 i,j=l

( [ [ ^ :,

x'[], y'j] I yj)

k,m

= E (^il[<.[y;,y;]]) i.j=l

(by the Claim)

= E (jc;i[< .y]) /=1 and hence that (6) depends only on y as desired. To see that (• h ) is symmetric, we reason as follows: m

( ^l y) = E

[by (6)]

y=l m

= - L (y" I[y). ^]) ; =i

[by symmetry on %{n - 1)]

= E ([y;,y;]i^) ; =1

[by (7) interchanging x and y]

= (yU ). It remains to be shown that (• | • ) is locally invariant on g(n). For this it will suffice to show that ([x, y]| z) = (x l[y, z]) for homogeneous elements X, y, z, where 0 < |deg(x)|, |deg(y)|, |deg(z)| < n, degix) + deg(y) + deg(z) = 0, and at least one of these degrees is ±n. If deg(x) = ±n and 0 # deg(y), 0 ^ deg(z) the invariance follows from (6). The same applies if 0 ¥=deg(x), 0 deg(y), and deg(z) = ±n. There remain three cases: Case 1. 0 < |deg(x)|, |deg(z)l < n, deg y = ±n, deg([jc, z]) = Tn, ( [ A t , y ] U ) -----( [ y , x ] | z ) = -{y\[x,z])

[definition (6) on [;c, z]]

= (y\[x,x]) =

[by (6)]

= (x,[y,z])

(by symmetry).

358

Contragredient Lie Algebras

Case 2. deg(jc) = ±n, deg(y) = Tn, deg(z) = 0. We may assume that x has the simple form [ jc' , x "], 0 < |deg(x')l, |deg(A:")l < n. Thus ( j : | [ y , 2 ] ) = ([j c',JT "]l[y ,z])

= {x'\[x",[y,z]])

[by (7)]

= ( x ' \ [ [ x " , y ] , z ] + [y,[^:",2 ]])

(by induction assumption and case 1) = ([x', [x", y]] I z) + ( [ [ a;', y], x"] 1z) (by induction assumption) = ([^>y]lz). Case 3. deg(jc) = ±n, deg(y) = 0, deg(z) = H-n. Then we have ( x | [ y , 2 ]) = - ( [ a: , z ]| y) = ( z |[ jc ,y ] ) = ( [ j c , y ] | z ) , using case 2 twice and the symmetry of (• 1• ). This completes the induction step. We turn our attention to contragredient algebras. Let (g, be contra­ gredient as in Section 4.1 and maintain all the notation that was established there and in Section 4.2. Proposition 2 Let g be contragredient as above, and let (* I *): 9 X g ^ IK be an invariant bilinear form. Then (0 ( 9 “ I 9^) = (0) for all a, p Ei Q such that a + j8 ^ 0; (ii) for ( ' \ ' ) to be nondegenerate, it is necessary and sufficient that the restriction o f to 9“ X g~" be nondegenerate for all a ^ Q; (iii) (• I • ) w symmetric on Dg X Dg. Proof, (i) Let a, /3 e

and let jc e g“, /i e 1^, and z e g^. Then

( [ x , h ] \ z ) = ( x \ [ h , z ] ) <=> (/3 + a)(/z)(jc I z) = 0. Since h is arbitrary, this shows that (jc | z) = 0 unless ¡3 = - a , thus estab­ lishing part (i). Now (ii) follows from (i).

4.4

Invariant Bilinear Forms

359

(iii) Let jc e g", y e g“"* for some a e II. Then [x, y] e Ka ^ and ([ji :,y ]| a'' ) = (y l[a'^,Jt]) = 2(y U ) and ( [ ^ . y ] ! « ' " ) = ( ^ l [ y , « ' ' ] ) = 2( j ; | y ) . Let (• 1• )' be defined by (x \ y)' = (x | y) —(y 1x). Then (• I * )' is invari­ ant and vanishes on g“ x g““ for each a e II. By part (i) we see that both g“ and g““ lie in the radical of (• | • )'. Since the radical is an ideal of g, it follows that ( • ! • ) ' vanishes on the ideal generated by the g“ with a e ±11. This ideal is precisely Dg (Proposition 4.1.12). □ An invariant bilinear form (• | • ) on a contragredient Lie algebra (g, is called proper (relative to if (• 1• ) restricted to g“ x g““ is nondegener­ ate for each a e II. A contragredient Lie algebra (g, is called invariant if there exists a proper invariant bilinear form (• 1• ) on g relative to Notice by part (iii) of Proposition 2 that such a form is necessarily symmetric on Dg. Normally it is quite irrelevant whether such a form is symmetric on all of g. Invariant Kac-Moody Lie algebras are often referred to in the literature as symmetrizable Lie algebras. Proposition 3 Let (g, c^) be invariant contragredient with proper invariant form (• | • ) and structure matrix A. Then relative to any display {e^, ay, j> («<• I

= («; Ifj)Aji

for all i, j e J.

Furthermore the quantities (e, | /¿) are nonzero. Proof. We have

= (« M [« ;./;])

= ([«/>//] I[«;>/;]) = {ei \ f i ) Ai j . By the definition of proper and CTl we see that (e, | /^) =5^ 0.



Contragredient Lie Algebras

360

A matrix

e is said to be symmetrizable if there exists a family such that for all i and j in J,

Notice that if J is finite, then this can be interpreted as stating that A • diag(£y) is a symmetric matrix. This concept generalizes the one defined in Section 4.3. Restated, the last proposition says that a contragredient Lie algebra is invariant only if its structure matrix is symmetrizable. The structure matrix of such an algebra may be symmetrized using e¿ = | for all i. Remark 7 If ^ is symmetrizable then evidently = 0 if and only if A ji = 0. Thus A is combinatorially symmetric (see Section 4.3). If A is indecomposable, then the set {ej} is uniquely determined up to a scalar multiple. Furthermore the {gy} may be taken in the smallest subfield of IK containing all of the A¿j/Aj¿, Aj¿ ¥= 0. If the A¿j all lie inside a subfield of R and for all i and j both A¿j and Aj¿ have the same sign, then all the e¿ may be taken of the same sign, for instance, positive. As a matter of convention we will always assume that the > 0 in these circumstances. In particular this holds for Cartan matrices. If A is decomposable, then these remarks apply to each of the individual blocks of A. Let (g, be a contragredient algebra with structure matrix A. Our aim now is to show that if A is symmetrizable, then g is invariant. Suppose then that A is symmetrized by {fylyejDefine a surjective linear mapping ( 8)

(•) :Ö ,

by linear extension of a¡

af ■■=e¡a'^.

By means of (• )^ we define a bilinear mapping

as follows: (9)

(a® I/i) := ,

/z e f).

Notice that ( a ?

I tty)

=

=



A¡jSj

and hence that ( • | • ) is symmetric on

=

=

< a,-,e y a />

A j ¡ £¡

=

[aj

X Q^.

I a ? )

4.4

Inyariant Bilinear Forms

361

We may define (• | • ) on X by (9) and symmetry. It is irrelevant how we define (• | • ) on the rest of X 1^. We take 1^' to be any supplement of ¡2k in and define (• | * ) on 1^' x to be symmetric but otherwise arbitrary. Remark 2 We note that the nondegeneracy of < • , • > implies that for each a« # 0 in Q^, (a° | i)) # (0). Example 1 '

A =

2 -2 0

-1 2 -1

0 -2 2

is symmetrized by /1

diag{ 1,2,1} =

Since the row rank of A is 2, we extend A using Proposition 4.2.1 to '

2 -2 0 0

-1 2 -1 0

0 -2 2 1

o' 0 1 2J

Write ft = IKai'^e IKa^®

Kd^

and ft'^= K«! ® lKa2 ® IKtts ® Kd, with the last matrix defining the pairing. In the notation above. = 2«2",

«? =

• ) in the basis {aj, '

2 -2 0 0

-2 4 -2 0

where * is the arbitrary choice for id '' |

«3

== «3"

a ^,d 0 -2 2 1

O' 0 1 *,

Contragredient Lie Algebras

362

We now return to our contragredient algebra g. Define a Z-grading on g by setting g" = ®ht(a)=/z9“* definition of contragredient, g is gener­ ated by g“ ^ 0 0 g^ = g(l). We introduce a symmetric bilinear form (• | •) on g(l) by (10a)

( • 1•) on

(10b)

(g“ l 9^) = 0

defined as above. ifa,p^Q ,a + p^0.

(10c) [x, y] = (x I y)a^

( ^ i)) whenever a e g , jc e g“ , and y 0 g"“.

Of course at this point (10b) and (10c) only say anything if |ht(a)| = |ht(/3)| < 1. It is easy to see that (• | • ) is symmetric and locally invariant on g(l). For local invariance there are only two distinct nontrivial cases that need to be checked: Let a: e g“, y e g““ (a # 0), and let h

Iy)

= ~{a,h){x

Iy) = (x |[/î, y]),

([jc ,y ]l^ ) = (jcl y ) ( a ° |/i) = ( j:| y ) { a , h ) = (J il[y ,/i]). Proposition 4

Let ( q, be contragredient, and suppose that its structure matrix A is symmetrizable by Let (O ^ i G ik ^ be defined by (8) above. Then there exists a proper symmetric invariant bilinear form (• I *) on g with the following properties: (i) (a? I a?) = A^jSj for all i, j ^ 3 and (a® \ h) = ( a , h ) for all a s and h GO [* I * ] : 9“ X g““ -> f o r a l l a ^ Q a n d [ jc, y] = ( x \ y ) a ^ f o r e g“, y e g"“. (iii) (9“ I 9^) = (0) if a + p 0, (iv) (• I • ) a-invariant.

a ll

Furthermore, if rad(* I • ) == {a: e g l(x 1 g) = (0)}, then rad(* | • ) w a graded ideal of g, and ra d (- 1•)

n 0 g“ = rad(g),

rad(* I •) n f) c Z (g). Thus rad(* | • ) c n(g) {see Section 2.7).

4.4

Invariant Bilinear Forms

363

In particular, if g is radical free, then the restriction o / (• 1 • ) io g“ X g ^ is nondegenerate for all a ^ A \ {0}. Proof The existence of (* I • ) on g satisfying part (i) follows by defining ( I ) on g(l) using (10) and then applying Proposition 1. Part (iii) is immediate from Proposition 2. To establish part (ii), note that with a: e g“, y e g"“, [x, y] e (Proposition 4.1.12). Thus for all h œ Î). {[^^y] - { x \ y ) a ^ \ h ) = { x \ [ y , h ] ) - ( x l y ) ( a ^ |/ i ) = ((A: I y) - ( x \ y ) ) = 0 Remark 2 then shows that [ a:, y] = ( jc | y)a°. Now part (iv) follows from parts (ii), and (iii). Set ê = {;c G g |(jc I g) = (0)}. The invariance of (• | • ) implies that ê is an ideal of g. In particular ê is graded. Let 5“ e ê be homogeneous of degree a, a e Q. If a ¥= 0, then [5“, g““] = (5“ | g“"")u:° = (0). Now, if the ideal ad(U(g))i“ of g generated by s"^ meets \ {0}, then there is an element u e U(g)"“ such that ad(w)5“ ^ ^ \ {0}. Then ad(M)5“ e Ô kXÎO}. Choosing h si} with (ad(w)i“ | /z) ¥= 0 and using the invariance, we have (5“ | g““) ^ (0), which contradicts the above. Thus 5“ s rad(g). On the other hand, if a = sO, then for all )3 e A, <)8, 5“) = (/3° | 5“) = 0, and hence [5“, g^] = (0). Thus 5“ e Z(g). This shows that ê c rad(g) + Z(g). Finally, if x s rad(g) is of degree a ¥= 0, then [;c, g”“] = (0), and therefore x s ë by part (ii). □ Remark 3 It is remarkable that g“ X g““ is one dimensional for nonzero a when A is symmetrizable. This need not happen if A is combinatorially symmetric but not symmetrizable [Sg]. Proposition 5 Suppose that (g, «^) is a minimally realized contragredient Lie algebra and that its structure matrix is symmetrizable. Then any invariant bilinear form (• I • ) on g defined by Proposition 4 is nondegenerate on f). In particular, if g is radical free, then (• 1• ) w nondegenerate on g. Proof Let h s i ) . Then, using Proposition 4, (i)l5) = (0) => /1 e rad((-l • )) => h s Z(g). Since the realization is minimal, h s (Proposition 4.3.5). Thus we can write h in the form for some a in Finally, (0) = (/z 11^) = (a° I ]^) = (a,i}) by (9), and hence a = 0, Thus h = 0, If A is symmetrizable with

364

then

Contragredient Lie Algebras

is symmetrizable with = {A^)ns7^^

We may apply the construction of ( • I * ) on realization

carried out above to the dual

/? ^ = (r,n \n ), which is a realization of Æ . Thus we begin with a linear map

defined by (a,y) Evidently this is just the inverse of the operator ( •)^ we defined above. We denote it again by ( •)^, since no confusion usually results: ( 11)

(.)0 Qk - ^ Q k -

We now define (• | • )* on There are several ways in which we can do this. Following the same process as above, define (• | • )* on 1^* x by ( 12)

Extend (• I • )* to <2k ^ t)y symmetry and to all of 1^* X 1^* in some arbitrary way as before. However, if is finite dimensional and (• | •) is nondegenerate on 1^ (for example, if (g, ,5^) is minimally realized) then we can use (• | • ) to construct an explicit isomorphism a> between ^ and 1^*, namely (ifcl-) We can then use this isomorphism to transfer (• | •) to 5*, thereby obtaining a nondegenerate bilinear form (• | • )* on This is precisely the way in which the Killing form is moved over to in the finite-dimensional case. Let us see that this process produces (•!•)* satisfying (12). Let a e Q^. Then a° ^ and under the isomorphism a>, (a ° | •). From (9), (a° I /i) = { a \ h } for all h showing that o)(a°) = a. Then co\q^ is the inverse of (-)°, which we had agreed to also call (-)°. We now extend ( )®to all of Í) by declaring (-)° = w. Thus (1 3 )

( k° , h} = ( k \ h )

for all A:,/i e ]^.

4.4

Invariant Bilinear Forms

365

Kxr (*)^, then for all a, ¡3 ^ if*. If we also agree to denote o).-1^ by (p\af = (14)

= (^° 1a**) by definition of (• | ' )* = <j800,«o>

by (13)

= . From this (12) is obvious. Whenever dim is finite and (• | •) is nondegenerate we will assume that (• I • )* is defined in this second way. In particular (13) and (14) hold. In any case we always have (13')

(k^,h) = ( k\ h)

(14')

(jS la)* =

forall

e fi,

for a ll/3 e fi*, a e 0 k -

Henceforth we write ( • I •) instead of ( • 1• )* [thus both ( )° and ( • 1•) now have double meanings]. We summarize our conventions and notation in the following: General case (•)“ w n IBFl 0 K - 0 ^ , : « ? = s , V IBF2 for all A: e 0;^, A e ( k\h) = (k°,h) IBF3 for all a e 0,^, /3 e (/3| a) = IBF4 (a,-1a,) = 2e,IBF5 ( a r |« r ) = 2 e r ' IBF6 Si > 0 for all i if the matrix A permits this IBF7 Si e Q for all i if the matrix A permits this

dim 1^ finite, (* | -) nondegenerate (•)“ for all k , h (k\h)=(k^,h) for all a, p ^i )* (/3|a) = <^,a°> a,^= 2af/(a,-1 a,); a, = 2 (« r)V (« r 1« r);

A selection of the diagonalizing constants e, for a symmetrizable matrix A together with a symmetric bilinear form (• | •) on g and another one [also denoted by (• | •)] on for which the conditions IB Fl-6 hold is called (by abuse of language) a standard invariant symmetric bilinear form on g.

Contragredient Lie Algebras

366

Proposition 6 Let (9, be an invariant contragredient Lie algebra, and let (• | • ) be a standard invariant symmetric bilinear form on g. Then (0 Gad acts as a group of isometries o f g relative to (ii) Whenever aj rj acts as the reflection in a j (resp, af) on {resp, 1^*) relative io (* 1• ), that is, rj{h) = h 2{a\ a¡)

(hi)

forallh^íj,a^íl'^;

W acts as a group o f isometries on

{resp. 1^*) relative io (• | • ).

Proof Gad is generated by elementary automorphisms, and these act as isometries on g relative to (• | • ) by Proposition 1.7.1. For we have Vjih)

=h

-

=h -

{ a j \ h ) a J = h -

2 ( a /

1

(«9 I

V

IBF2)

I / )

(bylB FlandlB FS).

and, mutatis mutandis, ry(a) = a —2((a | aj)/(aj \ aj))aj. This proves part (ii). Now part (iii) follows from parts (i) and (ii), together with the definition of W (Section 4.1). □ From IBF7 we see that (ala) e Q for all a ^ Q. Proposition 7 Let (g, «^) be an invariant Kac-Moody Lie algebra, and let (• | • ) be a standard invariant symmetric bilinear form on g. Then (i) (a I a) e {(«. | a,) | / e J} c Q_^ for all a (ii) ( a |a ) < 0 / o r a / / a e ^ '”A, (iii) for all a e A, a e'"*A <=> (a | a) < 0. Proof Part (i) is clear from the PT-invariance of (* | • ) while part (iii) then follows from part (ii). Let a e'^^A. We may assume, without loss of general­ ity, that a e^'^A^. Since Wa c^'^A^. (Proposition 4.1.5), there is no loss of

4.5

Casimir-Kac Operators

367

generality in further assuming that a is of minimal height. Then for all i e J, ht(r^a) > h t(a) => ( a ^ a ^ ) < 0 => (a | a¿) < 0, so clearly (a | a) < 0 since a e A+.



Let i? = (]^,n, n ^ ) be a realization of the Cartan matrix A, An element p e ]^* is called a minimal regular weight if for all i ^ J, ( p , a ^ ) = 1. If is a basis of 1^, then of course p is unique. Minimal regular weights appear many times in semisimple Lie theory and in many places later in this book (e.g., in Section 4.5). The terminology comes about as follows: In the most important representations of a Kac-Moody algebra the weights are integral: elements A g 1^* satisfying ( A , a ^ ) g Z, for all i g J. Of these, the dominant weights are those satisfying (A, a ^ ) g N for all i g J, and the regular weights are those satisfying, for all / g J, (A, 0. Thus the “minimal” (dominant integral) weights are those satisfying ( A , a ^ ) = 1 for all i G J. Suppose that A is symmetrized by ^ j and (• | • ) is a bilinear form on 1^* satisfying the conditions IBF. Suppose that p is a minimal regular weight. Then (15)

l

=

<

p

, a

r >

=

P l

2a,- \ (a, I a,) /

2(p 1a,.) (a,. | a,) '

Thus 2(p I a,) = (a, I a,)

for all i e J.

Remark 4 Let A be an indecomposable Cartan matrix of finite type, £nd let g = g(y4, R) be the corresponding split simple Lie algebra over K. If IK is the algebraic closure of K, then by Section 4.3 g(.i4,/?jj^) = (K®j^g(^, i?), and hence g is central simple (Exercise 1.7). Hence any standard invariant bilinear form on g is a multiple of the Killing form. 4.5

CASIMIR-KAC OPERATORS

I have heard statements that the role of academic research in innovation is slight. It is about the most blatant piece of nonsense that it has been my fortune to stumble upon. Certainly, one may speculate idly whether transistors might have been discovered by people who had not been trained in and had not contributed to wave mechanics or the theory of electrons in solids. It so happened that the inventors of transistors were versed in and contributed to the theory of solids.

368

Contragredient Lie Algebras

One might ask whether basic circuits in computers might have been found by people who wanted to build computers. As it happens, they were discovered in the thirties by physicists dealing with the counting of nuclear particles because they were interested in nuclear physics. One might ask whether there would be nuclear power because people wanted new power sources or whether the urge to have new power would have led to the discovery of the atomic nucleus. Perhaps—only it didn’t happen that way, and there were the Curies and Rutherford and Fermi and a few others. One might ask whether an electronics industry could exist without the previous discovery of electronics by people like Thomason and H. A. Lorentz. Again it didn’t happen that way. ... Or whether, in an urge to provide better communication, one might have found electromagnetic waves. They weren’t found that way. They were found by Hertz who emphasized the beauty of physics and who based his work on the theoretical considerations of Maxwell. I think that there is hardly any example of twentieth century innovation which is not indebted in this way to basic scientific thought. —Henrick Casimir

Throughout this section (g, will be assumed to be invariant contragredi­ ent and radical free. We endow g with a standard invariant symmetric bilinear form (• I •): 9 X g

We also recall that (■ I ■)l8“xg-<' is nondegenerate for all a e Q \ {0}, since g is radical free. As in Section 4.4 we also denote the corresponding bilinear form on 1^* X f)* by

The category <^(g, 5^) of Section 2.5 will be denoted simply by 0 , We plan to construct what, in the language of categories, would be called a natural transformation from the identity functor to itself. In plain language this means that NTl: for each module M < 0 , we have a g-module homomorphism (or operator)

4.5

Casimir-Kac Operators

369

NT2: for all M and N in ^ and for every g-module homomorphism f : M - ^ N , the following diagram commutes M -^M i f fi N -^N This leads to a family {F^}m of operators that plays a crucial role in most of the subsequent theory. The construction of these operators depends on the existence of the symmetric invariant form (* I • ), and this accounts for the considerably less developed theory of Lie algebras q(A, R) when A is not symmetrizable. Recall that dim(g“) < oo for all a ^ Q \ {0} (Proposition 4.1.1). The nondegeneracy of the pairing g“ X g““ implies that if = [x^,. . . , is a basis of g“, then there exists a unique basis = [y^,. . . , y„} of g~“ such that I yj) = 8^j, The bases B^ and B_^ are then said to be dual to each other. Lemma 1 Let a Ei Q \ {0}, and let {x^,. . . , and {y^, ...,y^} be bases o f g“ and g"“, respectively, so that these bases are dual to each other. Define y “ — ® G g 0 g and T“ = g U(g). Then (i) y“ and T“ do not depend on the choice o f dual bases o f g“ and g""^. (ii) I f u E and V E g““, we have n

M= L 1=1 n v =

E

IX i ) y t ,

(«k) = E 1=1 (iii) Let a, a' e <2 \ {0}, and let r “ and y “' be written in the forms T,%\yj ® Xj and ® x'k, respectively, with respect to some pairs of dual bases. Then for all z e 9“ “ Itave

E [yit, z] ® 4 = E yy ® [ ^ . 4 ] ^=1

7=1

9®9

Contragredient Lie Algebras

370

and

'L{y'k^AA= k=\

in U (g ). ;= 1

Proof. Part (ii) is an immediate consequence of the fact that the bases {jCj,. . . , jc„} and {yj,...,y„} are dual to each other. If and are any other two such bases then, by means of part (ii), we obtain

HY¡®X¡= i= \

E

E

y¡{Y¡ Ix¡)

® E (yj k= \

¿= 1 \ ; = 1

=

E

E(5^-

j , k = \ \i = l

=

hkyj ®x„

E j,k = l

=

' Lyj ^Xj , j

thereby showing that y “ is independent of the choice of dual bases. Next we use the linear map g <8> g U(g) given by x <8) y to finish the proof of part (i). For part (iii) we define a symmetric bilinear form (*, • ) on g ® g by (x (8>y, x' <S>y') = (x Ix ') ( y I y ').

Because of analogous properties of (• I • ) it is easy to see that for all a, a', j8, j8 'e (2 \ {0},(*, • ) determines a nondegenerate pairing between g"" <8) g^ and g“' <S> g^' if a + a' = 0 = + j8' and (g“ (S> g^, g“' 0 g^') = (0) otherwise. It follows that in order to establish the first assertion of part (iii), it will suffice to show that

E

k=l

[y*>

z]

E

j~l



®

[ z, Xj ] , a

® 6| = 0

for all a e g" and

e g

4.5

Casimir-Kac Operators

371

By definition, the left-hand side of the above equals

k=l

J=l

m

= E k = l

n

+

(yy I

I[z, b])

[because of the invariance of ( • | •)]

y= i = { [ z \ a ] \ b ) 4- ( a \ [ z , b ] ) = 0. For the second assertion of part (iii) we again apply the natural map g ® g U(g) with x y xy to the assertion we have just established. □ Let p e Section 4.4). Let M e

be a minimal integral regular weight fixed once and for all (see We define the operator r

where

and



discussed in the introduction by + V'

are two operators defined as follows:

Definition of Let M = be the weight space decomposition of M. Then is defined so that F^ acts on each weight space as multiplication by (p, + p I p + p) —(p I p) = (p + 2p | p). Definition of F^ View M as a left U(g)-module. Then for each a e 0 \ {0} the element F“ e U(g) acts on M. We denote this operator by F^ and define

Although the sum in the definition may be infinite, it makes perfect sense as an operator. Indeed, if A e P(M ), then the set {a G (2+ I A + a e P ( M ) } is finite (Lemma 2.6.1). Hence there exists only a finite number of a e A+ such that r “(Af^) # (0).

Contragredíent Líe Algebras

372

Thus is well defined on each weight space of M. Notice, however, that need not be determined as an operator by some element of U(g) if A+ is infinite. Finally, we observe that both and are graded operators; that is, they apply into for every weight space of M. Thus + F^ also has this property. The operator is called the Casimir-Kac operator of the g-module M. Of course, depends on the initial choice of p but for our purposes a single choice of p suffices, so we do not record it in the notation. Proposition 2 [Ka2] Let M e

Then F^ commutes with the action of g on M.

Proof Since acts on each weight space of M as scalars and graded, it is clear that commutes with the action of on M, Thus it suffices to show that the action of F^ + Fj[^ commutes with that of each and /y for all j e J. For simplicity we omit the subscript M in the rest of the proof. Let V e M^. We have (1) ( r % - e^r°)

■V = { { f i +

aj

+

2p\n

+

aj) -

(p. +

2p\ p)}ej ■ v

= {{p + 2p I aj) + [aj I p + aj)]ej ■v = {2{p I a,.) + {aj I aj) + 2{p \ aj)]ej ■v

= 2[p + aj I OLj)ej • V, where we have used (4.4.15): 2(p 1 ay) = (ay | ay). Similarly (2) (r° // - /yr°) ■V ^ [{p - aj + 2p \ p - aj) - ( p + 2p \ p ) ] f j ■v = - 2 { p \ a j ) f j ■V .

Next we compute the commutator of F' and Cy, in two parts. We have F“^ = efej where ef e g is such that {ef \ Cj) = 1. Since af = Cy«/ = [-Sjfj, Cj] = i - £ j f j I CyX-tty) (see IBF and Proposition 4.4.4), we conclude that ef = ejfj.

4.5

373

Casimir-Kac Operators

Then (3)

2 ( r “>e^. - c / “/) • V = 2ej{fj • ej ■ej ■v - Cj • fj ■ej ■y) = - I s j a y - €j ■V = -2ej(iJ. + a j , a j ) c j ■v = - 2 [ i i + Uj I aj)e^ • V.

Following along similar lines, we show that (4)

2(F“^X - fjT-j) ■v = 2{^\ aj)f, ■v.

Comparing (1) and (3) and (2) and (4), we see that to establish the proposi­ tion we need only show that

E

r-

ae A+\{«;} commutes with the action of ej and fj for all j e J. It is useful to note that if a E A+\{ay}, then either a — aj ^ A or

a —

A+\{ay}.

e

since 2«y ^ A. Let {x^ f^} and be bases of g“ and g““ that are dual to each other. Here k e K ia), where K(a) is some finite set. It is convenient to define K(a) = 0 if a E A^_. We have (5)

(

E

E

T“e , - e ,

' aeA

q: e

=

E a sA AK >

=

E

A

E

(y-a,k'Xa,k- ej-V

V)

k s K (c c )

E

+

aeA+\{ay} k^K{a)

where we recall that only a finite number of nonzero terms occur in this sum. By part (iii) of Lemma 1 with a' = a + aj and z = we see that

E k '^ K ia ')

= E k ^ K ( a )

y-c.kUj^X^j,].

374

Contragredient Lie Algebras

Thus for any a ^ the (finite number of) terms involving roots in a + laj cancel out in pairs. After cancellation, any remaining terms involve roots a for which a + ay ^ or a —ay ^ A I n either case the offending terms are clearly zero. This shows that the left hand side of (5) equals 0 as desired. A similar trick can be used to show that L

T“

A+\{ay}

commutes with the action of

/y.

This finishes the proof of the proposition.

Coming back to the two properties that we wished T to have, we see that NTl is now proved. As for NT2, suppose that f : M ^ N is g-module homomorphism. Then / : for all weights ii, and for x e it is elementary to check that /(T ^(x)) = T^(/(x)). Proposition 3 Let M e and let

T) be a highest weight module with highest weight pair be its Casimir-Kac operator.

(0 acts on M as the scalar (A + 2p 1A). (ii) I f N is a submodule of M and p is a primitive weight relative to N, then (A + 2p I A) = (p. + 2p 1p ). (iii)

I f p.

and [ M : L(p)] > 0, then (A + 2p | A) = (p + 2p | p).

Proof Let u e U(g). By our previous proposition we have T^u • V = uTm • V = u ■{ r ^ -

v

)

= ( A + 2p\ A)u • v.

Since U(g) ■v = M, part (i) follows. For part (ii), choose w e with w ^ N but w (z N. Then w == w + N is 3. highest weight vector of weight p for M/ N. It generates a highest weight submodule U(g) • w of M/ N, and hence by part (i), ru(8)i5>(^) =

= ( p + 2 p lp )w .

On the other hand, if ir: M -» M / N is the canonical map then = ( A + 2p I A)ir(w) by part (i) and NT2.

4.6

The Radical Theorem

375

Finally, if fji and [ M : L ( ) ] > 0, then given any local composition series {MJ for M at L(/i) occurs as some factor Any weight vector in Mj that is the preimage of a highest weight vector of L(/a) is a primitive vector of weight /x (Lemma 2.6.3(iii)). Then (A + 2p | A) = (/x + 2p I /x) proving part (iii). □ ijl

Remark 1 For finite-dimensional semisimple Lie algebras, Casimir opera­ tors refer generally to elements in the centre of U(g). On representations of g they thus produce operators commuting with the action of g. For a description of the center of U(g) one can consult [Bo4]. The most common of the Casimir operators is the quadratic Casimir operator F == LfT[^xfXi, where { x j , { a : * } are dual bases of g relative to the Killing form. For the infinite-dimensional case Kac reorganized the sum using basis elements from root spaces and “normal ordering” the products so that the vectors from positive root spaces precede (in order of application on modules) those from negative root spaces. This produces an expression which, as we have seen, makes sense as an operator on modules from category

4.6

THE RADICAL THEOREM

In this section, unless mentioned to the contrary, we let A = (^¿y)/ye j ^ symmetrizable matrix and R a realization of A. We denote by u the universal algebra of (A , R) and set g = u/rad(u). All the notation of Sections 4.2 and 4.3 is maintained throughout. We identify h with a subalge­ bra of both u and g and endow both of these algebras with invariant bilinear forms ( *I • ) u and ( • | * )g in such a way that (• ), = (• • )u when restricted to ^ X t We denote this common restriction by (• | • ) and use the same notation for the dual bilinear form

Our intention is to establish an important result due to Gaber and Kac [GK] that states that rad(u) is generated as an ideal by some of its homogeneous components rad(w)“, where the a ’s appearing as generators are character­ ized in terms of the bilinear form (• I • ). In the case where ^ is a Cartan matrix, this leads to a characterization of rad(u) as the ideal generated by the that were defined in Section 4.1. This is called Serre’s theorem when A is of finite type. Lemma 1 Let abe a Lie algebra, and let Vi{a) be its universal enveloping algebra. Define U'^(a) to be the two-sided ideal o f U(a) generated by a viewed as a subspace

Contragredíent Lie Algebras

376

of U(a)

[jo

U(a)

=

K1

©

U'*‘(o)]. Then

(i) U+(a) = U(a)a = aU(a); (ii) a n (U^(a)U+(a)) = [a, a]; (iii) § n SU'^ía) = [§, §] if § is a subalgebra o f a. Proof (i) Both U(a)a and aU (a) are two-sided ideals of U(a) containing a (because 1 and a generate U(a) as an algebra). This clearly implies part i. (ii) Let IT; U(a) -» U (a/[a, a]) be the homomorphism induced from the canonical map a a/[a, a]. Since a/[a, a] is abelian the enveloping alge­ bra U (a/[a, a]) is isomorphic to a symmetric algebra S = (Section 1.8). It is clear that ir(a) c and that -n-(U‘^(a)U‘''(a)) c rr(a n U‘^(a)U^(a)) = 0, and therefore a n U'^(a)U'^(a) belongs to the kernel of the restriction of ir to a; this is [a, a]. The reverse inclusion, namely [a, a] c a n U(a)'^U(a)'^, is clear. (iii) By Corollary 2 of PBW (Section 2.8), we know that U(a) is a free left U(§)-module admitting a basis of the form {1} U { x ¡ ^ , Xj ^ ¡ ^ < ... A: > 0, where (xj + §};ej is some totally ordered basis of the quotient space a / l with Xj e a. Thus (U(§)A:y|... Xj^) n § = (0), and hence § n § U (a )'" c § n § U (§ )‘^. We can now use part (ii) with a replaced by i.



Via the canonical mapping - : u ^ g any g-module may be viewed also as a u-module. In addition, the corresponding associative algebra homomor­ phism - : l l ( u ) ^ U ( g ) allows us to view U(g) as a right U(u)-module, namely q • u ■= gU for all g e U(g), u e U(u). Proposition 2

Identify if with a subalgebra o f both u and g, let A e ^*, and let M(A) and M ix.) be the Verma modules of highest weight X o f n and g respectively. Then

(i) U(g) ®u(u)M(A) is a highest weight q-module of highest weight A. (ii) The natural surjection f : M(X) -* U(g) ®u(u)M(A) is an isomorphism i f is the surjection given by the universal nature of MiX); see Section 2.2). Proof (0 Clear. (ii) We look for an inverse for /. Think of M i X ) as a u-module via . That is, X • V = X ■V for all X © u , y ^ Mi X). We then obtain a u-module surjection - ,

onto

^ .

M i x ) ^ M(A)

377 The Radical Theorem

4.6

given by the universal nature of M(A). This extends to a linear mapping

which is easily seen to be a U(g)-module homomorphism. Consider the multiplication map U(g)<8> M (A )^M (A ) U (u)

given by X

®V ^

X

•V

for all

X

e U( g ), í; e K.

By composing this map with the above, we obtain a U(g) homomorphism (and hence g-module homomorphism) Ar:U(g)®

M(A) ->M(A). U(u)

It is immediate that / and x

inverses of each other.



Let us fix a minimal regular weight p.

Theorem 3 [GK] Let A he a symmetrizable matrix, R a realization of A, and u = \x{A, R) the universal algebra of iA , R), Let rad(u) = r_ 0 r+ be the radical o f u. Then r+ {resp. r_) is generated as an ideal by the elements of {resp. r ““), where (0 a e (2+, (ii) (2p \a) = (a \ a). Proof Let Miff) be the Verma module for u with highest weight 0, and let ¿5+ be a highest weight vector of M(0). Consider the unique maximal proper submodule iV(0) of M(0). Since ejfj • u += a f ' v^= 0

for all j G J,

we see that each /^ • ¿5^ g MO) and that these elements generate MO) as a module. Since highest weight submodules of Verma modules are themselves Verma modules we conclude that the submodule of M(0) generated by f j ' v+ is the Verma module M i —af), Thus M 0 )= L m - a j ) . ;s j

378

Contragredient Líe Algebras

Recall that u_ is freely generated by the f / s (part (i) of Proposition 4.2.4), and hence that U(u_) is the free associative algebra on the f / s (Proposition 1. 10.2). It then follows that for all choices of U j g U(u _), j g J, the family {mJ JJ' f }-ci c U(u_) is linearly independent and hence [from the construction J J ^ of M(0)] that the sum of the M i —af) is direct, ( 1)

iV(0) =

0 M{-aj).

yej

By Proposition 2 we have a g-module isomorphism U(g)®

M(-aj) = M{-aj) U(u)

which together with (1) gives ( 2)

U(g)0

iV(0) s 0 M ( - a ) , U(u)

;e j

where each M i.-a/) is the Verma module of g with highest weight -Uj. Consider the map (p: r_-> U(g) ® given by for all X G r_. We claim that ^ is a u-module map. (Recall that r_ is an ideal of u and hence an u-module under the adjoint action. Similarly g is a u-module by means of the canonical map “ : u g.) Indeed, if m g u and x g r_, we have
1

^ U ' X ' Vj^— 1 ^ X ' U ' V^

= U ® X ' V^—X ^ U '

= u ® X ' V^

(since 3c = 0)

= u(p(x). This calculation also shows that cp annihilates [r_, r_]. Taking into consider­ ation (2) we obtain an induced linear map 0 Af(-a^). /sj Moreover r_/[r_, r_] has a natural g-module structure, and


4.6

The Radical Theorem

379

a g-module homomorphism (this is easy to verify). We claim that


®fjV +

= L “;( l

+

Under the isomorphism (2) we may identify v{.-= 1 ® fjV+ with a highest weight generator of M( - a j ) . Thus from (p{x) = J^Uj-

0 M{-aj)

we see that Hy = 0 for all j ^ J. This last implies that x ^ v_n r_U(u_)'^= [r_,r_] by Lemma 1. This shows that

0 for some i e J. Then L ( - a ) is a proper factor in M i —ai) and by Proposition 4.5.3, ( —a + 2p I —a) = ( —a , + 2p I —a,). However, (2p | a,) = (a, | a,) by (4.4.15) and thus 2(p | a) = (a | a). Let i? = (a e e + I(2p I «) = ( a I a)}. Since r_/[r_, r_] is generated as a Q_-module by its primitive vectors (Proposition 2.6.5), we obtain t _ / [ x _ , x _ ] = £ U ( g _ ) r l “ mod[r_,r_] a^R =

U ( u _ ) n “ mod[r_, r_], a^R

Contragredient Lie Algebras

380

and hence r_/[r_, r_] is generated as a u-module by the elements of rZ“ + [r_, r_], a ^ R. Finally, let §_ be the ideal of u generated by {rZ“ | a e i?}. We want to show that §_= r_. By the above §_+[r_, r_] = r_. Thus [§_ + [ r _ , r _ ] , r _ ] = [ r _ , r _ ] , and hence § _ + [ [ r _ , r _ ] , r _ ] = r_. By induction it follows that (3)

§_+ r " = r_,

where r ” = [ r " “ \ r _ ] . Now the weight spaces -(¡2 ++ *** +j2+X«-times), and hence

of

r"

lie in

n 1:-= (0) n= 0

(also see Proposition 2.7.5). Then (3) implies that §_= r_, as prescribed by the theorem. To establish the result for we use the anti-involution a. □ Corollary Suppose that the entries o f the matrix A are real numbers that are either all positive or all negative. Then \x{A, R) is contragredient and radical free. In particular %(^A,R) = vl{ A, R) and and g_ are free. Proof. Since A¿^ # 0 for all i, the algebra u is contragredient (Proposition 4.2.7). Let S = (5,y) be the structure matrix of u. Then (ibid. Remark 5) 2A,j c = ___jL ^ij A * In particular 5,,. > 0 for £,’s. (If {epyej symmetrizes that the universal covering fore apply Theorem 3 to u. Section 4.4)

all i, ; e J and 5 is synunetrizable with positive A, then symmetrizes 5.) We conclude algebra u of g is synunetrizable. We can there­ If a e A^. and we write a = Ec,a„ we have (see

2 ( p \ a ) = 2XXp,c,e,a,^> = 2X)c,e,-

4.6

The Radical Theorem

381

and ( a | a ) = 2 £ c f 6 ,. + Y,CiCjSjSn /

i

(all of these sums have finite support). Thus 2(p 1a) - (a I a) = 2£(c,. - cf)si - Y^CiCjBjSij < 0.

i

i*i

The theorem then shows that rad(u)+= (0) and hence that u is radical free. Finally, since u is the universal covering of 9, we conclude by Proposi­ tion 4.2.8 that 9 itself is radical free; in fact u = 9. □ Theorem 4 Let (9, be contragredient and suppose that its structure matrix is a symmetrizable Cartan matrix^ A = j. Let R be the natural realization of A in the context o f (9, and let u(A, R) be the corresponding universal algebra. Let J(R) be the ideal o f Proposition 4.2.10. Then (i) J(R) is the radical o f m{A, R)\ (ii) rad(9) is generated as an ideal by the elements dtj = dj: = (ad fj)

Vi

for all

In particular 9^(^, R) = %{A, R). (iii) If 9 is integrable (i.e., if 9 is a Kac-Moody Lie algebra), then 9 is radical free. Proof. If (i) is true then (ii) follows at once by Proposition 4.2.8 and (iii) follows from the fact that 9/rad 9 is radical free (see Exercise 2.18). We have to show that j {r ) = rad(u). Using Proposition 4.1.11(0 we see that J{R) c rad(u). To show the reverse inclusion, we let ¡jl'.vl 9^ •= \x/J{R) be the natural mapping. Then it will suffice to show that 9^ is radical free, for then, using Proposition 4.2.8 again, rad(u) c ker()Lt) = J{R). According to Theorem 3, rad(u) is generated by certain elements x^ where (4)

“ s Q+ and2(p|a) = ( a |a ) .

Let be such a generator and suppose that rad(g^)“. By Proposition 4.1.10, ^^A(g^) =-A(gVrad(g^))

¥= 0. Then

^

382

Contragredient Lie Algebras

and since real root spaces are always one dimensional (Proposition 4.1.5) we see that rad(g^)“ = 0 if a e Thus we may confine our attention to those a for which e (g^)“ and a e ^'"ACg’O. Assuming that our bilinear form on g^ is chosen so as to conform to (IBF) of Section 4.4, we conclude from Proposition 4.4.8 that (a |a ) < 0, and thus by (4) that (p|a) < 0. However the definition of p (see(4.4.15)) together with a ^ gives (p|a) > 0. This contradiction shows that ¡1 kills all the generators of the radical of u and hence the entire radical. □ Remark 1 Is the assumption that A is symmetrizable necessary to obtain the statements of Theorem 4? At the time of writing this remains an outstanding open problem in this subject. 4J

HERM ITIAN CONTRAGREDIENT FORMS

Let (g, be an invariant contragredient Lie algebra carrying a standard nondegenerate symmetric invariant bilinear form (• 1*). Using the anti-in­ volution (T we can construct a new form ( * I*) : 9 X g

IK

by <x I y> = ( a: lo-y). We observe the following properties of < • | • >, which are trivial conse­ quences of the definition and the results in Proposition 4.4.4. Proposition 1 (i) ( • I • > is symmetric and contragredient (see Section 2.8). (ii) g“ _L g^ with respect to ( • | • > unless a = jS. (iii) The pairing < • I • > lg“xg« w nondegenerate for all a. The object of this section is first to prove that if K = IR, g is an invariant Kac-Moody algebra, and (• | • ) is if scaled correctly, then < • | • > is positive definite on g“ X g“ for all a e A \ {0}. We can use this to define a hermitian contragredient form that is positive definite on root spaces when IK = C. Later we will use this form to establish a positive definite hermitian contra­ gredient form on any irreducible highest weight module of g over C. For the time being we assume only the conditions on g announced above. We define an operator similar to the Casimir-Kac operator of Section 4.5: r g_, r(jc) ==

E

E

0
i

jc]]

for all a: g g"“,

where for each a e A+, {e^-^ and are dual bases relative to (• | •). Let p e be a minimal regular weight.

4.7

Hermitían Contragredíent Forms

383

Proposition 2 For a e A^. and x e g““, r(x ) = 2((p | a) —(a | a))x. Proof. Let M ■■=M(0) be the Verma module of highest weight 0 for g, and let denote a highest weight vector of M(0). It suffices to show that for r e g-“, a e A+, T ( a:) • v+= (2(p I a ) - ( a | a ) ) x • From the Casimir-Kac operator K we have (1)

0 = X•

• y+) = r ^ ( x ■v ^ ) + T¡^(x ■y+)

= { - a + 2 p \ - a ) x ■V++ 2 Y,

^ ' ^ +-

peA+

i

Using the fact that for /3 e A+, e f - x - v + = [ e ^ ¿ \ x ] - v + + x - e f - v ^ = i ^ ^ ^ ’ ^^

if^< a, otherwise.

From (1), ( 2 ( p \ a ) - ( a \ a ) ) x • v += 2

‘ ^+

Y 0
E EFi rel="nofollow">».FS>.*ll

-

0
(2 )

i

i

+ E

Z W - A ‘%

'^ 0 < / 3 < a

i

- E

0
i

'

Observe that the set {)8 e A+ | j8 < a} has the symmetry p we may rewrite the terms inside the braces as

E

0
Z [ 4 ‘- A ‘ % i

a - p. Thus

E E«'-(.-»,[«.e,l,

0
i

which then cancel completely by part (iii) of Lemma 4.5.1. Finally using (2), (2( p | a ) - ( a | a ) ) j r • i; + = which proves the proposition.

Y

L

0
i

[4 rel="nofollow"> ^]] ‘ ^ +□

Contragredient Líe Algebras

384

Lemma 3 Let g be an invariant Kac-Moody algebra. Assume that its Cartan matrix is symmetrized by ^ Q+- Assume (• I *) is defined according to the conditions IBF o f Section 4.4. Then 2( p l a ) > ( a l a )

for all a

Proof We use induction ht(a). For a = a, of height 1, 2(p I = (a^ I «¿) > 0. Suppose that ht a = A: > 1. If a then (a | a) < 0 by Proposition 4.4.8, whereas 2(p | a,) > 0 for all i => 2(p | a) > 0. If a then there is a ; e J so that rja = a — ay has height k' < k. Hence 2 (p | a ) > 2 (p | a - ay) = 2(p 1rjo) > [r^a I rjo) = ( a I a ) .



Proposition 4 [KP2] Let g be an invariant Kac-Moody algebra over U and assume the hypotheses of Lemma 3. Then < • I * ) w positive definite on all nonzero root spaces of g. Proof Because of a it suffices to show this for root spaces g““, a e A+. For -a ^ we have (f i

I//> = (e,-1fi) = ef' > 0

(see Proposition 4.4.4 and IBF4 in Section 4.4). Suppose that ht a = A: > 1 and the result is proved for g“^ with 0 < ht )3 < ht a. For each jS e A+ with ht )3 < ht a, let {e^!}^} be a self-dual basis (relative to < • | • >) for g"^. Then for [e% \ e^p) = {e% \ e^l\) = 5,^, which shows that and {ep) are dual with respect to (• 1• ). For any X e g~“ \ {0),

(2(p|o;) - (o:|a)) =

D 0
=

E 0
0
L ( [ « - W [^i8^ •']] I i

E([«p^^] i i

by the induction hypothesis. Thus <jc | x rel="nofollow"> > 0.



385

Exercises

Remark 1 Proposition 4 remains true if the given field 1 : is replaced by any ordered field. □ Let be a Kac-Moody algebra over IR defined by A , and let < • 1• > be the corresponding symmetric contragredient form on qJ . A \ which is positive definite on nonzero root spaces. Let g(y4) := C 0 Then q( A ) is a complex Kac-Moody Lie algebra and we can extend < • 1• > to be a hermitian form on g (^ ) uniquely (depending on which variable is to be antilinear), and it is positive definite on nonzero root spaces. Summarizing we have Proposition 5 Any invariant Kac-Moody Lie algebra g over C carries a hermitian contragre­ dient form < • I • ) that is positive definite on nonzero root spaces. The form {• \ - ) is unique up to positive scalar factors on each o f the indecomposable factors o/ Dg (see Proposition 4.3.8). Remark 2 Propositions 4 and 5 can be extended to include other radicalfree contragredient Lie algebras carrying nondegenerate symmetric invariant bilinear forms. The only requirement is the condition (PC)

2(p I a ) > ( a 1a:) for all a G A+ and

> 0 for all i e J.

EXERCISES 4.1 Let ^ be an / X / Cartan matrix of finite type. (a) Show that A has an /-dimensional realization R = (i\,U ,U ^).

(b)

(c)

(d) (e) (f)

Let g = q(A, R). This Lie algebra is up to isomorphism indepen­ dent of the choice of R in (a). Show that g is a semisimple Lie algebra and that g is simple if and only if A is indecomposable. (In this case g is called the simple Lie algebra of type A over K.) Let (• I • ) be standard symmetric invariant bilinear forms on g is positive definite when and i)*. Show that (• I * ): X restricted to Q q X (rational span of the roots). Show that A U {0} (Proposition 4.4.8) and that '^^A c 1^* is a finite root system with Cartan matrix A and base II. Show that dim^^ g = / + T^A| < oo. Compute dim g for all indecomposable Cartan matrix of finite type.

Remark For algebraically closed fields IK the only finite-dimensional sim­ ple Lie algebra are the Lie algebras g(-^4) when A is of type Ai, Bi, Ci, D^, ^4’ ^rid G2.

Contragredient Líe Algebras

386

4.2 For each of the finite type Cartan matrices A of rank 2 construct a two-dimensional realization R of A and explicitly compute a basis for g(A,R). 4.3 Let A be a Cartan matrix of type A¿, and let R be an /-dimensional realization of A. Prove that g = (A, R) - §!(/ H- 1, K). 4.4 Let K be a 2/ + 1-dimensional IK-space, / > L Fix a basis {ljq, Ü2i} of V. Let be the (nondegenerate sym­ metric) bilinear form on V whose matrix with respect to the above basis is ' -2 0 0

10 1 11 1I

!0 ) 1 111 I 1 1

21 / -identity matrix. Let V' •= © and let be ¿=1 the restriction of j8 to V'. (a) Show that g()8) (see Exercise 1.1) consists of all matrix of the form

where / is the /

X

0

1^ 1 2b^ 1 1 1c

1 b \ 1 11 B 1 -A^j

where A is an arbitrary / X / matrix, B and C are arbitrary skew symmetric / x / matrices, and a and b are arbitrary 1 X / matri­ ces. Conclude that g(j8) has dimension 21(1 + 1) and that g()3') is a subalgebra of g()8) of dimension 2/(/ - 1). (b) Let a

E , - E,/+/,/+/> 1 < / < /.

Show that ]^ := 0 is an abelian subalgebra of g()8'). ¿=1 (c) Let be the basis of b* dual to , c b- For 1 :< i < j < I define “

E qj +¿

^ ~'^E i +¿ q — E qj ^ ^ij ~ E^i+jj+i “ ~^j,i ~ ^ l +i,l+j = ^¿J+j ~ ^ j j +i

Exercises

387

Let A == [±2s¡, ± £, ± Sj\\. < i < / < /} and A' != {±£,- + £y|l < i < / < / } . Show that 9(jß) =

e 0 K X^ and a e A

9(j8') = ^ ® 0 aeA' (d) Show that [h, X^] = a(h)X^ for all h and a e A. Conclude that g()8) is a Lie algebra of type Bi and that g()3') is of type D^. 4.5 Let F be a 2/-dimensional IK-space; / > 1. Consider the matrix / =

0

I,

-I,

0

where /, is the identity / x / matrix. Let ¡3 be the bilinear form on V defined by /3: P{v, w) = v^Jw. (a) Show that /3 is alternating and nondegenerate. (b) Let g(/3) be the Lie algebra defined by /3 (see Exercise 1.1). Show that g(j8) consists of all x =

- a^ '

^

square

/ X / matrices such that B = and C = C^. Conclude that dim|^ g(/3) = /(2/ + 1). (c) Let 1 :< I, j < 21, be the matrix with 1 in the i, j position and 0 elsewhere. Let ay = Ea - E,+ij^i,

1 < / ^ /.

Set = E|.=iKa,^= ©/^jlKa/. Show that is an abelian subal­ gebra of g(/3). (d) Let {£,}j s / sz c: ]^* be the basis dual to {an<=i,z ^ For 1 < / < j < I define ^2ci ~ ^i,l+i’ ^ - 2 ., = 7+/,/’ AT. = F. ,• - E, ^

— e¡ + ej

+ ~ ^ij+j

^ l + i, l + j ^

^j,l +i’

Show that each of these 2/^-matrices belongs to g(jß).

Contragredient Lie Algebras

388

(e)

(f)

Let A = {2s,, ± e, ± 11 < / < ; < /} c 1^*. Show that g(j8) = ij 0 [h, x j \ = a(h)X^ for all a ^ A and h Let A be the Cartan matrix of type Q , and let q(A, R) be the Lie algebra defined by some /-dimensional realization of A. Prove that q(A, R) = g()8).

4.6 Let ^ be a Cartan matrix and R a minimal realization of A. Show that q( A , R ) is finite dimensional if and only if A is of finite type. In particular all finite-dimensional Kac-Moody algebras are invariant. 4.7 Let (g, be a finite dimensional Kac-Moody Lie algebra, and let (• I • ) be a minimally realized positive definite invariant bilinear form on g (see Exercises 4.6 and 4.1). Let M e ^ (g , <^) be a highest weight module (a) If jjL is such that [ M : L(/i)] > 0 show that (filfi) -

(b)

2 ( A

+

p Im )

= 0 .

(Use Proposition 4.5.3). Conclude that M has a finite composition series.

4.8 Let g be a minimally realized finite-dimensional Kac-Moody Lie algebra. (a) Show that p = is the unique minimal regular weight. (b) Show that g is a semisimple Lie algebra and that g is simple if and only if A is indecomposable. 4.9 Let ^ be a symmetrizable Cartan Matrix, i? = ( l ^ , n , n ^ ) a realiza­ tion, and '^^A the corresponding set of real roots of g (^ , R), Prove that for all a e'^^A, a^ = 2a^/{a^ \ a^) = 2a^/{a \ a) (see Proposition 4.1.6 and Section 4.4). 4.10 Let A ht 2i Cartan matrix, R a realization. Prove that Dg(y4,/?) is centrally closed. [Take a universal central covering algebra of D g(^, R\ and lift back a set of generators. Show that these can be adjusted to satisfy the relations (Rl) and (R2) of the original set of generators of D g(^, R\] 4.11 In this exercise we obtain an explicit realization of the Lie algebras g(^,i^), where A is an affine Cartan matrix of type A^P, Cf-\ D p , E p , EP, EP, FP, or o p and R is a minimal realization of A. Let Ah&di Cartan matrix of type A^, C^, D^, E^, E^, Eg, F^, or G2, and let A be the corresponding finite root system with base n = {«1, . . . , a/}. Let (f> = L\=ln¿a¿ be the highest root of A, and let A be the affine Cartan matrix constructed from (f> in Lemma 3.5.3. Let g = g(v4, R) be the simple Lie algebra of type A based on some minimal realization R = (1^, II, 11^) of ^ over the field IK.

389

Excercises

Let (• 1• ) denote standard invariant bilinear forms on g and also on 1^*, and assume that it is so scaled that ( a \ a ) = 2 for long roots. Finally, let lK[i-^] denote the ring of Laurent polynomials 1 e K, = 0 for all but finitely many i e Z}. (a) Let § — IK[i-^] 0|)^g 0 Cc be a one-dimensional vector space extension of the Lie algebra IK[t -^] (over K). Define a new bracket [ •, • ] ~ on § by bilinear extension of (i) [ g , c ] ~ = o (ii) w ® X , <8> y]~ = ® [x, y] + q( x I y)c for all i, j e Z, X, y e g. Prove that (§,[•, • ]~) together with the mapping h± 1] ® 9,

TT: g (S>X

(b)

a0

<S>X,

is a central covering of lK[r ® g (see Section 1.9). Let res: IK[i-^] -> K be defined by res(E«y t^) = a Prove that [ f ® x , g ®y ] ~ = fg ® [ x , y ] + r e s |g ^ j ( j : I y)c for all / , g e IK[i*^],A;,y e g.

Henceforth we will simply write [•, • ] instead of . (c) Let {e^, '', f^} be an §l2-triplet with e g’*’, e g“ '*’ (Pro­ position 4.1.6). Prove that = 2°/(° \ <j>°) = 'L'l^iftyay, where n / = n,(a,-1 a,)/2 . (d) Let e„ /i,, /„ i = 1,.. ., / be the standard set of generators of Dg, and identify them with the elements 1 ® 1 ® /i„ 1 ® /, of g. Define Cq == 1 ® /^ ,

/o == 1 ®

/iq ~ C ~ 4>'^■

Prove that {cq, / io,/o) is an §l2-triplet of g, and prove that {e„ hi, /, 11 = 0 , . . . , /} satisfy the relations (Rl) and (R2) of Proposition 4.3.3 for the affine Cartan matrix A. (e) Let §* := ^ © Kc © Kd, and set fl'^== {a^, a ^ , . . . , a/ } c ^ -lKft with {«i'',. . . , a /} c i) from the realization R and uq — ¡t Define n = {ao, « i , . . . , a,} c (§*)* by

:= 5,0-

390

Contragredient Lie Algebras

(f)

Prove that R •= n , n ^ ) is a minimal realization of A and that R is naturally embedded in R. Let § := q(A, R), Show that there is a natural surjective homo­ morphism :Dg ^ D§.

(g) Using Proposition 4.3.9, show that


(i)

if A: ^ 0, if A: = 0.

Show that = A + Z5. Show that the reflections act on A as follows: r^8 = 8

for all / = 0, . . . , /,

r^(a + k8) = r^a fQ(^oi + Ac5) =

(j)

+ 2

k8 + (Ac +

/ = 1, . . . , /, for all oc ^ A, k ^ Z,

where (f) is the highest root of A. Prove that § is centrally closed and that hence § is the universal covering algebra of

4.12 Let R = be a minimal realization of the Cartan matrix A = Let n = . . . , CD;} c ]^* satisfy (a)¿, a /> = S^j, 1 < i, j < I, where II^= {a]^,. . . , a/}. Let P = Cl Q, Prove that P, and also P+-= {fi ^ P\ ( , cr^^> e N for all / = 1,..., /}, span 1^*. jjl

4.13 In this exercise we consider a generalization of contragradient Lie algebras that allows one to treat the following very natural question: Let g be a contragredient Lie algebra, and let f c g be a subalgebra such that I ^ the diagonal subalgebra of g) and cr(i) = f, where a is the anti-involution of g. What sort of Lie algebra is I? It is, up to a central factor, one of these generalized contragredient algebras. This type of generalization was first introduced by R. Borcherds (Gener­ alized Kac-Moody algebras, /. ^4/g. 115 (1988): 501-512) in order to answer such questions. He assumed invariance and positive definite­ ness (as in Section 4.7). The presentation in this exercise follows our presentation in Section 4.4 and does not assume invariance. The exercise involves reworking most of Section 4.4, taking note of how to cope with the extra generality. At the end we return to the motivating subalgebra problem. It is noteworthy that even if the original contra­ gredient Lie algebra g is finitely generated, f need not be, and hence the potential that the index set J is infinite is very real.

Exercises

391

Let g be a Lie algebra over a field K. We say that g is generalized contragredient triangular or simply generalized contragredient if there exists a triangular decomposition (g+, 1^, Q+, a) of g satisfying the following conditions: GCTl If ej c is the given basis of 0 + according to the axioms of triangular decomposition, then the Lie algebra g^-*^ generated by g“> and g““j is three-dimensional for all j e J. GCT2 The elements of g“^ g”“', j e J, and generate g (as a Lie algebra). GCT3 The sum Eye 9“^] is ^ direct sum. (a)

Show that dim,^ g“^ = dim^^ g~“^ = dim J g " “^ g““^] = 1. If a / is a basis of [g“j, g““^], show that two cases are possible: Case H: [a^^, g“'] = (0) in which case we say that j e Jyy, Case S: [ a /, g“'] = g“' in which case we say that j e J^. Write J = Jyy U J5. Show that ; e Jyy <=> g<^> is a three-dimensional Heinsenberg algebra and / e <=> g^-'^ s §I2(IK). Conclude that (g, 5^) is contragredient iff Jyy = 0 . (b) A display of (g, is a set ~ (ej, a j , /y)ye j such that Dl: g(^> = IK/y ® K a / e Key, D2: [ey,/y] = a / , [a/,ey] = 2cy, [ a / , / y ] = - 2 / y whenever j e J5. D3:
a^=kjar,

fj = t^fj,

with kj = 1 fy = +1, whenever j e J^. (c) Define the structure matrix A = A ( 3 ) of display 3 = {ey, a / , /yly^ j of J by Aij

relative to a

^(x^yOij ),

Show that Ajj = 2 if ; e J5 and Ajj = 0 if ; e Jyy. Describe how A changes if 3 is changed. (d) Generalize all the theory developed in Proposition 4.1.1 to Proposition 4.1.7 to generalized contragredient Lie algebras (Let " J : = { ; ■ e J5 I ad Cj is locally nilpotent}. We say a e A is real if a = w u j for some w ^ W and j e " J .

Contragredient Lie Algebras

392

(e)

Let A be the structure matrix of (g, relative to a display. Fix j ^ Js- Show that the following hold. (i) j iff e Z <0 for all i e J, j # ; . (ii) If j g " J and i ¥=j, then == (adcy) = 0. (iii) If j then for all i e J, Aij = 0 « [ e , , c j = 0, A,j = 0

(f)

Let (g, be a generalized contragredient Lie algebra, and let g = g/t, where t is a o--invariant ideal of g contained in rad(g). Then the natural mapping ~ : g ^ g is injective on the subspace ^® Identifying 5 and 1^, we have that *^=_(^5S+,G+,cr) is a triangular decomposition of g and that (g, is a generalized contragredient. l^ rth erm ^e every display 3 of (g, induces a natural d isp l^ 3 of (g, and relative to 3 and 3 both (g, and (g, 3~) have the same structure matrix. Finally, "^A(g) c^"A(g)

(g)

■Aj, = 0.

and

IF(g)cIF(g).

Let (g, be generalized contragredient with structure matrix A = Define g — g/rad(g), and let " : g g be the canonical map. Then for j e (i) If A¿J e Z_ or if A¿J = Aj^ = 0 for some i ¥=;, then d^j — (ad and d~j -= ( a d b e l o n g to rad(g). (ii) For ad 6j (and hence ad fj) to be locally nilpotent, it is necessary and sufficient that A^j ^ Z < q that A^j = 0 => Aj^ = 0 for all i ^ j\ (h) Let (g, <5^) be generalized contragredient. If 3 and 3 ' are displays of ( q, 3~) and A and A' are their respective structure matrices, show that A is symmetrizable iff A' is. Follow Proposi­ tions 4.4.1 and 4.4.4. Define the concept of invariant generalized contragredient Lie algebra. Show that the proper form (• | •) on g can be chosen to satisfy IBFl, IBF2, IBF3, and IBF4 (a¿ I ay) = A^jSj for all i, j e J, and a^ = 2aJ/(aj \ ay) if j ^ J5. IBF5 (a,^ I a / ) = A^jS~^ for all i, ; e J and a,. = 2 ( a / ) V ( < I < ) if j ^ h A form satisfying IBF1-IBF5 is called standard. (k) An ordered generalized contragredient Lie algebra is a triple (g, 3 ) consisting of a generalized contragredient pair (g, 3^) and a display 3 relative to which the structure matrix A of

393

Exercises

(9, ORD

satisfies all entries of A lie in an ordered subfield F of IK and for all ; e J the set Rj -.= has the following properties: If j e Jff, either Rj c Fg.o or Rj c F
e J j, either R j

Define J * by y e

(z

í

^

q

Ot R

j

c

Z

Rj c F ^ q>

J \ J"^ so that

/ = J -U J+. If (g, 3 ) is radical free and A has the property that A¡j = 0 <=>Aj¡ = 0, then show that ^7 = J + n J5, '■'”/= = J \ " J = J -U ( j + n j „ ) . (Use part (g) above.) (1) Let (g, y , 3 ) be an invariant ordered generalized contragredient Lie algebra, and let A be its structure matrix relative to the display 3 . Show that the family isj)j^j syimnetrizing A can be chosen so that IBF6

> 0 1Cy < 0

if j e J"^, if j e J “ .

(m) Let (g, y .^ ) be as in (1). Show that g carries a standard invariant form satisfying the following: (i) The restriction of (• I•) to (2 ^ 2 is F-valued. (ii) (a, I tty) 0 if i, j e J, I 9«=j. (iii) ( t t y I a y ) > 0 if y e''*J. [Choose a form as in (1). First consider the case rad(g) = (0), and use (k). For the general case use (f).] Let p e 1^* be such that = l

if y e Js,

= 0

if y ^ J/Í-

(iv) If J'^ n Jo ='^*J show that

394

Contragredient Lie Algebras

(0 (ay I ay) < 0 for all j

Conclude that (a | a) < 0 for all a e

(ii) 2(p Ia) —(a Ia) e F^o for all a e A+. Moreover 2(p | a) = (a I a) if and only if either a = ay for some ; ^ J or a = + • • • +Cy^ay^, where /: > 2, {j\ \l < i < k ) and ^y = j =0 for all 1 < p < ^ (n) Define and recover the results about Casimir-Kac operators for radical-free invariant generalized Kac-Moody Lie algebras. (o) Let (g, D) be an invariant ordered generalized contragredient Lie algebra, and let A be its structure matrix. Show that the radical of g is generated (as an ideal of g) by the elements

dr:=

(a d /y )

+1

( J^

A , J = A . = 0.

Show that u modulo the above relations satisfies J^, and use the Gaber-Kac Theorem). (p) Let (g, «5^) be a contragredient Lie algebra. Let i be a subalgebra of g satisfying 5 c f and o-(f) = i. (a) Prove that there exists a generalized contragredient algebra together with a surjective homomorphism tt : ^ i, such that ker(7r) c centre ( ^ ) c and ^ is invariant if g is. (Order the positive roots of g+ in a way respecting height. Choose generators of f in a-symmetric pairs by ascending height. Note: The number of generators will in general be infinite even if g is finitely generated.) (b) Prove that if (K = [Rand g is invariant, then ^ can be chosen with ^ = f .

Chapter Five

The Weyl Group and Its Geometry A

m a n t r a v e l i n g a c r o s s a f i e l d e n c o u n t e r e d a t ig e r . H e f l e d , t h e t ig e r a f t e r h im .

C o m in g to a p r e c ip ic e , h e c a u g h t h o ld o f a v in e a n d s w u n g h im s e l f d o w n o v e r th e e d g e . T h e t ig e r s n i f f e d a t h i m f r o m

above.

T r e m b lin g , th e m a n lo o k e d d o w n to

w h e r e , f a r b e lo w , a n o t h e r t ig e r w a s w a i t i n g t o e a t h im . O n l y t h e v i n e s u s t a i n e d h im . T w o m i c e , o n e w h it e a n d o n e b l a c k , lit t le b y lit t le s t a r t e d t o g n a w a w a y a t t h e v in e . T h e m a n s a w a l u s c i o u s s t r a w b e r r y n e a r h im . G r a s p i n g t h e v i n e w it h o n e h a n d , h e p l u c k e d t h e s t r a w b e r r y w it h t h e o t h e r . H o w s w e e t i t t a s t e d !

—A Buddhist parable—from York: Vintage Books, 1960)

T h e W o r ld o f Z e n ,

Nancy Wilson Ross (New

The Weyl group W of a contragredient Lie algebra (g, was introduced in Section 4.1. As we saw, it is possible to gain valuable information about g by means of W. For example, the automorphisms of g of the form n^(t), a permute the root spaces g^ according to the rule n^(t ): g^ ^ where r^ ^ W is the reflection in a defined in Section 4.1. We used this to conclude that if a is real, then g“ is one-dimensional. Evidently we can think of W in relation to automorphisms of g, and we can also think of PL as a purely geometrical object that permutes the set Ac Information obtained by looking at PL as a group of permutations of A can be used to understand g, and vice versa. These considerations are quite vital for our later work on g and its representations. However, abstract root systems are quite important in areas of mathematics outside Lie theory, and we have consequently tried to make this chapter somewhat self-con­ tained. Thus our approach to PL is axiomatic and, on the whole, free from the Lie algebra context. In fact we do need a little Lie algebra theory to establish one of the basic facts about root systems right at the beginning (Proposition 5.1.4) and again in the section on imaginary roots.

395

The Weyl Group and Its Geometry

396

This chapter then is devoted to a detailed study of Weyl groups and abstract root systems. The framework in which we work is a structure called a set of root data. One of the main problems in dealing with infinite root systems is that although they may have finite bases in the sense of finite root systems, their subroot systems may only have infinite bases. Thus from the very outset one needs to consider infinite bases. On the other hand, to prove that subroot systems even have bases and then that bases of root systems are conjugate, it seems necessary to create a chamber geometry similar to the well known finite theory (see [Bo3]). Our definition of root data is designed to encompass all root systems and subroot systems of Kac-Moody Lie algebras, to allow construction of a chamber geometry, and to work over arbitrary fields of characteristic zero. It is based on earlier work of J. Tits, E. Looijenga, and Moody-Yokonuma. The presentation follows [MoPi2] quite closely. After establishing the notion of root data in Section 5.1, we have three sections dealing with basic facts on the Weyl group and its action on root systems, including the length function, the relationship with Coxeter groups, and the Bruhat ordering. The central section of the chapter is Section 5.6 on the chamber geometry of a set of root data. This is followed by a section on subroot data in which we prove the important fact that any subroot system of a set of roots may indeed be viewed as a set of root data in its own right. Section 5.8 is on imaginary roots. This contains the Kac characterization of imaginary roots and shows how the three basic types of root systems, finite, affine, and indefinite, are distinguished by their imaginary roots. The final section shows that any two bases of an indecomposable set of root data are conjugate up to an overall sign by the Weyl group. This shows immediately that the Cartan matrix is an invariant of the root system and is an important first step in proving that it is also an invariant of any invariant Kac-Moody Lie algebra (Chapter 7). 5.1 ROOT DATA Let K be a field of characteristic 0. By a set of root data over IK we understand a 6-tuple consisting of RDl: a Cartan matrix A = where J is an index set (see Proposition 4.1.9); RD2: a pair of vector spaces V and V ^ over IKtogether with a nondegen­ erate pairing ( • , • } : V X V IK; RD3: subsets II = {a,},ei ^ ^md 11'^= c such that (a,, a / > =Aij for all i , j e J.

5.1

397

Root Data

Furthermore we require that RD4: Q := and are free abelian groups admit­ ting bases of the form {%}, ^ Q and ^ i2 where the and the are linearly independent over IK and satisfy H e ® Kly. and ¿el

n^c © ¿el

The last of these axioms is familiar from the axioms of triangular decomposi­ tions. Note that the sets II and II ^ of RD3 need be neither finite nor linearly independent. The standard examples of root data are formed from Cartan matrices A and realizations R = (1^, II, II of ^ over K by setting V •= ij*, F^-= and < - , - > : ] ^ * X] ^ ^ [ K the natural pairing. We call ^ = (A, n , n • » the standard root data constructed from R, We define groups W c GL(K) and IT GL(K in the usual fashion: For each ; e J define Vj e GL(F) and r / e GL(K by r- : a ^ a — ( a ,

for all a ^ V,

rj^ : h ^ h - (aj, h)a^^ It is clear that rj and Section 3.2). Let

for all /i e F

are reflections in

IT:=

and

and

IT

and

2 ^:=IT^n^,

, respectively (see

< r / | ; e J>.

As usual we also define 2 := i r n

which are called the set of roots (resp. coroots) of 2). We also call 2) a set of root data for 2. Actually the set 2 corresponds to the real roots in the case of Kac-Moody Lie algebras, but since there are no other roots to be considered for quite some time, it is more convenient to simply call them the roots. One observes that the definition of root data invites one to consider the dual set of root data in which the roles of 2 and 2 ^ are reversed:

where < • , •

: F ''X F ^ IK is defined by

398

The Weyl Group and Its Geometry

Note that a ^ ) = 2 for all j e J. Thus aj 0 and 0, and hence 0 2 and 0 ^ 2 ^. Before establishing our first result we lay down a list of familiar looking objects 2

+ == 2 n X)

/e j X_:= - X + Q = L

;e j

and

X:f== - X ^ ,

Z«;, Gk == Z “ ;e j

e^== E z a / , ;ej

G ,r= = E K a/. ;ej

Let D be a set of root data, as above, with Cartan matrix A and root system 2. To begin understanding the nature of 2, let us consider a minimal realization R = (ij, B, B ^ ) of A, To avoid confusion with the objects of our root data, we change our standard notation for realizations and write B=

j} c r

and

B ''= { p / \ j

(Zfi.

Then, if < • , • > denotes the natural pairing of and 1^, we see that (A, B, • » is a set of root data. Axiom RD4 is satisfied with % := Pi and py^ for all i e J. Note that 2 (resp. 2 is the set of real roots of the Lie algebra q(A, R) (resp. %{A^, R ^)). Let # = = c G L ( r )

and

G -

©

be the Weyl group and root lattice of R. As usual let := B®. Proposition 1

Let Wq and Wq be the groups of automorphisms of Q and Q obtained from W and W by restriction to Q and Q respectively. Then (i) there exists a unique group epimorphism r : Wq r : r,

for all j ^ J;

Wq satisfying

5.1

Root Data

399

(ii) if ф: Q Q is the unique T-linear map satisfying = ay for all j G J, then for all w g Wq we have the commutative diagram Q W

i

Q

Q

iT(iv) Q

(iii) ./-rA) = X; (iv) ker i/f c {)8 G 0 I<j8, = 0 for all j g J}. In particular, if i is finite arulA is nonsingular, then iff is an isomorphism. Remark I We will see below that the above restrictions to Q and Q are actually faithful. We will also see later that W and W are isomorphic. Proof, (i)-(ii) If T exists, it is clearly unique. Let i, j g J. Then •■pj ■/3, ^

- (Pi,

= Pi - A^jpj,

while 0■ This shows that for all (1)

^ “ i “ AijOj. e J,

■■■r p j i = E c,.y^y ^ ry, • • • ry a,. = E c,7« r ysj

(The reverse implication is not immediate because the c,y on the right-hand side may not be unique.) From (1) it is easy to conclude that t exists and that the diagram of part (ii) commutes. (iii) We have 2

=

= Wil,{B) = i!)WB = ipCA).

(iv) Let j8 G g be such that i/f(/3) = 0. If ; g J, we have 0 = rji[,(l3) = H^p^P) = ^{p - (B ,p p p j) = -(P,B/}aj. Thus (p, p y ) = 0. Finally, if J is finite and A is nonsingular, then since R is

The Weyl Group and Its Geometry

400

minimal, we have 1^* =

and

shows that

In view of this result we call ® == (A, B, B 1^, 1^*, < • , • » a covering of 5), in fact the universal covering of S). The term universal is justified in Section 5.5 where we discuss morphisms. Lemma 2 There exists a unique group isomorphism * :W satisfying r f = ry. Moreover, if we identify W and W ^ via this isomorphism, then ( a , h ) = {wa, wh)

Proof If a e F and h

for all a ^ V , h ^ V ^ , w ^ W,

then for all j g J, (rja,h) = { a ~ { a ,a y ) a j,f^

= { a , h -{aj,h)aj^) = (a,r/h). We claim that for all j \ , . . . , j^, i^, ...Jrn ^ J, we have r, • • * r,Jn = r, *• • r

<=» r,-}\V • • • r,JnV = r, V • • • r:

Indeed, by the nondegeneracy of < • , • > , we have r,Jl • • • r,Jn = r,M • • • r, <=> r,Jn • • • r,J\ = r,

• • • rM

«
••• r , l h ) = Q for all a e F, /i e F

«=> rJ\^ • • • rJm y =

M

• • • r^^. ^n

It follows that there exists a well-defined map * :JV ^ W'^ given by (r.

V ;i

■■■ r ) * = r ^ Jn^

Jl

•••

Jn

.

It is dear that * is unique and that it is a group homomorphism. Similarly we

5.1

can find a homomorphism * : PF ^

Root Data

401

JV satisfying

(o r ■ ■ ■ o r ) * - o , ' " o . Thus W =

via *. The rest of the lemma is clear.



Henceforth we identify IV and PF ^ by the isomorphism of Lemma 2. Thus, for example, we write X ^= {W a/ | j e J}. Proposition 3 (Weak intersection property) Let the notation be as above. Then

WIP:

Zai n Yh ^ >0^; ^ (0) j^i Z a ^ n i ; Z ^ o < = ( 0) j^i

for all i e J, for a l l / e j .

Remark 2 These conditions are a weak form of linear independence on the elements of 11 and II ^ and are necessary to proceed further. Their proof requires RD4. Proof. Suppose that -nf^a^ = 'Lj^^njCtp where nj > 0 for all j ^ k. If nj^ < 0, then we obtain a contradiction by computing < • , > on both sides. If > 0, then 'Lj-rijaj = 0, where each nj > 0 and not all of these are zero. But by RD4 we can write aj = where the c¿j > 0. Combining these gives a contradiction to the independence of the {yj}. The case of H ^ is similar. □ Proposition 4 (Wonderful union property) Let the notation be as above. Then WUP:

2 =

and

where the unions are disjoint. Proof. Using the notation of Proposition 1 and recalling that (see Section 4.2), we have X =

U i ^C®A_) c X + U X _ .

402

The Weyl Group and Its Geometry

Now WIP shows that (2)

if ^ /e j

= 0 where all

e Z t h e n every

= 0.

Hence, if where < 0 and > 0 for all i, then by moving everything to the right-hand side and using (2), we find that = 0 for all i. This proves disjointness. □ Example 1 (Maxwell’s demon [Mx])t Let / 2 - 2 A = \-2 2 I

0

0^ -2

-2

2

Let V = R^o ® R«! 0 R o:2 be a three-dimensional real space, V* its dual, and < • , • > : K X V* R the natural pairing. Let II = {ao> “ 2) ^ and define II {uq , a^, a^] c V* by defined in the usual fashion and identi­ fying IF ^ with IF, let /3a = ('•2''i)* “ o and Claim 1

Pk = (.r2r y a ^ .

= «0 + 2k^a^ + 2(/c^ + k )a 2 and <

+ 2*V+

+ ic)a^

forall k e Z.

To establish this, reason by induction on k. Claim 2 For all p, q ^ Z, p ¥=q, we have < 0,

< /3 „ ^ ;> = 2. Indeed ( Pp, Pg) = ( ( ' - 2''l)'’« 0.('-2''l) ‘'«o') = ( « 0»(''2''l ) * < ) = ^ oiQ, (Xq + 2k^0LY + 2(^k^ + k)oL2^ = 2 - Ak^, ^This is another Maxwell and another demon.

5.1

403

Root Data

We return to our main construction. Let

2 -2 -1 4 -3 4

-2 2 -2 -1 4

-1 4 -2 2 -2

-3 4 -1 4 -2 2

Thus defined, B is a generalized Cartan matrix (infinite, of rank 3). Let

and define fl := Wr^T and

n ^ := W^T

where W^:= The set that

CZW,

is an example of a subroot system of X (see Section 5.7). We claim

is a set of root data with root system ft and Weyl group Wr^. RD1-RD3 are obvious. For RD4 we may simply take To = « 0. T i = 2tti,

T o" =< > The reader may verify that

T l" = 2 a l^

72 = 4«2,

72'^=4a2'^. ®

®

that

The interesting lesson in this example is that it demonstrates that even if we begin with root data based on a 3 X 3 Cartan matrix, we may find inside the corresponding root system sets of roots that are based on infinite Cartan matrices. It might occur to the reader that ft has some finite subset H, unknown to us, that could be used to replace the infinite set T in the sense

404

The Weyl Group and Its Geometry

that

where C is defined analogously to B using H. But this is not the case. We will prove in Section 5.8 that B is an invariant of its system of roots. This example shows why it is necessary to allow the index set J to be infinite in order to be able to discuss subroot systems. Proposition 5

Let if/ :Q Q be as in Proposition 1. The restriction o f i/f to is a bijection onto (resp. 2 _). Proof Suppose that Then

= il/(w2pj) for some

lll{w2

^ ^

{resp. ^^A_)

i ,j s J.

= l/rOy) = aj.

Now Lc*/3*, k^J where the

have all the same sign. Then OLj

^

A:ej

violates WIP unless = 1 and = 0 for all k ¥=j. Thus = Pp this shows that i/f is an injection. The proposition now follows from c S + and WUP. □ Let q: e S. Then by the last proposition there exists a unique p = Lj^jCjpj e'^^A such that ij/ip) = a. We have

« = E yej which we call the natural expression for a in terms of the {ay}. The quantity EyejCy is called the height of a and is denoted by ht(a): ht(a) == yej

5.1

Root Data

405

The next five results have already been established for root systems of Lie algebras. Here they are proved in a Lie algebra free context. Proposition 6 Let q: e S, and let j e J. (i) Qa n 2 = {+ «}. ( ii)

r / 2 A { « ;} ) = 2 A (« y }.

Similar results hold if we substitute 2 ^ for 2. Proof (i) It suffices to show part (i) when a = for some i e J. Suppose that e 2 for some p, q in Z. There exist integers Cj, j e J, all of the same sign such that 1/7 \ ‘1

/

Cross-multiplying by q and applying WIP, we see that c¿ = p /q Ei Z, Now, if na^ G 2 for some n e Z, then na^ = waj for some w and j e J. Then w = (1 /n)aj e 2 , and we can reason, as above, to conclude that n = ± 1. (ii) Let a e X+\{aj}. Because of part (i) we have a = where all Ci > 0 and Cl 0 for some / # j. Now r^a = a + kaj for some A: e Z. Thus r ja

(cj + k ) a j +

=

Y ^ C iO C i.

i*j

Because of WIP we see that TjU # Uj, so it will suffice to show that rjOL ^ X+. Suppose not. Then by WUP, {Cj + k)aj + L c,a,. = £ d,a,, i* j

/ €J

where d¡ < 0 for all i. Thus [d j -

{Cj

+ k ) ) a j = £ (c, - d,)a,. i^j

By WIP we have (3)

E (c, - d ,)a, = 0. i* J

But Cl — d i > 0, and (3) then contradicts (2). This shows that ry(2+\{ay}) c (X^\{aj)). Since r? = 1, equality follows. □

406

The Weyl Group and Its Geometry

Lemma 7 Let i, j e J, and suppose that w ^ W is such that

= aj. Then

(i) wr¿w~^ is a reflection o f both V and in af, (ii) wriW~^ = rj on {in Proposition 10 we prove that wr^w“ ^ = ry). Proof Let p Ei V. Then wr^w~^l3 =

— (w~^P, ay) ai )

= /3 -

(w~^p,a^}aj.

This shows that wr¡w~^ maps «y into —«y and pointwise fixes both the hyperplane {wy | y e F and = 0} of This establishes part (i). Next we write © = rywr^vv *. Then 0/3 = /3 + (<w

(4)

- )ay.

We conclude that ©ay = ay and that if k ¥=j then ©a*, e 2+ (for use WIP). In turn we have © 2 + c 2+, © 2 _ c 2_, and hence ©2+= We conclude that ©II = II. For suppose that ©a* = c, > 0 and that at least two c, are strictly positive. Since ©“ *2+= obtain

this we 2+. where X+, we

a* = E d , a , , /SJ where d^ > 0 and at least two d^ are strictly positive. This contradicts WIP, and hence ©II = II, as desired. If k E J, then by (4), ©a^ = for some n e Z. But ©II = II. Thus naj = ai for some / e J. By WIP we conclude that I = k and n = 0. This shows that ©a^ = Thus ©Ig^^ = id and (ii) follows. □ Lemma 8 i , j E J, wa^ = ±ay.

Let

P ro o f

and

su p p o se

th a t w

e

W

is s u c h

th a t w r -w ~ ^

=

r^ o n

Q ^ .

Then

We have —a j

= rytty = >vr^iv” ^ay

= w{w~^Uj — <w” ^a:y, = ay —


5.1

407

Root Data

Proposition 9

Let i, j e J, and let w ^ W . The following are equivalent: (i) wai = Ci j . (ii) w a y = a ^ . Proof. If wa^ = t t j , then wr-w~^ — r, on (2k (Lemma 7). Thus on wr/iv"* = rf" (identification of W and W'^), and hence ± a / (the last lemma applied to IT instead of IT). Consider now the identity (4) of Lemma 7. For arbitrary ^ e it reads /3= 13+ (<w'-‘i 3 , a , " > - < ^ , < > )« ,. = /3 + (<j8,wa,>'> - <j8,a/>)a:y. Suppose that w a^= Then by setting j8 = we get - 4 a j = 0. This contradiction shows that w a ^ = a ^ , as desired. The converse follows along similar lines by dualizing. □ Proposition 10

Let i, j ^ }. If w ^ W is such that wa^ = aj, then wr{w~^ = Proof Using Proposition 9, we can replace {p,wa^^} = (p, a / > , so now it reads

a / > of equation (4) by 0)8 = p for all )3 e F. □

Proposition 11

Let a, )3 e n , a ¥= j8. Then the order o f r^r^ e W depends only on the product := <)8, a ^ > and is given by 0

1

2

3

2

3

4

6

> 4 00

Proof Let X ^ V and consider the vector space U(x) •= IKx + Ka + K/3. This is clearly invariant under r^r^. Assuming that x ^ Ka -\r Kp, the matrix of r^r^ \u(x) relative to the ordered basis (x, a, /3) of U(x) is of the form 1

0

* *

0

(P,a^y - ( a , 13"^}

-1

The Weyl Group and Its Geometry

408

and its characteristic polynomial is ( A - l ) ( A ^ + ( 2 - A / ' „ ^ ) A + l).

If X we drop the first row and first column and obtain the \a characteristic polynomial + (2 + 1. For the cases = 1,2,3, + (2 + 1 has roots that are conju­ gate pairs of primitive third, fourth, or sixth roots of unity. Thus r^r^\u(^x) has distinct eigenvalues, so is semisimple and clearly has finite order 3, 4, or 6, respectively. Since x was arbitrary, has order 3, 4, or 6 on V. For - 0, = r^r^, and since For > 4, 2< —2 and A^ + (2 —A/^^)A + 1 has no roots of unity as roots. Thus has infinite order. Finally, for = 4, r^r^lc/(0) has eigenvalues 1,1, and since r^r^\u^o^ # 1, it has infinite order. □ The above proof shows the following: Corollary Let denote the group generated by r^ and r^. Then (r^,r^) acts □ faithfully on Ka Kp. 5.2

THE LENG TH FUNCTION

We continue with the setup and notation of Section 5.1. In particular we assume that we have root data ® = {A, FI, II K, K < • , • » with root system X and Weyl group W, Given an element w e IF, iv 1, we can write ( 1)

W = r:

where ..., ^ J (these need not be distinct). Expressions like those of (1) are called words (of length n) of w. [Strictly speaking, words should be taken as sequences (r^^,. . . , r^) satisfying (1). Fortunately the less cumber­ some notation that we use is not likely to lead to any confusion.] There is nothing unique about the way in which an element of IF can be expressed as a word. As a trivial example. rj = rprj^

for all

; e J.

There is, however, a smallest positive integer n that permits w to be written in (1) as a product of n of these reflections. This number is called the length of w and is denoted by /(w). A word of w of length /(w) is called reduced. r , , from which it is r:Jn‘. then w~ We define /(1) = 0. If w = r, a

5.2

The Length Function

409

evident that /(w) = /(vv“ 0. In general there is more than one way to write w as a reduced word. The length of an element w of the Weyl group is closely related to the number of positive roots that are mapped into negative roots by w '^. More precisely for each w e PT we define 5^ = (a G 2+ I

G 2_}

We will show later (Proposition 3) that l{w) = card(5^). Lemma 1 Let j e J. Let w ^ W, and let

(0

be as above. Then

=

(ii) S^. = {«y}; (iii) ry(5^ \ {tty}) = \ {tty}; ( iv ) I f aj i S^, then Uj G and Srjy. = rjS„ U {tty} if aj G 5^, then aj ^

(disjoint union);

and

(v) card(5^) < Kw). Proof (i) The proof is clear. (ii) This follows from Proposition 5.1.6. (iii) Let a G \ {ay} c Then (2)

r y tt G

by Proposition 5.1.6. On the other hand, (rjW)~^(rja) = w~^a

e S_.

Combined with (2) this shows that

The reverse inclusion now follows by replacing w by rjW.

410

The Weyl Group and Its Geometiy

(iv) By definition, Uj G 5„, <=> w~^aj e X_, ^

^rjw ^

- w - ^ a j

G

2 _ .

Since by WUP exactly one of these holds, part (iv) now follows from part (iii). (v) By part (iv), card 5^.^ < card 5^ + 1. Thus part (v) follows by induction on /(w). □ Lemma 2 Let w = r, • • • r, be a reduced word o f w ^ W. Then r,-^1 • • • r,Jn-l^(a ,Jn^) ^ 2 + +. Proof. Suppose the result is false, and let m be the largest positive integer such that Om ***

^

Set a ’= r, • • • r, (a, ). Then a e 2+ and r, (a) ^ X_. Thus a = a.- by part (ii) of Lemma 1. Set w' — r^^^^ • • • As we have just seen, = a,Jm , and hence w' = r,Jm iv'r,Jn by Proposition 5.1.10. We can now find a word for w of length n — 2, namely w = r: • • • r,JmwV,Jn = r,J\ • • • Jm r,- —l w' = r-Jl • • • rJm • • • r,-Jn —1 (the hat indicating that this term is omitted). This contradicts /(w) = n.



Proposition 3 Let w = rj^ • • • rj^ be a reduced expression of an element w ^ W . Then (i) 5^ = {aj^, rjaj^,. . . , ... rj^_aj}, and the elements of above are all distinct’, (ii) card(5^) = /(w).

displayed

Proof Each of the expressions rj^,r^rj^,... ,r^^ ••• ^ is reduced, and hence each of the roots displayed above is positive, thanks to our last lemma. Also, if 1 < m < n, we have w~^r:J \ *• * r,Jm —\ a,Jm = r,Jn • • • r,Jm a,Jm = —r-J n • • • rJm + l a,Jm (with the obvious conventions when m = 1 and m = n \ and this last root

5.2

The Length Function

411

belongs to 2_, again by the last lemma. We conclude that •••

^■5«-

Suppose now that two of the elements listed above are equal. This leads to an identity of the form a,Jm = r,Jm • * r,J p —l a,J p for some 1 < m < p < n. Applying rj^ to both sides gives —a, = r

‘ •r

a, ,

which is impossible since the right-hand side belongs to X+ by Lemma 2. This shows that all the elements in question are distinct. Since there are n of them, both parts (i) and (ii) now follow from card(5^) < l(w) = n [Lemma l(v)]. □ Corollary 1 Let w ^ W . Then 5^ = 0 ^ IV = 1, 5«, = {a,}

= Vj.

Corollary 2 W acts faithfully on Q. Proof If

w \q

= 1, then 5^ = 0 and iv = 1 by Corollary 1.



Corollary 3 W = W Q a n d W = Wq. (see Remark 5.1.1) Proposition 4 (i) Let rj^ • • • rj^ be a reduced word for an element w ^ W . If j e J, then l{rjw) = l{w) + 1 «=> ay « 5^ l{rjw) = l{w) - 1 <=> tty e

H'-i(ay) e <=> ^ “ ^(ay) e 2_.

In particular l(rjw) = l(w) ± 1. (ii) Let rj^ • • • rj^ be a (not necessarily reduced) word for w. Then n = l(w) mod 2. (iii) I f w and w' are conjugate elements o f W, then l(w) = /(iv')mod2.

412

The Weyl Group and Its Geometry

Proof, (i) This follows by combining Lemma l(iv) with Proposition 3(ii). (ii) Use induction on n . l i w = rj^. .. then, for any j\ Krjw) = l(w) ± l = n ± l = n - \ - l mod 2. (iii) This follows from (ii). □ If S is a finite subset of the root lattice 0 , we define <5) = L r ^ 0 y^S The sums turn up as an important ingredients of the character formulas later on. If the space V contains an element p satisfying = 1

(3)

for all ; e J

(for instance, if II ^ is finite and linearly independent in K ^ (see minimal regular weights defined in Section 4.4), we have the following simple formula for <5^>. Proposition 5 Assume that p e Vsatisfying (3) exists. Let w,w^,W2 ^ W. Then (i) (S ^ ) = p - w p , (ii) Proof, (i) We reason by induction on l(w). The result being clear for /(w) = 0, we assume that w = rjw' for some w' ^ W satisfying /(w) = 1 + l(w') and that part (i) holds for w'. Then p — wp = p — rjw'p = P - rjp + r^(p - w'p)

= P - {p - (p^oij^)oij) + rjiS^r) = oLj + r^{S^>) = <5.> (this last equality by Lemma l(iv) and Proposition 4). (ii) We have = p - W^W2p

= p - WiP + H^i(p - W2p) = as desired.

5.2

The Length Function

413

Corollary (i) wp = p «=> w = 1. (ii) <5„,> = Wj = W2. Proof, (i) wp = p => p - wp = 0 => (5^> = O= > 5 ^ = 0 = > > v = l (Corollary 1 to Proposition 3). GO

(S „)

=

<5^^>

=» p

-

w ip

=

p

-

W2 P

= » W i“ V

jp

=

p

=» w r ‘ w 2 =

1

(by part (0) =►Wj = W2* Proposition 6 There exists a unique bijection /:2 ^ 2 ^ satisfying f(waj) =

/or all w ^ W. Moreover a e S +« / ( a ) e

Proof It is clear that if / exists, it is unique. Suppose that = ^ 2^]Then W2 ^^1^/ = hence v= a / (Proposition 5.1.9). Thus Wiuy= ^ 2« / . This shows that there exists a well-defined surjection / from 2 into satisfying way >-* way. Using Proposition 5.1.9 again, we see that this map is injective. Let a e X, and write it as a = w^^ay for some ; e J, w e IP. Then using Proposition 4 applied to the root system X and the coroot system X'^ together with the usual isomorphism of W and W a = w '(tty)eX+«»/(ryw) > /(w) « w-iay'^e X^ « /(a) Nidation The bijection / : X -» X satisfies /(ay) = a / . There is no ambi­ guity then in denoting f simply by to the extent that (ay)'^= ay. With this notation (w a,)'"= w ( a / ) , (4)

a

e X+<^ a'^e X

414

The Weyl Group and Its Geometry

Note also that if a e 2 and a = (5)

then

= {wa^. way) = {a-^,ay) = 2.

For each a e 2 define a reflection : jc

e G LiV) by

jc — {x, a ^>a.

Proposition 7 Let a,

e 2

(i)

e PF. TTzen on/y if a = ±]8,

GO

(iii) e PF, moreover, = r, /or all j e J, (iv) r^h = h — {a, h )a ^ for all h ^ V Proof (i) The proof is obvious from the definition and from Proposition 5.1.60). We have wr^w~^x = w{w~^x — {w~^x, a"^)a) = x — {x, wa' ^}wa. By Proposition 6, wa ^ = ()vo:)^, and part G O follows at once. Choosing w so that w~^a = a^, we obtain wr^w~^ = r,, which shows that Oii) holds. Finally, part (iv) follows from part (ii) and Lemma 5.1.2. □ Proposition 8 Let a, p ^ 1,, a

±p.

(i) The following are equivalent: (a) = 0. (b) r^a = a. (c) = r«r^. (d) ( P , a ^ ) = 0 , (ii) > 0 <=> > 0. Proof (i) (a) => (b) Obvious. (b) => (c) Proposition 7(ii). (c) => (b): r^r^ = r^r^ => r^^^ = r^a = ± a => r^a = a, since a — kp = —a is impossible. (c) <=> (d) Use symmetry. (ii) Suppose this is false. Then by (i) we have (6)

5.2

The Length Function

415

for some a and )3 in S. By Lemma 5.1.2 there is no loss of generality in assuming that in (6) a e n . Replacing by —/3, if necessary, we may assume that Now by the last proposition r^a = a - /3 while

r^a^= a ^ -

By (6) these two have different signs by WIP and this contradicts Proposition 6 given that (r^a) ^ □ Let I c J be arbitrary. Let III •=

\i ^ 1 }

and

:= ( a / U' ^ l},

and let AI denote the submatrix of A corresponding the index set I. Define Wi :=

clLcG L(K ).

For convenience we set = {1}. Subgroups of W of the form are called parabolic subgroups. (The terminology comes from the theory of finite­ dimensional simple Lie groups.) What follows are some basic facts about parabolic subgroups. Define S, :=

2 ,^:=

We also define the sets 5^ and the relative length function /j on Wi in the obvious way. Consider the six-tuple ®,:= { A , , U „ U , \ V , V \ ( - ,• }). It is obvious that the axioms RD1-RD3 of root data hold. RD4 is also obvious in the most standard case in which the sets Hi and are linearly independent. In Corollary 1 to Theorem 5.7.1, we will also show that RD4 always holds when dimF is finite. In any case, if 2)| is a set of root data, when Wi is its Weyl group, 2 i its set of roots, and its set of coroots. Proposition 9 Assume that S)| is a set o f root data and let Wi be its parabolic subgroup of W. Then (i) S i = 5 , for all w G W,; (ii) 11 and I coincide on \ (iii) if *rj^ • • • rj^ is a reduced word for w g PLj in W, then

g

I.

416

The Weyl Group and Its Geometry

Proof. Let IV e W^. It is obvious that /i(w) > /(w). Let S i := Clearly 5^ c 5^. We now apply Proposition 3 to conclude that /i(w) > /(w) = card 5^ > card 5^ = /i(iv). This proves parts (i) and (ii). Let w be as in part (iii). By Proposition 3, aj^ ^ 5^ = 5^, and hence aj^ = > 0. By WIP, j\ e I. Induction on n now completes the proof. □ Given I c J as above, we define a subset IT ^ of IT as W^:= [ w ^ W \ wa,. e 2 + for all i e l). By convention IT^ = IT. Proposition 10 Let w G IT. There exist unique elements iv^ e IT* and W2 ^ ITj such that w = WiW2- Moreover /(w) = + Kwf)Proof We reason by induction on liw) to show that iv = IV1IV2 for some Wi e IT* and IV2 ^ with /(w) = /(wi) + /(1V2). If /(w) = 0, then w = 1 and 1 = 1.1 is as desired. In general if w e IT* we are done, since we can write w = Wj. Suppose that w ^ IT*. Then there exists i e I such that wa, ^ X_; that is, a, e S^-i. By Proposition 4, l(wr^) = /(r^iv“ *) = /(w“ *) — 1 = /(w) — 1. By the induction hypothesis wr,- = IV1W2. where iv^ e IT*, W2 ^ + ^(^2) + 1 = Kiv), and therefore iv = W1IV2''/’ where e IT* and 1V2''/ ^ as desired. We now show that the decomposition is unique. Suppose that w = W1W2 = W1W2, where iVi,Wi e IT* and iV2,W2 ^

Then

Wj = W1IV2IV2 If 1V2W2 * ^ 1, then w'2^2

^ S i _ c 2_ for some i e I (Corollary 1 to

5.2

The Length Function

417

Proposition 3). Then e w'iSi_c X_ contrary to e Thus W2W2 ^ = 1 and hence proposition is now complete.

= w[. The proof of the □

Proposition 11 Let I c J be arbitrary. Let a e X, and suppose that in natural form {see Section 5.1), a = Xy^j^y^y Then a e Xi <=!►Cy = 0

for all j ^ I.

Proof (<=): We maintain the notation of Section 5.1. By assumption == Replacing a by —a if necessary, we can assume that We reason by induction on the height of p to show that ¡3 •= WiB^. If htijS) = 1, then = jS, for some i e I. Suppose that ht()8) > 1. Write

yej where dj > 0 [see (4)]. Then by (5) 2 = (p,p''}=

Since < 0 whenever 7 ^ I we conclude that <)8, > 0 for some i e I. Then ht(r^j8) < ht()8) so that r^,^ by the induction hypothesis. Thus p e rp^^Ai as desired. Finally,

a = ilf(p) G i/r(^"A,) =

= PT,n, = X,.

(=>): Conversely, if a e Xi, then a = wa^ for some i e I and w g IF|. Let ^

* * * '*a,y «zV • • • ’

^

''^/1 ' * *

^ k ^ i^ k ^ k is the natural expression of a.

T h e n P :=

=



Theorem 12 Let A = {A¿f) be an I X I Cartan matrix of finite type. Let 3 ) = (A, • , • }) be a set o f root data over R for A with dim V = n < 00. Let X and be the roots and coroots for 3 . Then card(X) and card(X^) are finite. In particular X and are finite root systems with associated Cartan matrices A and A ^ respectively.

418

The Weyl Group and Its Geometry

Proof. Since A is of finite type, the Coxeter-Dynkin diagram of A lies in the list of Theorem 3.5.4. In particular A is symmetrizable, say, by e = diagicj,. . . , ej), where > 0 and As is positive definite (Proposition 3.6.9). Since A is nonsingular, II = { a ^ , i s a linearly independent set. Define (* I • ) on A" := c K by (a, | aj ) = A^jSj, so (• | • ) is positive definite on It is immediate that each reflection r, is an isometry of (• 1• ) (see, for example. Proposition 4.4.6), and hence S = WYi U • • • U 5^ when Sj is the sphere of square radius (aj \ aj) in X. Since Sj is compact and 2 c is closed and discrete, Sj n 2 is finite, and hence 2 is finite. In precisely the same way 2 ^ is finite. Of course we can identify V ^ and the dual space K* of K by < • , • >, and then we easily see from 2 c 2Za^, 2^c2Za^^ that e Z for all a , e 2. Also ( a , a ^ ) = 2 for all a e 2. Then 2 and 2 ^ are seen to be finite root systems (Section 3.2), and hence II is a base for 2 in the sense of finite root systems (Section 3.3). Thus A is the Cartan matrix of 2. Similar remarks apply to 2 11 and A^. This completes the existence part of Theorem 3.5.4. □

5.3

COXETER GROUPS AND THE EXCHANGE CONDITION

Let 5 be a set, and let oo be a symbol. A Coxeter matrix (on the index set S) is a matrix R = (M^^O indexed by 5 X 5 satisfying 2>2 Li m ss'

if s

s'.

for all s,s' ^ S = 1

for all s ^ S.

Our intention is to attach to the pair (5, R) a Coxeter group. This is done as follows. Let G = G(5) be the free group on the set S (see [Ja2]). We recall that a typical element of G can be written uniquely in the form cj?2 . . . where for all i we have 5, e 5, e Z \ {0}, and Let H be the normal subgroup of G generated by all elements of the form

53

Coxeter Groups and the Exchange Condition

419

such that ^ (note that oo ^ Z+). The Coxeter group C(5, R) of the pair (5, R) is now defined by C ( S , R ) := G/ H. A group C is said to be a Coxeter group if C = C(5, R) for some pair (5, R) as above. Remark 1 If = oo, then ss'H is of infinite order in G/ H. This justifies the choice of symbol oo. Since = 1, ( sH Y = 1/f for all 5 e 5 (i.e., C is generated by involutions). The following important result provides us with an endless list of interest­ ing examples of Coxeter groups: Theorem 1 Let W be the Weyl group o f a set o f root data 2) as above. Let S =

be a set indexed by J.

Define for all i, j e J, ' order o f r jj )

whenever r^r^ is an element o f finite order o fW otherwise.

( see Proposition 5.1.11)

Let R := (m

). . .

Then W is isomorphic to the Coxeter group C = C(5, R) o f type (5, R). In particular W is a Coxeter group. Proof We keep the above notation. For convenience we write Sj instead of SjH (i.e., Sj is the image of Sj in C = G/ H) . It is clear that there exists a (unique) homomorphism W satisfying for all j e J. Moreover if/ is surjective. Our intention is of course to show that ip is injective. We do this by following an adaptation of an argument of Steinberg [St].

420

The Weyl Group and Its Geometiy

Suppose that if/ is not injective. Then there exists an element SjJn # 1

( 1) such that

( 2)

n = 1-

Furthermore we assume that n above is chosen so as to be minimal. It follows from (2) and Proposition 5.2.4(iii) that n = 2m is even. Moreover m > 1 (and hence n > 4) because of the way in which C is defined. We can therefore write y. *. * jr,

= jr.

• ••

Jim

Jm+2

This shows that r, • • • r,Jm + l is not a reduced word and hence that there exists a smallest positive integer k < m such that W := r^*+1

Jm + \

is a reduced word but r, r, • • • r, is not. By Proposition 5.2.4(i) we have aj^ e 5^. We can now apply Proposition 5.2.3(i) to conclude that a,Jk = r, • • • r.ia, ) Jk + 1 Jt^ Ji + \J

for some k < t < m,

Then by Proposition 5.2.7(ii)

/-,Jk = r,Jk + \ • • • r,Jt r,Jt + l r,Jt • • • r,Jk + l so that 0*

r.Jt = r-Jk+l

Jt+l'

We claim that k = 1 and that t = m. Otherwise, Sj. = 5;,..

Jt + l

by the minimality of = 2m. By replacing the above left word by the above right word in the original word, we obtain SiJn =S:Jl

SjSj Jt Jt+2,

By applying if/, we conclude that the right-hand side of the last equation equals 1 (this because of the minimality of n) and hence that Sj^ • • * Sj^ = 1. This contradiction shows that k = 1 and that i = m, as desired.

5.3

421

Coxeter Groups and the Exchange Condition

It follows that

r,J1 • • • r,Jm

ГJ2 : • • * r,Jrrt + l

and that (3)

a,

-^1 = r}2

• • • Г: ( a ,

Jm^ Jm+i^) .

Now Sj^ *• • SjSj^ (otherwise Sj^ • • • Sj^ = 1) and • • • SjSj^) = \l/(SjSjSj^ • • • SjJSj^) = 1. Hence we can apply all of the above reasoning to this element to conclude that r,Jm + 1 = Г:3 *‘ * ГJ:m +2 j

We rewrite this expression in the form r,J = 1

r,J3 r,J2 ГJ3 : • • • ГJm : + l r,Jm+2 ГJm : +\

a

to see that S:Jm + l S:J m +2 S,Jm + \,

Su) = 1-

But S,

-'/71 + 1

S:

-'/7 1 + 2

S: , •'/71 + 1

Otherwise, if we multiply on the left by

a

we obtain

5,J m +2 = 5,-J\ S:J S:J 3

m + 2 symbols

S,J Ф 1.

m

a

s,Jm+\ ■ "

symbols

and we can then substitute the right-hand side of this expression into.our S,J2m to shorten it, thus contradicting the minimality original word 5 of n. S:J O f C o f S:Jm. . .+. .1S,-Jm + 2 S,Jm + 1 Here then is a nontrivial word 5,J3 5,J2 5,J3 length n whose image under i/r is 1. If we apply the above reasoning to it, we conclude just as in (3) that a

a,

J3

= ГJ:2

•••

ГJrr^ : ( a ,Jm + l )'

= a, . Jl

Thus = У3. Cyclically permuting the product, we conclude that /3 = = **■ ^ h m - v the same fashion we show that j’2 = j 4 = •• = ; 2mThus our original relation was (O /y.)” = 1-

422

The Weyl Group and Its Geometry

But then m is divisible by the order rrij^^ of and hence Sj^... Sj^ = = 1. This contradiction establishes our result. ”□ Next we investigate the {A, n , n F, F ^, < * , • ) ) be Weyl group W = . Suppose that w = is Proposition 5.2.4 either

so-called exchange condition. Let ® = a set of root data with root system 2 and We maintain the notation of Section 5.1. a reduced word of W. If + i e J, then by

Krj„^w) = l ( w ) + 1 or =l(w) - 1 . In the first case r, r, • • • r, is a reduced word for r, w, while in the second it is not. The exchange condition allows us to find a reduced word for 0„+i^ when Krjw) = /(w) — 1. More precisely it says that there exists some 1 < k < n such that r, w = r,- • • • r, ' ’ r , , where, as usual, " means deletion. We introduce a change of notation that will avoid the use of so many double indices. (The new notation also parallels the standard notation employed in other texts when dealing with these topics.) Define S := (o 1y e J} = [ r j a e n} and T '= [ wsw M *5 e 5 and

w

^ W).

With this notation every element of W is of the form 5i,. . . , e 5. Note that by Proposition 5.2.7, r= { rjaex } . We have already seen that the map

given by a ^ is a bijection (ibid.).

s„ for some

5.3

Coxeter Groups and the Exchange Condition

423

Proposition 2 (Strong exchange condition [Ve2], [Del]) Let w =

^ W, and let t =

^ T, where a e

(i) The following conditions are equivalent: SECl:

w~^a e 2_,

SEC2

l{tw)
(ii) If either of the conditions (i) hold, then SEC3:

tw = Si ' ' '

' ' ' s^ for some 1 < i < n.

(iii) If Si • • • is a reduced word, then SEC3 is equivalent to SECl and SEC2. Furthermore the value o f i appearing in SEC3 is unique, (iv) I f t Ei S and Si • • * is reduced, then the word 5^ • • • 5^ • • • o/ tw prescribed by SEC3 is reduced. Proof We first show that SEC2 SECl => SEC3. Assume SECl. Let 1 < i SEC3. This argument applied to a reduced word of w shows that SECl => SEC2. If we now replace w by r^w, we obtain from SECl => SEC2 that w V„a e 2 _=> l(r„r„w) < l(r^w), or equivalently that l{r^w) < l(w) => w

E 2 _,

which is precisely SEC2 => SECl. This establishes parts (i) and (ii). If is reduced, it is clear that SEC3 => SEC2 and hence that all three conditions are equivalent. In addition, if ^1 *• • s,. • • • where i < j, then *^1 *** ‘^/‘^/+1

S„

=

5l

■■■

Sj

■■■

S„,

• • ■ Sj = Sj ■■■ Sj_i. Thus •



■■■

S„

= s^ ■■■

Si

■■■

Sj



which is impossible since Si • • • is reduced. This finishes the proof of part (iii). Finally part (iv) follows from /(^vi^) < l(w) => l(sw) = l(w) - 1 (see Proposition 5.2.4). □

The Weyl Group and Its Geometry

424

Remark 2 The implication SEC2 => SEC3 is referred to in the literature as the strong exchange condition and as the exchange condition in the case when i e 5. The exchange condition was first established by H. Matsumoto and the strong exchange condition by D.-N. Verma. The term “exchange” is then due to the following: If ts^ • • • tSi • • • Si_i = Si • • • Si, which says that we can “exchange” t on the left with s, on the right of 5i • • • Si_i. Note that then tSi

Si

S ^ =

Si

and hence we have the corollary: Corollary 1 I f s ^ S and Ksw) < liw) then w can be written as a reduced word of the form SS2 • • • Corollary 2 Let w = Si • • •

e PT. Then there exists 1 < ¿i < ¿2 < ' "

< n such that

and Si^ • • • Si^ is a reduced word for w. Proof If Si • • • is reduced, the result is obvious. Otherwise, there exists a largest j such that Sj+i • • is reduced but SjSj+i ' • s^ is not. By the exchange condition, we have •^1 *’ *

~

where j < i < n. By repeating this argument, the corollary follows.



Remark 3 Let 5 be a subset of a group G. Assume that S generates G and that the elements of 5 are of order 2. Since 5 generates G, there is an obvious concept of a length function. Suppose that the “exchange condition” holds. Thus, if Si, , . . , s^ e 5, then /(^1 •••

<1(S2 •••

=>^i

5/

s„ for some i.

It can then be shown that G is a Coxeter group. (This was first shown by H. Matsumoto [Ma]; see also Bourbaki [Bo]). Therefore, if a group G is

5.4

The Bruhat Ordering

425

generated by involutions, G is a Coxeter group if and only if G satisfies the exchange condition. Remark 4 It is known [Mt] that in a Coxeter group G = (C, S) any word S1S2 ' " that equals 1 can be reduced to 1 by successive applications of the following type of substitutions: by

Replace

••• m,, terms

Replace

by

Remark 5 The Coxeter groups that appear as Weyl groups are precisely those for which the entries s s' of the Coxeter matrix are 2 ,3 ,4 ,6 ,00. The restriction that e {2,3,4 ,6 ,00} for all s s' is called the crystallo­ graphic restriction. Thus Weyl groups are, as Coxeter groups, precisely those that satisfy this crystallographic condition. The strong exchange condition is a theorem that applies to all Coxeter groups. However, to prove this one needs to introduce a more general form of root system introduced by [Deodhar]. For a recent treatment of this see [Hu2]. Proposition 3 ([St]) Let 2) = • \ • )) be a set o f root data with root system S and Weyl group W. Let G be the group with the presentation generators: a: e 2 relations: R^R^R~^ = R r ^i^Then the mapping G phism of G into W.

W defined by R^ ^ r^ for all a

Proof See Exercise 5.13.

5 .4

is an isomor­ □

THE B R U H A T ORDERING

Let W be the Weyl group of a Kac-Moody Lie algebra. In this section we define and study a partial ordering on W called the Bruhat ordering (or perhaps better the Bruhat-Chevalley ordering). The Bruhat ordering has numerous applications to the study of Weyl groups, weight systems, flag varieties, Verma modules, and combinatorics. Although we treat only Weyl groups here, the results in this section apply to all Coxeter groups [Hu2]. As in Section 5.3 define 5



{r„

I a

G

n }

426

The Weyl Group and Its Geometry

and r==

и

= {r„ 1«

Define a partial order < in Ж as follows: Given w and w' in Ж set >v < w' if and only if either w = w' or there exists a sequence Wq, w ^, ... of elements of W such that BOl: Wq = w and = w', B02: Kw^) > /(vv^_i) for all 1 < i < p, B03: w¿ = with e T for all f = 1 ,..., p. A sequence Wq, w ^, . •., as above satisfying B 01-B 03 is called a chain of length p joining w to w'. In this situation it is convenient to write w' = tp ... t^w and call this a chain of length p joining w to w\ It is rather easy to see that < is indeed a partial ordering, the Bnihat ordering in. The following diagram depicts the Bruhat ordering for the Weyl group of type C2.

(r a^'r a2' T«1T«2r«1 r

r

«1r «2

r

“1

notice that

< r O'!r «2 —

0^2r «1

«2

For example, to see that r

0^2r «1r «2

r

<^2r

5.4

The Bruhat Ordering

427

Remark 1 Since => that B03 could be replaced by B03':

e with

it is clear

e T for all ¿ = 1 , , n.

Thus the “left” and “right” Bruhat orderings are the same. We record the following simple facts. Our approach to the Bruhat order­ ing follows Deodhar [Del]. (1)

Ifw G Wand t ^ T, then tw < w

l(tw ) < l(w ).

Indeed l(tw) and /(w) have different parity (Proposition 5.2.4). (2)

w)v=l;l<w

for all w ^ W,

Lemma 1 L e t w ,w '

and s ^

S, If w

<

w ', t h e n e it h e r s w

<

w ' o r sw

<

s w '.

We may suppose that w ¥= w'. First suppose that tw = w' for some t Ei T. If s = t, then sw = tw = w', so that we can also assume that s ¥= t. We want to show that sw < sw'. Since (sts)sw = sw', it will suffice to show that l(sw) < l(sw'). Suppose not. Then l(sw) > l(sw') = l((sts)sw). Let w = be a reduced word of w. Then ss^... s^ is a word for sw and by the strong exchange condition there exists some 1 < / < n such that stsss^ • *• s^ = • • • Si_i. (Note that because s t the right-hand side is not the empty word.) It follows that

P ro o f

S tS S S ^

•••



Thus w' = tw = Si

Si

s^.

and this contradicts the fact that l(w') > l(w). To establish the lemma in general, we let w' = • • • t^w be a chain of length k from w to w' and use induction on k. Let w" = tj^_^ • • • t^w. Then w < iv" < w' and by induction either sw < w" or sw < sw". In the first case we are done: sw < w'. On the other hand, w' = tf^w" so that either sw" < w' or sw" < sw', and the second case follows. □ Proposition 2 (Subword condition) Let w, w' E W, and let w' = s ^ ... s^ be a reduced word for w'. Then w <w ' if and only if w = Si^ *• * for some 1 < • < i^ < n. Furthermore, if w < w', then the subword S: **• S: can be chosen to be reduced. Proof. Suppose that w < w'. Let w' = t ^ .. . t^w be a chain of length k from tv to tv'. We show that tv can be written in the form s, ... s, by induction on

428

The Weyl Group and Its Geometry

k . l i k = 1, then by the strong exchange condition SEC3, ^

• • • 5,. • • •

To establish the general case, we repeat this argument. Conversely, suppose that ... Si^, We show that h' < w' by induction on the length of w'. If Z(w') = 0, the result follows from (2). We now distinguish two cases # 1. Then by induction W=

<52 • *• 5„ = S^w' < w'

(by faCt 1) .

¿1= 1. Then by induction 5,^ • • • 5,^ < 52 • • • 5„, and hence by Lemma 1 either w = S:*1 • • • 5,‘■m< 59^ • • • 5„^ < 5; • • • 5: < 5; 5o *** S„ = W'. For the final statement use Corollary 2 to Proposition 5.3.2.

or >v = □

Proposition 3 (Z-lemma) Let < be the Bruhat ordering o f (IT, 5). Let w, w' e IT, and let s E: S. Suppose that l{sw) < l{w) and that l{sw') < /(u^'). Then the following condi­ tions are equivalent: Zl: w < w', Z2: sw < sw', Z3: sw < w' .w' w sw Proof Write w' as a reduced word s^ • • • 5„ with s^= s (Corollary 1 to Proposition 5.3.2). Z l => Z2: By the previous proposition w = s^^ • • • 5,^ for some 1 < ¿^ < • • • < ¿^ < n. If ¿1 = 1, then sw = 5^^ • • • Si^ so that 5w < 5w' = 52 • ** s^ by Proposition 2. Ijf ¿1 ^ 1, then we use the exchange condition to conclude that sw = 5;, • • • 5; • • • 5, for some j. Now this is a subword of sw' = 52 ... 5„, and hence sw < sw', Z2 => Z3: The proof is clear, since sw' < w'. Z3 =» Zl: By Proposition 2, sw < w' => sw = s¿^ • • • s¿^ for some 1 < i^ < • • • < i^ < n. Then w = 55^j • • • 5^^, and this is always a subword of 5. • • • 5„. Thus w < w'. □

5.4

The Bnihat Ordering

429

Proposition 4 Let w,w' ^ W be such that w < w ',w ^ w'. (i) There exists a chain of maximal length joining w to w'. (ii) In any chain w = Wq < < ••• < = w' o f maximal length we have /(w^) = iw¿_f) + 1 for all 1 < i < p. In particular, all maximal chains are o f length Kw') — l{w). Proof (i) The proof is obvious from the definition of chain. (ii) The result will follow if we can show that given (3)

there exists a chain w^, Wj, • • •, = 1.

as above then

joining w to w' such that l{w^ —

If /(w') - /(w) = 1, then w' = tw for some t e T because of B02 so that the result is clear. Thus if the proposition is false, then (3) fails to hold for some pair w < w' with Z(w') - l(w) = N > 2 ,B y choosing N and l(w') as small as possible, we may assume that for sll a,b ^ W with a < b wo have INDl: (3) holds for a and b whenever 1(b) — 1(a) < N, IND2 (3) holds for a and b whenever 1(b) — 1(a) = N and 1(b) < l(w'). Note that if w = 1, then the result is obvious. We henceforth assume that w 1. Let be a reduced word for w'. By Proposition 2 we may assume that w admits a reduced word of the form w = 5^^... 5,^ for some nonempty sequence 1 < • < i^ < n. Case 1.

1. By Proposition 2 IV =

• • • 5,-^ < ^2 • • •

= W'.

Then INDl implies the existence of a maximal chain joining w to s^w', and this with one more step gives a chain from w to w' satisfying (3). Case 2. = 1. Then /(ijw) < l(w) and /(5iw') < l(w'). By the Z-lemma we have s^w < s^w', and by IND2 we can join SiW to s^w' with a chain. w

(4)

w

-s.w p-l

430

The Weyl Group and Its Geometry

with /(w^) = /(iv,_i) + 1. Notice that p > 2, since Ks^w') — Ks^w) = l(w') — l(w) > 2. There are two subcases Case 2a.

By the Z-lemma

w

5iW' we conclude that w < < w'. If w = s^w^, then = s^w, and this contradicts p > 2. Similarly ¥= w'. Thus l(w) < < l(w') so that by INDl we can join w with and with w' (hence w with w') in the desired fashion. Case 2b. < w^. By the Z-lemma

s^w so that w < < s^w' < w\ But l(w) = /(^ivv) + 1 = Hence w < => w = Wj. Thus (4) shows that we have a chain from w = to w' as required. □ Remark 2 Proposition 4 shows that B02 can be replaced by the stronger looking B02': l{w^) = /(iv^.j) + 1 for all I < i
MORPHISMS OF ROOT DATA: SUBROOT SYSTEMS

Throughout this section 3 = (A , II, H K, K ^, < * >* )) will denote a set of root data over K. Let 3 ' = (A \ U \ H ' V', ,• >') be another set of root data over a possibly different field IK'. We use ' to denote the objects

5.5

Morphisms of Root Data: Subroot Systems

431

of 3 '. For example, n- - { a » ,.,,.

A morphism of

into

is a pair (
of Z-linear maps

such that MORI: (p(U) c n ' and c MOR2: <x, y) = ((p(x),(p^(y)y for all x e Q and y ^ Q^. The concept of isomorphism and automorphism between sets of root data is defined in the obvious way. Note that no assumptions are made on the relationship of V to V' and to F ' In fact 3 and 3 ' can be isomorphic without V and V' being defined over the same field. We denote by Aut(.^) the group of automorphisms of 3 , Example 1 Let 3 = {A, B, B 1^, 1^*, < • , • » be the universal covering of 3 (see Section 5.1). Recall (see Proposition 5.1.1) the unique Z-linear maps ilf:Q-^Q

and

ijj \ ßj ^ aj

and

given by

Then

3

(/f ^ : ßj^ ^

.

3 is a. morphism (said to be canonical).

Proposition 1 Let ((p,(p^): 3 ^ 3 ' be a morphism. (i) For fl// a G n and a' e II', (p{a) =«'<=> ( p ^ ( a ^ ) = a '^ .

In particular
for all a, e II. II' ^ are injections.

432

The Weyl Group and Its Geometry

(iv) There exists a unique homomorphism r : W ^ W' satisfying r(r^) = ^
(1)

Q' t(w)

Q

Q

and

V

J L . g ,v

^

1 Q'

r(w)

1

commute for all w ^ W . (v) (p maps S {resp. S_) injectively into S' {resp. S'+,S'_). Similar statements hold for cp^ and S Proof (i) Assume ' < 0]. The reverse implication follows along similar lines. (ii) The proof is obvious from part (i). (iii) Assume that a, ß ^ U, a ¥=ß, and that

( a , ß ' ' ) = { ( p ( a ) , ( p ' ' { ß ^ ) ) ' = { < p ( a ) , ( p ( a y y = 2.

(iv) and (v): By Theorem 5.3.1 and Proposition 5.1.11, W is 2l Coxeter group, and the orders m^ß of the products depend only on (a, ß ^ ) { ß , a ' ^ ) . Similarly W' is a Coxeter group, and now part (ii) shows that the map r^ ^ a e n extends uniquely to a homomorphism T iW ^W ', Let X ^ Q and a e II. Then =
5.5

Morphisms of Root Data: Subroot Systems

433

From this it is clear that
n S ') = 2'^,

and similarly
Since T is injective, it follows that vr^'V ^ = r^. and hence by Proposition 5.2.7(i), (ii) va' = ± a , so w'a' = ± wa. But w'a' = -w a is impossible, for then c p ( w a ) = c p ( P ) =
and hence


Corollary // I c J, I =?i= 0 , ¿znd is the subgroup o f W generated by the reflections r,, i G I, then Wi is the Coxeter group with generators {r^ I i ^ 1} and the relations (r^ry)'”'-' = 1, where m^j = is given by Proposition 5.1.11. Proof Let '= (Aj, n ,, IIi'^, F, K ^, < • , • » be the set of root data ob­ tained by restricting A, n , and 11^ to the index set I. Then we have the obvious morphism of into 3 , and hence by part (iv) of the proposition, the Weyl group of 3 ^ (which is a Coxeter group) is mapped injectively onto Wj, □ Remark 1 If the pair (cp,(p^) is an isomorphism of root data, then (p: S S', ^ ^ : S S ' ^ are bijections and r : IP ^ IT' is an isomorphism of IP and IP'.

434

The Weyl Group and Its Geometry

Remark 2 Proposition 1 makes it clear that the essential information in a set of root data is contained in the mai^ix A. _ _ Let K be a field containing K. Let F = and_F ""= tK® The pairing < • , • > extends uniquely to a (nondegenerate) IK-pairing < • , • >r : F X

K.

For all a e n J e t a == 1 ® a e K ^milarly define a ^ 1 ® a e V for all a e n'^. Let n := { a l a e n} and n^== ( a | a n T h e n

is a set of root data oyer IK said to be obtained from ^ by extension of the base field from IK to IK. Obviously ^ and are isomorphic as root data via a a, a ^ a It is also quite easy to restrict the field. We begin again with Let F be a subfield of IK. Let ^ Q ^nd ^ be the K-linearly indepen­ dent sets in V and V ^ whose Z-spans are Q and Q ^ as given by RD4. We claim that there exists a set M d I and F-linear spaces Fp = Fp^ = 0^^j^Fj8y^, and a nondegenerate pairing <-,->F:nxFp" such that F =

for all i , j e I.

For instance, set M == lU I', where I' = {i' 11 e 1} is a set equipotent to I. Form vector spaces Vf and Ff'^ with bases {j8,}, eM ^^d {/3j}, eM> ^nd define < • , • >F by (^¡yPj''>r = <%■>')'/>> F = <j8,,/3/>F = 5,y, F = 0

for all i , j e I.

Now set Q = 0 Z i 3 ,c F F , /e l

Q'':= 0 Z ) 8 J c F f^ /el

Then Q - Q, Q ^ as Z-modules via y-, respectively, and we can thereby identify II and II ^ as subsets of Q and Q After doing

5.5

M orphism s o f Root Data: Subroot System s

435

this, we evidently have a/>iF = Aij

for all /, j e I,

and we see that • , -»F is a set of root data over F isomorphic to In particular we can construct rational root data in this way and then by extension obtain root data isomorphic to ^ over any field F of characteris­ tic 0. This allows us in Section 5.6 to use F = R and thus take advantage of the topology of R" in proving results about root data. Let be a set of root data with root system 2. A nonempty subset ft of 2 is a subroot system if for all a, e 2, CK,)S e ft =>

e ft.

In view of the remarks we have just made, the fact that ft is a subroot system of 2 is independent of the particular set of root data in which 2 is manifested. We study subroot systems in Section 5.7. Proposition 2 Let .^ = (.4, n , n ^ , K, < • , • >) and = { A , ft', F', F ' \ be isomorphic sets of root data over fields IK and K' via a pair of maps (cp,(p^) for which the corresponding isomorphism o f their Weyl groups is T\W ^ W \ Then w EiW is a reflection in the space V if and only if rw is a reflection in V'. Proof Let Q q (resp. ^ q) be the rational span of Q in F (resp. Q in F')Clearly


<S) <2q = C k C K; Q

® Q q - Q k' ^ V'Q

Let w G IF be a reflection. By restriction to Q q we obtain the nontrivial (by the Corollary of Proposition 5.2.3) involution w on Qq. Now w has eigenvalue - 1 with multiplicity exactly one on F and w has - 1 with multiplicity at least one on Qq. Because of (2) w has eigenvalue - 1 with multiplicity one also, and so vv is a reflection (see Section 3.1), say, with a hyperplane H of fixed points.

436

The Weyl Group and Its Geometry

By means of the diagram (1) we see that = tw \q'^ and hence that is a reflection in the hyperplane H' — Let us see that this implies that w' '= tw is itself a reflection of V'. Let

tw \q'^

h'^H' By (2),

is a hyperplane of

and hence = K'y e H i .

where y e Q'^r \ {0} is chosen so that w'y = - y . Let F denote the space of fixed points of w' in V'. We observe that by the definition of w' as a product of a'j e II' (since w' e W'), one clearly has w'x G X + for all X G V', Thus writing X =

we see that V' c

w'x 2

X — ------------------ +

w'x 2

X + ------------------

+ F, Thus V' = K'y

H i . - \ - F = K'y 0 F,

and therefore w' is the reflection in y with F as its hyperplane of fixed points. □ 5.6

THE GEOMETRY OF A SE T OF ROOT DATA

Let ^ = (A, n , n V, V • » be a set of root data over U. We main­ tain all the notation of the previous sections except that now IK is replaced by R. Throughout the section we also assume that dimgj(F) = n is finite. Because of RD2 and RD4 we have dim,R(F^) = n, J is at most countable (though not necessarily finite), Q= and Q ^= for some {%} c Q and c g ^ linearly independent over R. Henceforth we will think of both V and V ^ asjopological vector spaces by identification with R". If 5 c R", then 5^ and 5 will denote the interior and closure of S, respectively. In this paragraph we study the action of the Weyl group W on V from a geometrical point of view. The principal object of interest is a certain convex cone 3£, the Tits cone, in V. The Tits cone is decomposed into a collection of

5.6

The Geometry of a Set of Root Data

437

smaller cones by a set of hyperplanes H, one for each positive root of the root system 2 associated to 3 , The Weyl group operates so as to leave 3£ stable and to permute these smaller cones amongst themselves. Since V and V ^ can be interchanged by replacing ® by ® there is another Tits cone X ^ in F Both are used in the theory of contragredient Lie algebras. (Warning: Some authors use X and X^ with exactly the opposite meanings to ours. We prefer to keep “checked” objects in V ^.) Much of what follows concerns hyperplanes of V. Any such hyperplane is of the form / / = {x e V \{ x, h ) = 0}, where /i e F

It decomposes V \ H into two open half-spaces i / ± = [x e V \ ( x ,h ) e ±R^}.

Two points X, y e V \ H are on the same (resp. opposite) side of H if x , y lie (resp. do not lie) in the same one of these two open half-spaces. H separates x and y if x and y lie on opposite sides of H. If h,h' ^ V ^\{0} define the same hyperplane H, then h! = ah for some nonzero e K. The reason is that if V = H ® Ru and a is defined by ( m, W) = a{u, h), then <jc, h! — ah) = 0 for all x e F. Given any set H of hyperplanes of F we can define a relation h on F by X y if andonly if for each hyperplane / / e H either jc, ye / / or x, y lie onthe same side of H, It is obvious that ^ is an equivalencerelation. If X, y e F, X y, we denote by [x, y] (resp. ]x, y[) the closed (resp. open) line segment joining x and y. Thus = ( tt + (1 - i )yl 0 < i < 1}, = {a: + (1 - i ) y | 0 < i < 1}. Let X and X be the set of roots and coroots of respectively, and let JV be its Weyl group. Thus X = WTl, X ^= WU'', and for all x ^ V ,

{wx,h} = {x,w~^h}. For each a ^ e X

define the hyperplane /f„v:= { x e

= 0}.

438

Since

The Weyl Group and Its Geometry

{a, a ^ ) = 2, w e have V = Ra 0

Clearly is a reflection that interchanges the two half-spaces V as its hyperplane of fixed points (Section 3.2).

and has

Note that H^v= a^= (Proposition 5.1.6) <=> r ^= ±jS ^ (this last by Proposition 5.2.7). Set H == The equality {w~^x,

= <jc,)va^>

for all jc e K, w e W,

2^,

shows that wa and hence that W acts as a group of permutations of H. The fundamental chamber (relative to H ^) is defined as f := |x € V\(x, a / > > 0 for all ; e j | . For each subset of I of J define the set Fj = (jc e F |< jc ,a /> = Oif / e l a nd ( x , a ^ ) > Oif i e J \ l } .

Note that F = sense that

Each of these sets Fj is convex, and each is a cone in the X G Fj => (R+x c F ,.

Since the elements of n ^ are not necessarily linearly independent, there is no guarantee that Fj ^ 0 . Notice, however, that Oeif^== ¿ej

5.6

The Geometry of a Set of Root Data

439

Given two subsets A and B of V, we say that A supports B (and that B supports A) if A and B have the same affine span. Proposition 1

(i) # 0 . Moreover F °= F. (ii) For all k ^ J we have that F^|^^ spans, hence supports, the hyperplane (iii) F = U , c j ^ i y / be as in RD4. The set A = {x V \ ( x , y n > 0 , Proof, (0 Let ! < / < / } is open and nonempty. Since 2 + c ©/ = ; it is clear that A c F. Thus F° 0 . We claim that for all 0 < i < 1 we have iF + (1 t)F^ c F^. Since the^eft-hand side is open, it will suffice to show that it lies in F. Now, if X ^ F, then <jc, a /> > 0 for all j G J. Let y e F^, and 0 < i < 1. Then (tx + (1 — t)y, aj^) > 0 for all j G J. This establishes our claim. Finally, if a : g F and y g F®, then ]x,y] c F° so that x g F®. (ii) Let B be an open ball in F. For each x E: B, rj^x satisfies the inequalities

> 0

j ^ k.

The same goes for every point of the interior U of the convex hull of B\jvj^B, Now U riH^v is a nonempty subset of ■f(*} from which part (ii) follows. _____ (iii) Let X G Fp If_y g F, then ]x, y [ c F . Thus j c G ] x , y [ c F . This shows that U i c The reverse inclusion is clear. □ Proposition 2

For each subset I c J for which Fj ^ 0 , Fj is an equivalence class of

jj.

Proof Let a : G Fj, and let x denote the equivalence class of x in V, Evidently X c F|, since Fj is defined by a subset of of the relations defining X, Now suppose that y g F j, and let a ^ G 2"^. Since //^ v = we can suppose that a ^ g and write a Ey^ with Cy > 0. Then <jc, a = Eye ^ / ) ^ 0 with equality if and only if ; g I whenever Cy # 0. It follows that 0 and <x, a^> = 0. Thus either x and y both lie in or both lie in This proves y x. □ Recall the parabolic subgroups PT|, I c J defined in Section 5.2. Proposition 3

Let I, I' c J, and let w e W, I f wFj n FJ =?^= 0 , then I = I', wF| = F^> = Fj, and w e W^. Moreover w fixes F| pointwise.

440

The Weyl Group and Its Geometry

Proof. We use induction on the length Kw) of w (relative to {rfi e J}). If l(w) = 0, the result is clear. Suppose that /(w) > 0. For any i e J, we have the following chain of equivalences: l{r^w) < l{w) <=» w

e 2^

«

e

(Proposition 5.2.4 applied to 2

2: > 0

<=> {r^wx, a f ) > 0 <=»

for all X e F for all j: e F

c

<=> wF c H~y.

( 1)

Thus l(r¿w) < l(w) => wF Cl H~y gives (2)

^

^

C\F

Now suppose that x e jv F jJl Fy # 0 . Choose / e J so that Kr^w) < Z(]r). Then X e wF^ fl Fy c wF C\F a by (2) and Proposition l(iii). As a result X = r¿x e and x e FJ. Hence x = r^x e r^wFi H Fy, The induc­ tion assumption implies that I = I', r^wF^ = Fy = Fj, and e PPj. How­ ever, X G H^y n Fy <=> Z G I' = I. Hence iv g PFj and wFj = F|. That w fixes Fj pointwise follows from w ^ □ Since W permutes the set of hyperplanes H, W preserves the equivalence relation and hence permutes the equivalence classes of ^ h - particu­ lar each of the sets wFj, I c J, is an equivalence class if it is not empty. We call these particular equivalence classes facettes. The union of all the facettes is the Tits cone 3E

:=

U { i v F i | w G P T ,I C J }

= \j{wF\w

G

W}.

Since each Fj is a cone, it is evident that 3£ is indeed a cone. Furthermore 3£ is PT-invariant. Since F^ ^ 0 , the interior of 3£ is nonempty. If two facettes vwFj and w'Fy intersect nontrivially, then by Proposition 3, I = I'. Thus each facette has a well-defined subset I of J associated with it, called the type of the facette. The facettes of type 0 , which are of the form wF0 = wF, are called the chambers of 3£. These are precisely the facettes that have a nonempty interior. The facettes of type {/}, with i g J, are called faces of 3E. From Proposition l(ii) the face ^0)

=

^ V \ ( x , a y y = 0,

> 0

fo r; G

5.6

The Geometry of a Set of Root Data

441

dearly supports (some authors say “spans”) the hyperplane Thus every face supports a hyperplane, and it is elementary that faces are the only facettes supporting hyperplanes. _ The faces / e J, all lie in F. Indeed these are the only faces lying in f , for if X ^ F, then a: e Fj for some I c J. If also x e wFy^ for some w ^ W and j e J, then by Proposition 3, {;} = I and wFy^ = Fyy The faces lying in wF for any w are then {wF^^^\i e J}. These are called the faces of the chamber wF. The hyperplanes wH^y supported by these faces are all called the walls of the chamber. Proposition 4 Let the notation be as above, then (i) 3£ = {a: e V\{x, a ^> < 0 for only a finite number o f a ^ 2+}, (ii) 36 and 36^ are convex cones. Similar results apply for 36 Proof (i) Let 36'Jbe the set in question. If y e 3£, then y = wx for some w and X ^ F. Let a; e 2+. Then by Proposition 5.2.6, <0«=> (x,w~^a"^y <=> w~^a e 2_<=> a e 5^. Since is finite, this shows that 36 c 36'. Conversely, suppose that x e 36'. Let Sj^ = {a e 2+Kx, a ^ ) < 0}._We show that x ^ 3i by induction on card (Sjf). If Sj^ = 0 , then x ^ F (z X. If 0 , then there exists j ^ J such that ( x, aj ^ ) < 0. ByProposition 5.1.6 it is easy to see that = rj(S^ \ {aj}). By induction rjX e 36, and hence x e /^36 = 36. (ii) Let X, y e 36. For 0 < A < 1 and a g 2+, the inequality

< 0 holds only if ( x , a ^ ) < 0 or
442

The Weyl Group and Its Geometry

Proof, (i) => (ii) The proof is clear. (ii) =►(i) Consider the open interval Jjc, y[. We claim that if p, q ^]x, y[, then p q. If not, we may assume that there exists / i e H such that either (a)

p e

and

q e H~

or (b)

p ^ H

and

q e H~,

and it follows in either case that H separates x and y :

Since ]x, y [c X, it follows that ]jc, y[ is included in one equivalence class of 3e. Thus ]x, y[ c wFi

for some w ^ W ,1 (z J.

Hence [x, y] c wF^ = wFj c wF.



Proposition 6 Let ;c, y e 36. (i) There exists only a finite number jt(x, y) of hyperplanes o f H separating X and y. (ii) I fy = wx for some w e IT, then tt(x, y) < /(w) with equality ifx lies in a chamber. Proof. Recall that the elements of H are in one-to-one correspondence with the dements of X+. Since W stabilizes both 36 and H, we may assume that X e F and y = wz for some z e F and e PT. Let a X + . Then separates x and y ^(x,a'^)> 0

and

(y,a^)<0

<=><x,o:^>>0

and

< 0

<=>(x,a^)>0

and

<=>0 and

a e 5^,

Both parts (i) and (ii) now follow from the fact that card S^ = l{w).



5.6

The Geometry of a Set of Root Data

443

Proposition 7

Let x , y ^ di. Then the closed interval [x, y] lies inside the union of finitely many facettes. Proof For two points p and of 3E to lie in different facettes, they must lie in different equivalence classes. Thus there must be a hyperplane if of H that either separates p and q or passes through one of these two but not the other. With this observation in mind let us analyze the closed segment [x,y]. Let Zi,. . . , be the consecutive points at which the hyperplanes (finite in number) separating x and y cut [x, y]:

By the above observation each of the open intervals ]x, z^[, ]z^, Z2L .. •, ]z^, y[ lies in a single equivalence class. The proposition now follows. □ Proposition 8

Let jc e 36^. The set := {if e HU e if} is finite. Proof Let y e 3E®\ U (This is possible since U / / e n ^ is of the first cat^ory.) Then y x. Let B be an open ball centered "^at x whose closure B lies inside X®. The line through x and y meets the frontier of B at points p and q. Then p and q belong to but not to any if e Also if if e Hj,, then i f separates p and q, since x = |( p + ^) e if. By Proposi­ tion 6, Hj, is finite. □ Proposition 9

Let di be the Tits cone, and let F be its fundamental chamber (i)

If w and l ( Z j are such that wF^ C\ F 0 , then w Πand w fixes FI pointwise; (ii) I f w EiW fixes jc e 3E, then w pointwise fixes the facette containing x\

The Weyl Group and Its Geometry

444

(iii) W acts simply transitively on the set of chambers, and the following condition holds FR:

I fx G 3£, there exists a unique z e F such that x e Wz,

In particular F is a fundamental region for the action o f W on 3£. Proof (i) This is Proposition 3, since F = U Fj. (ii) Let jc G 3£ be such that wx = x. Let w' El W and I c J be such that X G w'Fj (this is a typical facette containing x). Then w'~^ww' fixes a point of F|, and hence all of F| because of part (i). Thus w fixes w'Fi pointwise. (iii) W is transitive on the chambers by definition. If wF = F = then vi^ G = {1} by part (i), showing that W is simply transitive on the cham­ bers. FR follows from part (i). □ Proposition 10

Let / /

G

H, then FT fl

spans, hence supports, H.

Proof The reasoning is the same as in Proposition 1.



The picture we now have of 3£ is that of a convex cone partitioned into a set of disjoint cones {wFi), the facettes, by the set of hyperplanes //^v with a^G The facettes with nonempty interiors are the chambers wF, w and the Weyl group acts so as to permute them in a simply transitive way. In the most common situation II and II ^ are linearly independent sets in V and V respectively. Suppose in addition that II spans V, Then II ^ spans V ^ , since d i mK^ = dimF. Define co,, i g J, by ( cd,, « /> = 6^ y. Then it is easy to see that F is the cone generated by the simplex 5 := (x

V\x = Lc^iOi, Ci > 0, Ec^ = 1};

G

that is, F = {R+x|x

G

5} = (x

G

Fix = Ec,o)^, c, > 0}.

Thus F is a “simplicial cone,” and hence so too are all the chambers.

5.6

The Geometry of a Set of Root Data

445

The face ties I J, are also simplicial cones (of smaller dimension), namely Fj is generated by the simplex = (x e Vjx =

= 1, >0

if

/ ^ I,

= 0 if / e l } ’

If we continue to assume that II and II ^ are linearly independent but no longer assume that II spans K, then we have to take into account the subspace

n

n

This space is pointwise fixed by W, and every facette is stable under translation by : vuFj = wFj + Consequently 3£ =

.

+ H . If we let V /H ^

be the natural mapping, then W acts uniquely on V /H IT-equivariant map: w(iJLx) = jjl( wx)

for all w

e IF , jc e

so as to make

a

V.

One may then consider the convex cone /¿(3E). It is the disjoint union of the “facettes” {w/i(Fi)}, The “chambers” are then the simplicial cones {wii(F)}. We make no further use of this in what follows If F is a minimal realization of A, then II and H ^ do consist of linearly independent elements and dim H ^ = corank A. Thus for A of finite type we can arrange for H ^ = (0) and emerge with the first picture above. However, for A affine we can never do better than dim H ^ = 1, and the second picture is appropriate. The examples at the end of this section illustrate some of the possibilities. We return to our general development. If T is a nonempty subset of V define H y := { / / e

H | y c / i } ,

:= Iw e W\wy = y

for all y e y ) ,

[ y ] := the subspace of V spanned by Y.

446

The Weyi Group and Its Geometry

Proposition 11 Let Ybe a nonempty subset o f 3£, and let K •= C\ h There exists w ^ W and I c J such that

^

^

(i) = ^ w W ^w-\ (ii) = In particular the three following groups are equal: (iii) The elements of W that fix Ypointwise. (iv) The subgroup o f W generated by all reflections r^ such that r^ fixes Y pointwise. (v) The subgroup of W generated by all reflections r^ such that Y c Proof Let yj , . . . , e y be a basis of [y]. Because 3£ is a convex cone the set {E/ = 7,^A^yjA^ > 0} is included 3£. This shows that 3£ contains a nonempty open subset of the topological subspace [Y]. Each hyperplane i f e H \ H y intersects [y] in a proper subspace. Since the number of such hyperplanes is countable (see beginning of this section), there exists x g [y]ri3£ such that X ^ H whenever / / e H \ Hy. Thus (3)

y

Let wFj be the unique facette to which x belongs. It is convenient now to translate the whole problem by \ replacing Y by w ^y, jc by iv ^jc, and K by x~^K. Then x e Fj, and hence by Proposition 9 = Wi = W'"'.

(4)

Suppose that Hy # 0 , let H e Hy, and let a e 2+ be such that H = Since X G [y], we have < x , a ' ^ > = 0. Writing a ^ = Cja/, c,. in natural form (Section 5.1) and using the fact that jc g Fj, we conclude that Cj = 0 if ; ^ I. Thus a^G (Proposition 5.2.11). Conversely, if )8^ g X f, then <x, = 0, and hence x g FT^v. By (3), FT^vG Hy. It follows that H y= Of course, if Ny = 0 , then 1 = 0 , and this last equality still holds. In particular r, pointwise fixes K for all i e I and hence by (4), IV'"' c JV^.

5.6

The Geometry of a Set of Root Data

Finally, noting that

we have c JFW =

czW ^c:W ^=

and whence

^

447

= W^. Translating back by w gives parts (i) and (ii). □

Corollary

I f r ^ W i s a reflection, then r =

for some a e 2.

Proof Let H be the hyperplane of fixed points of r. By Proposition 10, if n 3£ spans H, By Proposition 11, is generated by all the reflections r^ for which H c //^v. Thus r is a product of some reflections r^ for which H = Hi^v, By Proposition 5.2.7, is unique up to sign, and it follows at once that r = r^. □ Proposition 12

Let X e 3£°. (i) There exists an open convex set B in X® containing x and satisfying the local flniteness condition: forallH ^H .

(ii) If B
Proof (0 Let / j , . . . , /„ be closed intervals in linearly independent direc­ tions of V lying entirely in 3£® and containing x in their interiors. Each Ij lies inside the union of finitely many facettes (Proposition 7) and each of these facettes intersects Ij either in an open subinterval or in a point (since facettes are convex). Let Zy^,. . . , Zjku) points obtained in this fashion. Note that if / / e H intersects the interior of Ij at a single point p, then p= for some 1 < / < fc(;). Let /y be an open subinterval of 7y chosen so that Jj

448

The Weyl Group and Its Geometry

and Zji ^ Jj

for all 1 < / < A:(y) whenever Zy, ^ x.

The above discussion shows that for all / / e H, /f n /y ^ 0 <=>jc e //. Then the convex hull B of the set /i U • ♦• U is by construction a set satisfying LF. (ii) Let B be an open convex neighborhood of x satisfying LF. Assume that fl 5 ¥= 0 . If ¥= x, then there exists if e H separating x and wx. Indeed, if not, by Proposition 5, x and wx lie in the closure of a common_facette F'. There is no harm in assuming that F'czF. Then x,wx ^ F = Uicj^i* X and wx lie in facettes of the same type and hence x, wx e F^ for some I. Now Proposition 3 implies that x = wx, which is false. By assumption then, B and wB lie on opposite sides of H, Thus wB f] B = 0 . It follows that wx = x and hence that w e □ We now consider the case when A is of finite type in some detail. Proposition 13 Let 2) = (A , ing are equivalent: (i) (ii) (iii) (iv) (v) (vi) (vii) (viii) (ix)

• , • )) be a set o f root data over R. The follow­

The Cartan matrix A is o f finite type. There exists w ^ W with wF = —F. 0 g 3E^. 3i = V. The number o f facettes is finite. The number o f chambers is finite. W is finite. S is finite. X is a finite root system.

Proof, (i) => (ii) if A is of finite type, then 2 base n (Proposition 3.3.6). Since -1 1 ^ is another base for (check the definition in Section 3.3), there exists an element w ^ ^ W with WqU. -II ^ (Proposition 3.3.5). Now o F = {x e

> 0 for all

= {x e F|<x,vvoa;'^> > 0 for all a

II

= {x e F|< - x , a ^ > > 0 for all

n'^} = - F .

5.6

The Geometry o f a Set of Root Data

449

(ii) =* (iii) 0 lies in the interior of the convex hull of F and —F (Proposi­ tion 1), hence 0 e 36®. (iii) <=» (iv) The proof is obvious. (iii) =» (v) Since 0 e 36® and 0 ^ H for all /f e H, Proposition 7 shows that H is finite. Let C be a facette, and let x e C. For each //„vS H, a'^e X+, assign a label A^(x) g {-1-, - ,0} by

a::( x ) =

i -I[o

if ( x , 0! ^) > 0, if<x,a^xo, if = 0.

Since A^(x) is independent of the choice of x e C, we can define A^(C) = A^(x). Now facettes C and C are equal if and only if A^(C) = A^(C') for all a'^e X+. Since the number of possible labels is finite, so is the number of facettes. (v) =» (vi) Since chambers are facettes, the number of chambers is finite. (vi) => (vii) W is simply transitive on the chambers. (vii) => (viii) Since if and only if a = +/3, X is finite. (viii) => (ix) X satisfies the axioms of a finite root system (with ambient space the linear span of X in F). (ix) ^ (i) Let us show that II is a base of X in the sense of finite root systems. It will suffice to show that II consists of linearly independent elements. Let V be the linear span of X, and let (-| •) be a positive definite IF-invariant bilinear form on V (see Proposition 3.2.5). Suppose that we have a nontrivial relation E, s jC,a, = 0, c, g R. If all the c, > 0, then restricting to the set I for which c, > 0, we see that the matrix (^/y),,;^/ has a null root and hence decomposes into affine Cartan submatrices. Suppose that (^,y),ysK is one of these affine components. Then E, eK^<“ / = 0, c, g Z+. This contra­ dicts WIP. Thus we have E, ejC,o;, with mixed signs. We can now finish the proof by following the argument of Proposition 3.3.1 (part (ii) of the proof), but for this we must know that (a ,|a p < 0 for all i # ;. To see this, note that r, is an involution of V that pointwise fixes the hyperplane n V and maps a, into -a ¡. Since it is also an isometry of (-| • ), it is the reflection X ^

X ~ 2(x\a¡)/(a¡\a¡)al

Thus for all j we have 2(ay|a,)/(« ,. I«.) = A j i , and since >1 is a Cartan matrk, it follows that (ayla,) < 0, as desired. We have shown that II is a base of x! Accordingly A = ((a,^'^))a,;3en is a Cartan matrix of finite type. □ Proposition 14 Let X ^ X. Then x e implies is finite. In particular the stabilizers of any facette in 36® are finite. I f U. is finite, then x e if and only if IPF} finite.

450

The Weyl Group and Its Geometry

Proof. Suppose that x e Let B be an open ball with x e B c 3£° and satisfying LF of Proposition 12. Any chamber with x in its closure meets B, and it follows from Proposition 8 that the set of such chambers is finite. Since permutes these, and the action is faithful, is finite. Next we assume that II is finite, and prove that is finite implies X G 3£°. We can assume that x e F, for some I c J. We let II, == {a,|i e I}, n , ^ := G I}. Let A i ■= (v 4 ,y ),y G I be the submatrix of A obtained from I. Then © , : = ( ^ „ П „ П , ^ F , F ^ < • , • >) is a set of root data (see Section 5.2 for a discussion of parabolic subgroups). The Weyl group of S), is the parabolic subgroup IP,. For S), the fundamental chamber is F<*> :=
G

F| 0 for all i e I }

and its Tits cone is XO>=

(5)

U WF® M 'S » ',

Suppose that IPF) ¡g finite. Since IPF) = = IP, (Proposition 11), it follows that IP, is finite. Then by Proposition 13, ( 6)

= V.

Furthermore, since x since IP,x = X,

G

F „ we have <x, a' ' > > 0 for all « ' ' g II''\II,'^ and

<x,wa'">>0

for all w

G

IP,,

n ^ 'X n ,''.

Hence X G

C == { y e F | < y , w a ' ^ >

>

0

for all w

G

I P „ a ''G

n '^ \ n ,'^ }.

Since C is defined by finitely many inequalities, there exists an open ball B about X lying entirely in C. Let y ^ B. By (5) and (6) there exists a w g IP, with wy g F^*l Thus <wy,a''> > 0 for all a'^G H,'". Since > 0 for all a g (because y g B), we have w y g F c X. Thus y e X, and in conclusion F c X and X G X°. □

5.6

The Geometiy of a Set of Root Data

451

Proposition 15 W acts properly discontinuously on 3£^. In other words, given any pair of compact subsets U and V of 36^, {w e W\wU ClV ^ 0} is finite. Proof We may cover each of U and V with a finite number of closed balls lying in that satisfy the hyperplane condition LF of Proposition 12; that is, H 0 X ^ H, In particular, by Proposition 8 only finitely many hyperplanes of H meet each of these balls. It suffices then to prove that if U and V are closed balls and only finitely many hyperplanes of H meet U and V, then {w e W\wU f \ V 0>) is finite. Now in this case the labelling argument of Proposition 13(iii) => (v) shows that U is covered by finitely many facettes. The same goes for V, The relation wU fl V indicates the existence of facettes C, C with cnc/^0

C 'riK ^0,

wC = C ,

The same pair can occur for only finitely many w ^ W , since w'C = C and IT^ is a finite group (by Proposition 14).

w

Example 2 Let A =

^12 ‘21

be a 2 X 2 Cartan matrix. Let S) be the root data of A obtained by considering a minimal realization of A (Example 1, Section 4.2). We illus­ trate the contents of this section for such S). A of finite type: A minimal realization of A is given by R = is a finite root system (Proposition 13), and ij* = Ua^ ^ Ua2 can be identified with by means of a IT-invariant positive definite bilinear form ( I • ) (Proposition 3.2.5). Under this identification a / = 2 a ',/(a ja ,), i = 1,2. Figures 3.2 and 3.3 show drawn in the euclidean plane defined by ( I • )• The fundamental chamber F is given by F = (jc G

>0

= {x e f|*|(x|a^) > 0

/ = 1,2} i = 1,2);

452

The Weyl Group and Its Geometry

Figure 5.1. since { x , a ^ } = 2(jc|a^)/(aJa^). Thus the walls of F are the hyperplanes [ a j - ^ , and F lies on the same side of as a^. The resulting decomposi­ tion into facettes is now easy to see. The schematic view of the root system of type A 2 in Figure 5.1 shows how the PT-orbits of the facettes appear. Facettes with the same letter are in the same orbit. Figure 5.2 depicts the fundamental region C and its PF-translates for the finite root system of type ^2-

«1

Figure 5.2. 2.

A affine: There are two cases A = 5Cf>: A =

2 -2

-2 2

2

-4

-1

2

In either case in a minimal realization

we have h* = Ud* ® Rap © R«!,

5.6

The Geometry of a Set of Root Data

453

where d* can be chosen so that < d * , 0 = l,

< d * , a / > = 0.

The null and conull roots are given by 5 = «0

5 = “o

2«,,

and 5

<

+ «i'"

5

2a^ + < ,

according to the two cases. Since <5, a / > = 0, / = 0,1, we have WS = 8. Since ( d * , a ^ y = 0 = ( 8 , a ^ ) , //„V = Ud* + Similarly - n ( ‘i* - y ) + RS. Picture ]^* with the subspace Ud* + Rag as the plane of the page and R8 in the direction orthogonal to this plane. Every hyperplane contains R5: indeed R5 is the subspace H*=

n

defined in the discussion following Proposition 10. The intersections of the with the open half-space D^:=

>0}

appear like the pages of an infinite book (see Figure 5.3). The fundamental region F is an open wedge, and 3E = U We illustrate this for the case space ^*/R 5 by the mapping

= D^\JU8. Identifying Rd* -l- Rao with the quotient

ad* + ba^ + c8 ^ ad* -t- buQ. The line {x,S'^} = 1 in Rd* + Roio is stabilized by W and is met by the

The Weyl Group and Its Geometry

454

hyperplanes //^v at the points The requisite calculations are

+ k / l a ^ , k ^ Z, k odd (see Figure 5.4).

+ - a , \ = d* - I - + 1

''ll

d*

3.

- «0

+ 2^0 j = d* - - « 0 +

- 1 /2 «0

d*

d*

+ 1 /2 «0

A hyperbolic: A =

with ^ 12^21 > 4

2 All

A^2 2

+ «o

5.6

The Geometry of a Set of Root Data

455

We simply state some results and sketch the resulting Tits cone 3£ (Figure 5.5). Set a - = ^ 21» ^ /?== {Ua¡' + be a minimal realization of A, We have ij* = Rofi + Ua2, which we coordinatize by (x, y) xa^ + y a 2* The Tits cone is that part of the third quadrant bounded by the pair of lines y

—ab ± y/ab(ab — 4)

X

2a

The fundamental region is defined by the inequalities lx

ay > 0,

¿X + 2y > 0. There are infinitely many chambers that crowd in around the two boundary lines of 3£. It is more convenient in this hyperbolic situation to look at —3£ which lies in the first quadrant. Figure 5.5 illustrates the case for the matrix 2 -2

-3 2

The open region bounded by the two lines y

3 + \/3

X

is “ 3£, and the region between the lines y = x and 2y = 3x is —F, The figure also shows some of the real imaginary roots. The integers associated with these are the root multiplicities. Up to this point in this section we have looked at sets of roots data over R. This has allowed us to develop a “chamber geometry” by means of which important information has been gained. For a set of root data over K 9^= [R many of the results in this section would be meaningless (e.g., the Tits cone

The Weyl Group and Its Geometry

456

---3 +^/3 a

y

cannot be defined over fields that are not ordered). Yet Section 5.5 suggests that some statements proved only for U should hold for arbitrary fields. We summarize some of the most important of these in Theorem 16 Let 2) = • » be a set o f root data over IK such that dim^(VX= dim ^iV ^)) is finite, (i) Let Q q == finite number o f a

and let S ■= {x ^ < 0 for only a For a subset Y o S we have

IV^ ■= [w e W\wfixes Ypointwise} = ( r J ( Y , a ' ^ ) = (0)>. I f x e 5, there is a unique z e F fl 5 with x e Wz.

5.7

Subroot Systems

457

(ii) The only reflections in V which belong to W are those o f the form r^ with a e 2. (iii) The following are equivalent: (a) A is a Cartan matrix o f finite type, (b) W is finite, (c) X is finite, (d) X is a finite root system. Proof, (See Section 5.5.) We first construct the rational set of root data and then its realization 3 q , Then 3 and are isomorphic. Now to we can apply the theory developed in this section. Then parts (i) and (iii) follow. For part (ii) we use Proposition 5.5.2. □ 5.7 SUBROOT SYSTEMS h&t 3 = (A , n , n F, F ^, < * , * ) ) be a set of root data over IK. In this section we assume that dimj^F = dimj^F n is finite. We maintain all previous notation and terminology for 3 , Recall that a nonempty subset il of X is called a subroot system if for all The main result of this section is: Theorem 1 Let 3 = {A, n , n F, F < • , • » be a set o f root data over IK. Let X be the root system of 3 , and let Ci czX be a subroot system. Then there exist a Cartan matrix B and a subset a o f X+ such that if we define H ^ = {a e H}, then (B, F, F )) Is a set o f root data with root system Cl,

S, H

j*

The proof of this theorem will be given later as a consequence of a series of preliminary results. Because of the results in Section 5.5 it will suffice to establish Theorem 1 in the case when IK = R. We will henceforth assume that this is the case. Define an equivalence relation ^ on F as in Section 5.6, but now using the set of hyperplanes e il}. Since c H, we have ^

^

H^y

for all x , y ^ V ,

The set of chambers relative to ii is defined as follows: := {C|C is an equivalence class of n and there exists a nonempty open subset U of V such that J7 c C fl *}. Note: If F' is a chamber of 3 , then F' cz C for some equivalence class C of ^ n on F. Clearly C is a chamber relative to fi (Proposition 5.5.1). In particular, 0,

The Weyl Group and Its Geometry

458

A face of a relative chamber C is an equivalence class of ^ on K that lies in C and supports a hyperplane In this case we also say that is a wall of C. Note that if O = S, then all these concepts coincide with those defined before. The first aim is to prove that walls exist. Let := . Since JV^ stabilizes and we see that ¡V^ stabilizes Given jc, y e K, we let 3^) = card{// e

IH separates x and y}.

Lemma 2 Let C and C be elements of The cardinal #^{x, y) with x finite and independent of the choice of x e C and y g C'.

C, y G

C\ is

Proof Fix a: G C, and let and y2 belong to C . Let H g If H separates x and y^, then a: and y^ lie on opposite sides of H. Therefore, if H does not separate x and y2, we conclude that either y^ and y2 lie in opposite open half spaces defined by / / or y2 e H. In either case, this is a contradiction, since y^ n3^2- This shows that the set of hyperplanes in separating x and y is independent of the choice of y ^ C and, mutatis mutandis^ for a: g C. Finiteness follows from Proposition 5.6.5 by taking a : G C n X and y g C' fl In the sequel we will denote this finite number by

C'),

Lemma 3

y

U

Let C e and let x ^ C f\?i. Let ^ 3£ \ // e Then there exists an open ball B about y in x such that # q( a:, y) = #^{x, z) for all z ^ B. Proof Take B to be an open ball about y in S satisfying LF of Proposition 5.6.12. □ Recall that

i f jc , y

g

K,

a:

=7^ y ,

the (open) ray from x through

y is

defined

by y) — [x + t{y - x)\t e R>o}.

Lemma 4 Let C El Let_x g C fl 3£, and assume that y e 3£ \ C. I f B is any open ball about y in 3£ \ C, then the cone of rays ^ ( x ) = \J ¡^^^R(x,b) cuts at least one face of C in an open subset of that face.

5.7

459

Subroot Systems

Proof. Let Z c 5 be a set of representatives of the rays of ^ ( x ) ; that is, G 5 => 3z G Z such that R ( x , b ) = R ( x , z ) , Zi,Z2 ^ Z;

¥=Z2

R{x, Zj) =5^ R{x, Z2).

If z G Z, the closed interval [x, z] is covered by finitely many classe^of ^ (Proposition 5.6.7), one of which is C (since x g C). Clearly C fl [jc, z] = [jc, c(z)] for some c ( z ) g [ ; c , z]. Moreover c(z) g X, and there exists a ^ ( z ) g such that c(z) g H [To establish this last assertion, note that if c(z) is off every hyperplane of H^, we can consider a ball as in Proposition 5.6.12 to find points in C further away from x than c(z)]. For each o:^ g let Z ( a ^ ) •= [c(z)|z g Z and c(z) g H^ v). Now ^(x), which is open, is the countable union = U «Ve^v (.^ (jc) n [affine span of

a:

and Z ( a ^ ) ]

of subsets of affine subspaces. Thus by Baire category Z(a generates as an affine space for some a ^ g Let c(zf),.. . , c(z„) g Z(a be an affine basis of If 5 denotes the open sirnplex with the c(z,) as vertices, then S is open in H^v, S c H^v fl 3£ and 5 c C. □ Corollary

Walls in exist. Moreover, if C and C are distinct chambers of there exists a wall separating C and C .

then

Proof Let C G (recall that we know that ^ 0). To show that walls exist, it will suffice by Lemma 4 to show that S \ C ^ 0 . Let x g C fl 3£, and let a G il. Then g 3£, but r^x ^ C. Indeed, if x g if^v, we can choose a ball B about rj^x) such that B c H~w. Finally, if C ¥= C and x g C, y ^ C , then x Because neither x nor y lie in a hyperplane of at least one hyperplane of separates x and y. By Lemma 2 this hyperplane separates C and C . □

The Weyl Group and Its Geometry

460

Choose C G to be the unique relative chamber containing F (see Section 5.6). According to the last corollary C has at least one wall. Let H be defined as follows: a '= [a

is a wall of C and

Note that by the definition of F, a

> 0 for all x e C}. Let

:= < r ja e H>.

Proposition 5

Let the notation be as above. Then (i) W-s acts transitively^ on Cq , (ii) JV^B = n and ft (iii) « a, )8 ^ ^ e 2 is a Cartan matrix. Proof, (i) Let C' be a chamber relative to ft. We reason by induction on #(C, C ) (see Lemma 2) to show that C = wC for some w e W>sIf #(C, C') = 0 then C = C' by the last corollary. Assume #(C, C') = > 0. Let U be an open subset of V such that U c C' fl 4. Fix jc e C fl By Lemma 4 we can find y ^ U such that the open ray R(x, y) meets a face of C. Let H^v, Of e H, be the wall of such a face. Let [x^,. . . , jc„} e]jc, y[ be the distinct points at which a hyperplane of cuts [x, y]. We order these points starting from x as

Let z e]jci, X2L where X2 •= y if n = 1. Then z e r^C (this is because is the unique hyperplane of going through x^, since x^ lies in a face). Since [z,y], hence [r^z,r^y] is cut by N — 1 hyperplanes, we have #(C, r^C) = N - 1. By induction wr^C = C for some w e (ii) Let )8 e ft. We claim that we can choose x e fl S such that X ^ H whenever H e From Proposition 5.6.10 we can find a relatively open subset 5 of with 5 c S . Then 5 ¥= U H since ft is countable. Our claim then follows. ^Once we have established Theorem 1, it will follow from Proposition 5.6.9(iii) that the action of on is simply transitive.

5.7

461

Subroot Systems

Let X be chosen as above, and consider an open ball B about x satisfying LF (see Proposition 5.6.12).

Let 5"^ be one of the open semiballs defined by Now, by the choice of x and B, B^< zC for some C' e From this we conclude that is a wall of a relative chamber C'. By part (i) we can write C' = w” ^C for some w e PFc. Then wH^v= is a wall of C. Since it follows by definition that ±w)3 e H. We conclude that W-sB = ft. (iii) Let )8 e H. We claim that is the unique hyperplane of separating C and r^C. Suppose that separates these two relative chambers. Then (1)

<.^,7''> > 0, <x,y'^> -

<0

for all x e C.

(We may have to replace y by - y if necessary.) Choose X inside an open subset of V lying in C fl X. Then we can find an open ball B about r^x with B <^r^C, The interior of the cone of rays from x to this ball B cuts in an open subset S of Choose z e 5 such that z^ If we now let x approach z in (1), we reach a contradiction. This establishes our claim. In particular, if a e H, a then does not separate C and r^C. Thus for all jc e C. (2)

> 0,

and

If we now let x approach a point of <j8, a ^ > < 0, as desired.

> 0. not in

we conclude that □

This last proposition contains most of the information needed to establish Theorem 1. However, we still need a result about lattices to eventually show that RD4 holds. Lemma 6 o

Let L be a lattice in R" and C a convex cone. Suppose that the interior C Then C contains a basis o f L.

0.

Proof Since C contains balls of arbitrary large diameter (being a cone), we have L n C 0 . Because C is a cone, it follows that there exists e L fl C v ^ of L. For N such that is primitive. Extend to a basis sufficiently large, Nv^ + v^ ^ C for all 2 < i < n, and it is clear that {^1, Nvi + i;2> • • • ? is a basis of L lying inside C. □

462

The Weyl Group and Its Geometry

Lemma 7 Let L be a lattice in IR", and let Cbe a closed cone in IR". Suppose that the dual cone has nonempty interior C^, Then there exists a basis .,., of L such that the real cone generated by this basis contains C. Remark 1 The hypothesis that Cn - C = (0), i.e., C is pointed.

has a nonempty interior is true [Br] if

Proof. Let L* be the Z-dual of L. Then the dual cone to C is C^-= {jc e IR"|jc.i; > 0 for all u ^ C }. By assumption 0 . By the previous lemma there exists a basis , . . . , ¿;*} of L* contained in C^. Let T be the real cone generated by this basis: r — L"=;lR>oi^f5 and let be its dual. Then r^ = E ¿=1 where u^} is the basis dual to {i;*,..., u*}. Now T c C‘^=> C'^'^= C, while {i;f, . . . , y*} is a basis of L* => . . . , i;„} is a basis of L. □

Proof of Theorem 1. To the subroot system ft of S we have attached the six-tuple (B, H, H K, F * ))? which has been shown in Proposition 5 to satisfy RD1-RD3 and is known to have ft as its root system. All that remains to be shown is that RD4 holds. Lets 7 i , . . . , y/ be as in RD4 (for 3J) so that / / < 2 = 0 Zy^ and n c 0 I^y.. i= l

i= l

Let C be the real closed cone of V generated by {y^,. . . , y/}. Set <2' =

Za

(the root lattice of ft),

and let C' — V' fl C, where V' •= U Note that C' is a pointed cone [i.e., C' n ( - C ' ) = (0)], of F ' and that <2' is a lattice of F'. By Lemma 7, Q' contains a basis [y\,. . . , y^} that generates a real cone containing C'. Finally Hc C, and hence S c C'. Thus

Hc ^ L R^or;|ne zy;I = e Ny^. Similar considerations apply to H

5.7

Subroot Systems

463

Corollary 1 Let 2) = » be a set o f root data over IK. Let II = {aj\j e J} and let I c. J be a nonempty subset. Let IIj, 2 i, etc., be defined as in Section 5.2. Then (i) S i is a subroot system of 2 (ii) 2 ^ is a set of root data with root system Sp Proof (0 Let a = ua^, f3 = vaj, be elements of 2 i where a^,aj g Ui,u, V G W^. Then r^p = ur^u~^vaj g W P^i II i = Sj, proving (i). (ii) We can assume that K = R. According to the theorem there exists a subset H of 2i+ which serves to construct root data for Sj. Furthermore, following the proof of the theorem, H is constructed from the walls of the unique relative chamber C (relative to -that contains the fundamental chamber F of 2 . We will be done if we show that H = Hi. If a G I I I ^hen / / ^ v is a wall of F. This means that some open subset U of //^v that supports lies in some equivalence class of of F. Then U serves to show that / / ^ v is a wall of C. Also if jc g F c C, then (x,a"^) > 0 and so, by definition, a g H. Conversely let a g H c Si+. Let x ^ F (z C. Then x and r^x are sepa­ rated (relative to Si) only by the wall On the other hand the line segment [x,r^x] = [x,x — ( x , a ^ ) a ] passes through some wall of F, say I f ' ^ J \ I then ia, oi^y < 0 (since a g 2i+) and then both {x, > 0 and ( x - ( x , a " ^ } a , a y y > 0, a contradiction. Thus i g I and is a wall of C by what we have already shown. It follows that H^v= FT^y and hence a ^ = a / (note, a^G 2i^+). This proves that H c III and hence that 3 = Hi as required. □ Corollary 2 {See also [De 2], [Ku 2]) Let 5 c 2, and let '= {r^\a g 5). Then Weyl group o f a set o f root data. In particular is a Coxeter group.

is the

Proof. Let fl := W^S. Then ft is a subroot system of 2 with Weyl group W^. □ Corollary 3 {See also [FTT]) Let A g F

and let

2^ : = { a G 2 | < a , A > G Z } . Then 2^ is the set o f roots o f a set o f root data. Remark 2 We do not know under which conditions 2 ^ admits a finite base.

464

The Weyl Group and Its Geometry

5.8

IMAGINARY ROOTS

Let 2 be a root system determined by root data (^,11,11^, < • , • » . If e ¡2, a e X , and r^cp =


if w > 0, if w < 0.

A subset of (2 is said to have the root string property relative to X if RSPl: X c and RSP2: whenever


and a

e

X, then [.

There is a unique minimal subset A = A (^ ) of V with RSP relative to X. In fact, if we define inductively A o-2, A„

— {P\P

^

[
e

X, where cp e A„_ i },

then Aq c Ai c ... and A == U A„ has the root string property and is minimal. Henceforth A denotes this minimal set with RSP relative to X. We call A the root string closure of X. We denote A \ X by ''"X. Proposition 1

A is W-invariant. Proof. We show that A„ is IT-invariant by induction on n. This is clear for A q . For A„, let p E [(p,T^(p], where


^w
= [w
e

A„_ i ). It follows that

=



Let ^ be a set of root data as above, and let 3 be its universal covering. We maintain the notation of Proposition 5.1.1. In particular il/:Q ^ Q is iht covering map.

5.8

465

Imaginary Roots

Proposition 2 Let A and A be the root string closures o f % and S, and let {A„} and {A„} be the sets as above that define A and A, respectively. Then fK =

for all n

i/rA = A.

Proof = S = Aq. Suppose that = ^ n - v For A Q, A ^ Q with i/rA = A and for a g 2, a e S with <pa = a, we have A

A A + sa

X + sd

and i/f([A, r¿A]) = [A, r^A]. Thus, if /3 ^ A„, p G [A, r^A] for some A e A„_i, {¡/(p) G [A, r^A] c A„. Conversely, if j8 e A^, then p g A G A^_i, « ^ 2, choosing preimages A e A„_i, a g 2, [A, r^A] with il/P = p. This shows that (^A„ = A„ for all that i/rA = A. Remark 1 The map ijj'.A the Cartan matrix

B' :=

a e 2, and ^ = [A, r^A] for some we find that p g « g N and hence □

A need not be injective. For example, consider

2 -2 -1 4 -3 4

-2 2 -2 -1 4

-1 4 -2 2 -2

-3 4 -1 4 -2 2

which, as we saw in Example 5.1.1 is of row rank 3. With the notation of Example 5.2 the set T = {p^, p^, P2, P^) provides us with root data = {B', r, r , V , V ^ , ( • I • » . Call the resulting root system 2', and observe that ^0 - 3/3i + 3 p 2 - p 3 = 0. ^ Let with root system 2', be the universal covering of W , and let A and A be the root closures of 2' and 2'. We know that 2' -> 2' is injective. ..iff ^ « However, A A is not injective. Indeed y •= Pi P2 Pa con­ nected support and satisfies <7, p ^ ) < 0, / = 1, .. ., 4. Now this implies that y G A, as we will see in Theorem 6 below. For the same reason 33f ± n(pQ - 3pi + 302 — P 3 ) ^ A for \n\ < 10 and all 21 of these roots have the same image in A.

466

The Weyl Group and Its Geometry

The next proposition shows that imaginary roots for abstract root data are as expected in the Kac-Moody case: Proposition 3

If X A for some root system A o f a Kac-Moody Lie algebra, then the root string closure of 1, is A, Proof Let denote the root string closure of 2. We already know that A d '^^A and that A has RSP. Thus c A. We show that A ^ \ ^ = 0. Similarly A _\ O = 0 . If A+\ ^ 0 , choose e A+\ of minimal height. Note that ht > 1. Then by Proposition 4.14 either 1. there exists a e n such that 0 < ht < ht in which case r^p e so also e < 0 and for at least one a e II we have P - a ^ A^. In this case - a e <&, and since (p — a , a ^ ) < -2 , P ^ [ p - a,r^(p - a)] c <|). □ Corollary

In the notation o f Proposition 2,

”2 and ( / r - i r 2 ) n A = ' ' ”2 .

Proof We can interpret 2 as the real roots of a Kac-Moody algebra and hence view ^"*2 as its imaginary roots. Suppose that y e " ”2 and y — ij/iy) e 2. Using W, we can suppose that y = e II. Writing y = all Cj of the same sign, we have y = 2cy«y = which contradicts WIP. Conversely, let y e'"*2. If = y and y e 2, then y e 2, which contradicts ^"*2 = A \ 2. □ In the remainder of this section we study some properties of imaginary roots. We will do this only in the context of Kac-Moody Lie algebras. Let A = be a Cartan matrix, and let R = (1^,11,11^) be a realization of A, We let Q = A, R) be the corresponding Kac-Moody algebra over IK. This gives rise to the set of root data whose root system 2 is the set of real roots '^^A of g and whose root string closure A is the set of all roots of g. We will maintain all the standard notation for 3 , Given a = 2cyo:y e Q, the support of a, supp(a), is defined by supp(a)

:={; eJlcy #o}.

Clearly supp(a) is a finite set. The set of nodes of the Coxeter-Dynkin diagram T that is indexed by supp(a), together with all the edges of T that join the nodes of supp(a), form a subdiagram T(a) of T. The support of a is

5.8

Imaginary Roots

467

connected if r ( a ) is connected (as a graph); (see Section 3.4). Alternatively this means that for all i, j e supp(a) there exists a set i = = j of elements in J such that for a\\ k = 1 , n, ^ 0. The first result is completely elementary but very useful: Proposition 4 If a ^

then suppia) is connected.

Proof We can assume that a e A+. Then by Proposition 4.1.1, g" is spanned by elements of the form [e^^,. . . , e^^], where + ••• = a. If supp(o:) were not connected, then for such an expression for a there would be a maximum p < k, for which supp(a^ + • • • +«/^) is not connected. Then [e,y. .. , e,.J = ad , e,J) = 0 (or ad = 0 if p = k - 1), since e, ] = 0 for all r > p (Proposition 4.1.8). □ Since it is awkward to always distinguish between the nodes of T and the indices by which we label them, we usually use them interchangeably. Our definition of the connectivity of supp(a) is an example. Similarly we can speak of supp(o;) being of finite type, the connected components of supp(a), and so on. Let [a e Q qKo:,

> 0 for all i e j},

[a e Q q K«, a ^ } > 0 for all i e j | . If our base field is R and J is finite, then the Tits cone 3£ (See Section 5.6).

is the fundamental chamber of

Proposition 5 Let a

Then

(0 Wa (ii) Wa n ( — is a single point {p} and ¡3 is the {unique) element of minimum height in Wa. Proof, (i) was proved in Proposition 4.1.5(iv). Let p e Wa be chosen of minimal height (in view of part (i) such elements exist). Then ht(r^)3) = ht(P - <)S,a/>a,) = ht()8) - <)8,a:,^> > ht()3) for all i e J, and hence < - /3, a ^ ) > 0 for all i. Thus e As for the ui^ueness assume j3 and j8', both in A, are such that j8, G WaC{{ - ^ ) - Then this situation arises inside 3 i for some finite subset I of J. Looking at the real version of we obtain )3 = from Theorem 5.6.16. □

The Weyl Group and Its Geometry

468

Define

^conn _

^ R j s u p p ( a ) is connected}.

By Propositions 4 and 5 the unique point of minimum height in each orbit Wa, a lies in Thus +c Our main result reverses this inclusion. Theorem 6 [Ka4] Let A be the root system o f a Kac-Moody algebra. Then ''”A^_= We prepare for the proof of this by a number of results of independent interest. Suppose that A is indecomposable (hence J is connected). Let a e (2^, and write a = Then for j e J, (a, a / > = 'Lx^A¿J, Sup­ pose next that a e 0 ^ fl so that (1)

Ex,y4, > 0

for all ; e J.

Then supp(a) = J, for otherwise we can find a e J \ supp(a) with ( a , a k ) < 0. In particular card J < oo. Using Proposition 3.6.5 (applied to A^, which is of the same type as A) we conclude that either A is of finite type and at least one inequality in (1) is strict or A is affine, an ^ all the inequalities in (1) are equalities. In the same way if a e C)(— = R+, then ( 2)

E XiAij < 0

for all j e J.

If J is finite then either A is indefinite and at least one inequality in (2) is strict or A is affine, and all the inequalities in (2) are equalities. If J is infinite then letting K — supp(x) we see that (^z7)/,yeKis indefinite or affine and then A itself is neither finite nor affine. Proposition 7 Suppose that A is indecomposable. (i) I f A is of finite type, then R ^= 0 . In particular ^"*A = {0}. (ii) I f a ^ Q+ C i^cin d (a , a / > ^ 0 for at least one i e J, then A is of finite type. □ We will need the following result about root strings. We prove here the minimum that we can get away with. There is a more elaborate discussion of these facts in Section 6.2.

5.8

Imaginary Roots

469

Lemma 8 Let jS e A, and let a

If

< 0, then ^ + a is a root.

Proof This proof follows from Proposition 3.



Proposition 9 Suppose that j8 ^ A+ and for all i g J, /3 +

^ A+. Then

(0 iSe^^A, (ii) supp(p) is of finite type and is a connected component o f the CoxeterDynkin diagram T of A. Proof Let K denote the connected component of F containing supp()8), and let B := (^/y)/,yeK- Note that B is indecomposable, A(^) = AflEyeK^«;? and j8 e A^_(^) (see Remark 4.3.4). Let be a Kac-Moody algebra based on some minimal realization of B. Then, using Proposition 4.3.7, the assump­ tion )8 + ^ A for all i e K shows that « == H Q b ) ■9 | = U ( 9 b _ ) • U ( ^ ) ■ U ( 9 g ^ ) • g g c

9 |E =(2+U{0)

(• denotes the adjoint action). Since a is an ideal of uDDg^D E«eA(B)+9s Proposition 4.3.9. Thus ^+(B), hence A(B), is finite showing that B is of finite type (Proposition 5.6.13). If supp(/3) K, then we can find j e K\ su pp( j8) with <)8, a /> < 0. Then )3 H- ay e A by Lemma 8, contrary to hypothesis. Thus part (ii) is proved. Since B is of finite type. Proposition 3.6.5 shows that for at least one 0. Repeating this argument, if necessary, on rj that there is 2lw ^ W with wp e A_. Then by Proposition 5(i), e'^^A. □ Proof o f Theorem 6. It suffices to show that c"'”A+. If A is of finite type, then R+= 0 (Proposition 7), and there is nothing to prove. Assume that A is not of finite type. Let a e Choose )8 e A+ of maximum height subject to a e 0 ^ U{0}. We assume by way of contradiction that a - jS e (2+. Write a = "Lm^ai i e J, /3 = Ilk ¿aI By assumption m^ >

i ^ J.

for all i. We proceed by steps.

1. supp(a) = supp(j8): Otherwise we can find an i e supp(a) \ supp()8) with i joined by an edge of F to supp(j8). Then <j8, a,'^) < 0, so, by Lemma 8, /3 + a, ^ A+, contradicting the choice of j3. Define E := {/ e J|m^ = A :J .

The Weyl Group and Its Geometry

470

2. 0 ¥=E J: By assumption E ¥= J, Since => p ^ A+, Proposition 9 shows that if E = 0 , then supp(j8) is a connected component of finite type in F. But then a e R ^(B ) = 0 , where B is the submatrix of A defined by supp()8) (= suppCo:)). Thus E ^ 0 . Let f/ be a connected component of supp(a) \ E supp(a) has the schematic form

E

U'

E

U

E

Define i^U For i ^ U, (p , a ^ y > 0 by Lemma 8 and (p', a /> < 0 (since p' has zero coefficients on U), and hence ) > 0.

(3)

Also there is at least one i e U for which the inequality in (3) is strict. Indeed supp(a) is connected, and some i e U must be joined by an edge to some vertex of su p p (a)\i7 . Then (p',a^^y < 0 and ( P u , a n > 0 . We have then, by Proposition 7(ii) applied to the submatrix of A corresponding to i/, 3. U is o f finite type: Set i^U 4. < 0 for all i e U: For i ^ U we have = (a P , a ^y , since i7 is a connected component of s u p p (a )\^ . Since a ^ R ^ , ( a , a ^ y < 0. We already have (p, a / ) > 0. Thus (a', a ^ y < 0. Since U is of finite type and a' is a positive integral combination of the a,, i G U, step 4 is impossible by Proposition 7(i) [applied to (A^j)^ j^ц], This finally proves that a e A+. However, also a e => 2a e => 2a e A+. Thus a and so a e"'”A+. □ Corollary, (i) a e^""A => Qa n i2 (ii) For a G A \ {0}, a e'^^A <=> Za fl A = {a, 0, —a). Proof (0 We may assume that a Then a = wp for some p e R^f' If q ^ Q+ with qa e Q_^, then qP e R conn + c A+, and hence qa = w(qp) Also - q a G^'”A_. (ii) Use Proposition 4.1.5(i) and part (i). □

5.8

Imaginary Roots

471

Proposition 10

Let A be indecomposable, and suppose that J is finite. (i) A is o f finite type = {0}. (ii) A is o f affine type = Z8 where 8 is the null root o f A. (iii) A is indefinite <=> there exists a e^"*A+ for which supp(a) = J and {a, a ^ ) < 0 for all i e J. Proof Since "”A^_= it suffices to examine 3.6.5 (actually applied to A ^) to conclude that

We use Proposition

A not of finite type <=> # 0 <=>"'”A ^ {0}. A is indefinite <=> there exists a e R^^^^ with supp(a) = J and {a, a y ) < 0 for all i e J. In the affine case R^^^^ can only contain null roots (otherwise, we are in the indefinite case). By Proposition 3.5.1 there is a unique ray of null roots. Thus j^conn ^ z^8 , where 8 is defined as in Proposition 3.5.1. Since W8 = 5, '■'”A+= Z+5, whence ^'"A = Z^. □ Corollary

Suppose that A is a Cartan matrix and that J is countable. Then the following are equivalent: (i) ^'”A = {0}. (ii) Each of the connected components o f the Coxeter-Dynkin diagram r(y4) is o f finite type or lies in the list . . . O — O — O — O — O - -A „ 0 — 0 — 0- O <= O — O • • • C„ O => O — O • • • 0

^A ^

1

O — O — O ••• O Proof Any root has connected finite support. It follows that ^'"A = {0} if and only if every subgraph of r(yf) defined by a finite subset of the nodes of r ( ^ ) is of finite type. In particular, (ii) => (i). Conversely, if ^"*A = {0} and if there are connected components of T (^ ) with infinitely many nodes, then there are infinite sequences of nested connected subgraphs of finite type, each one containing one more node than its successor. But only the finite Coxeter-Dynkin diagrams of types A, B, C, D admit such nesting, and then only in the ways shown. □

472

The Weyl Group and Its Geometry

5.9

CONJUGACY OF BASES

In this section we prove that for indecomposable root systems, bases are conjugate by W augmented by {± 1}. We assume throughout that dim F < oo, but we do not assume that the basis are finite. The proof uses imaginary roots as a key ingredient. Let { A , n , n \ V , V \ { • ,• » be root data with root system S. A subset B of 2 is a base of 2 if with B= we have that

is a set of root data with corresponding root system equal to S. Thus with the notation of the definition we have 5 is a Cartan matrix; 2 = IFsH, where IT5 — ; when the base field is U, V admits a fundamental chamber C relative to H and C® ¥= 0 ; and n is a base of 2. It is also clear that n ^ and H ^ are bases of 2 where 2 ^ is viewed as the set of roots of the dual set of root data 3 ^ (see Section 5.1). Example 1 For w g IT, ( ^ , w n , w n ^ , F , F ^ , < • , • >) is a set of root data (we have to replace the {%},

of RD4 by {w%}.

Similarly -^ := (^ ,-n ,-n ^ F ,K \< -,-> ) is a set of root data. Thus —wH and wU are bases for all w ^ W. Let 2 be the root system associated with root data 3 . A subset 5 c 2 is decomposable if

5.9

Conjugacy of Bases

473

and for all e 5^, 72 ^ ^ 2^ (7 ^7 2 ^ = 0 (<=> {72,71 ) = 0 by Proposition 5.2.8G)). Otherwise, 5 is indecomposable. Let ^ = U , n , n \ F , F \ < be a base of 2. Proposition 1 n indecomposable

» be a set of root data for 2, and let H

2 indecomposable <=> Eindecomposable.

Proof. Suppose first that H decomposes into H i U S 2, where { a , ^ ^ ) = 0 for all a e Hi and e H2. Then with the obvious notation we have W= the elements of and commute, fixes H2 pointwise and 1^22 pointwise. Thus

X = »^h(H) = »^'h.(Hi )UW^3,(H2) is a nontrivial decomposition of 2. Conversely, if 2 decomposes as 2 i U 22, then set Hi == H H 2„ i = 1,2. If H2 = 0 , then < 2 , 2 ^ ) = (W-s(BiX 2 ^ ) = (0), which is impossible (a e 22 { a , a ^ y # 0). Since n is a base, the result applies equally well for H. □ Theorem 2 Let ^ be root data as above, and let 2 be its root system. Assume 2 is indecomposable. I f and are two bases o f 2, then there exists an isomorphism r o f onto 3's' (see Section 5.5) such that t H = H'. Moreover T can be taken so that it is induced by w or —w for some w belonging to the Weyl group of 2^. Before proving this we indicate two important consequences.

H H'

Corollary 1 The Cartan matrices o f any two bases o f an indecomposable root system 2 are equal (up to re-indexing the rows /columns). In particular the Cartan matrix is an invariant of X. □ Let 2 be the root system of the root data 3 . By an automorphism of the root system 2 we mean a pair (a, cr e GLiQu^) x GLiQ^^) satisfying AUTl: 0-2 = 2, cr ^ 2 ^ = 2 \ AUT2: (aa = for all a e 2, AUT3: { x , y ) = > for all x

y

The group of all automorphisms of 2 is denoted by Aut(2). If cr e Aut(2), then it is immediate that

474

The Weyl Group and Its Geometry

is a set of root data and a determines a morphism of 3 into Clearly —\ y and each w determine automorphisms of S, so we can identify { —\y} and W with subgroups of Aut(2). Also A u t(^ ) determines automor­ phisms of S, but these are very special since by definition they must stabilize n and n Such automorphisms are usually called diagram automorphisms, since they clearly correspond to the automorphisms of the Coxeter-Dynkin diagram of A. Corollary 2 Let S be the root system of the set of root data 3 . Then (i) W < A u tO .\ W n A u t { 3 ) = {!}, (ii) Aut{X) = W y \A u t{ 3 ) if 2 is finite, (iii) Autfl,) = {±1} X W X A u t ( 3 ) if 2 is infinite. Proof of Theorem 2. Using the results of Section 5.5, we can assume that our base field is R. Let F and C be the fundamental chambers for II and H. It suffices to show that WC n(±i ^) ^ 0 , for in that case, seeing that both wC and F (or —F) are equivalence classes for wC = ± F for some w ^ W . The walls then being identical, ± w a = II. If A is of finite (resp. affine) type, then the interior 3£(II)® of the Tits cone is V (resp. an open half space of V). In either case 3£(n)^nC # 0 or 3 e( n) ^ n( -C ) ¥= 0 , and hence WF n ( ± C ) ^ 0 . We can suppose then that A, and similarly the Cartan matrix B of 3>^, is of indefinite type. By the last proposition, A and B are indecomposable. Introduce a set in 1-1 correspondence with H, and write H = {oLi\i ^ J h}Let 3 ' and 3 be sets of universal root data for 3-^ and 3 with correspond­ ing root lattices Q and Q. Then using the obvious notation there are linear maps il/', {¡z for which we have the following picture:

Q'u

«A'



Qu

Qu

n

n

t'

2

‘■'"A'

‘■'"A



t ‘"■a

5.9

Coiyugacy of Bases

475

Note that the surjectivity of and ^'"A ^"'"A is by the Corollary to Proposition 5.8.3. Choose I c Jg with the following properties: I is finite and is indecomposable. B y is indefinite. El == {«¿1/ e 1} spans (although and may be infinite dimen­ sional, is finite dimensional). To see that an I exists in the case that

is infinite, choose I such that

{«¿}, ei spans (2r, I is connected (i.e., Bj is indecomposable), card I > dim Q r + 2. Then B y can be neither of affine or finite type, for in that case B y would have dimension either (/ + 1) X (/ + 1) or / X /, where / = dim Since B y is indecomposable and indefinite, there is by Proposition 5.8.10 an imaginary root y' e'"*A'+ (positive relative to H) such that supp(y') = I, (y',a'/y < 0

for all ; e I.

Let =• y e^'^A, and choose y e"'”A with il/(y) = TNow by the construction of f', <0

forall; e J s ,

< 0

forall; G J s,

and hence

with strict inequality on I. However, we claim that <7, a /> < 0

for all j e J^.

For suppose that = 0 for some ; ( e Jg \ I). Write y ' = 'Lciá'i, /el Then

r =E /el

C,. > 0 .

The Weyl Group and Its Geometry

476

and 0 = =

=> (ai, a / ) = 0

for all i e I.

¿el

But aj lies in the span of Hi, so 2 = (aj, a / > = 0. This contradiction shows that —y e C. Since no hyperplane meets C,
( 1)

^ 0

for all a e 2.

Now y (relative to fl). Suppose that y that htn(wy) is minimal, so <wy, <5^> < 0

for all ¿ e f t .

<)vy, a^> < 0

for all a e n ,

(wy, a ^ ) < 0

for all a e n

Choose w ^ W so

Thus

and hence

because of (1), and hence —wy e F. Thus -w y e Ff]y^C. If y we conclude similarly that for some w ^ W, wy e F n —wC. This is what we wanted to prove. □ For Corollary 2 we note that there is no w e IF with wF = —F (in the nonfinite case), since then w2 += 2_, contradicting the finiteness of the length function l(w). Remark 1 Maxwell’s Demon (Example 5.1) shows that Aut(H) can be infinite. More precisely one can show that for the Demon, Aut(H) A u t( S ) /± W is infinite dihedral. EXERCISES 5.1

Let be a set of root data and 2 its set of real roots. For each finite subset 5 of 2 recall <5> = and <0> = 0. A finite subset 5 of 2+ is called perfect if there exists unique distinct ..., such that <5> = jSj + • • • Show that the following are equivalent: (a) S is perfect. (b) S = for some w ^ W.

477

Exercises

5.2 Let 2) = ( ^ , • » be a set of root data. Assume that A is an I X I matrix. Let S be its root system and W its Weyl group. An element c e WKis called a Coxeter transformation if there exists an ordered base B = ..., of 2 such that Cr

"/3/*

Assume that the Coxeter-Dynkin diagram of ^4 is a forest. (a) Show that all Coxeter transformations are conjugate (see Exercise 3.10). (b) Assume W is finite. The common order of all Coxeter transfor­ mations is called the Coxeter number of W and is denoted by h. Verify that h is as follows: (W of type *, ft = - X A i J + 1), {Bi, 2 l \ (Q , 2/), (D,, 2(/ - D), (Eg, 30), (E^, 18), (E^, 12), (E4,12), (G2,6). (c) Show by direct calculation that for all finite indecomposable reduced root systems |A| = /z/ (an instructive noncomputational proof can be found in [Bo3]). be a root system of 5.3 Let A := {+ (e^ —ej)\l < / < ; < / + 1} c type AI (see Sections 3.1 and 3.2). Let II — [a^ ■= e, —£/+ill < z < /} (a base of A), and identify W with 5/+^ via = (z, z + 1). (a) Show that ( 1 , 2 , . . . , / + 1) = and that w E:W is a Coxeter transformation if and only if vv is a cycle of length / H- 1. (b) Suppose that p — / + 2 is an odd prime number. Assume that 2 is a generator of Z/pZ ^. Let tt e be the (p — 1) cycle (1,2,4,..., 2^"^). Show that / ( 7 7 ) with respect to II is (p^ l)/8 . Conclude that (p^ - l) /8 is odd. 5.4 Let C = C(5, R) be a Coxeter group. We maintain the notation of Section 5.3. Attach a labelled graph F = (5, E, M) to (5, R) as follows: vertices: S edges: labels:

E



((^,*s')

^

5

X 5|m^y

for all

> 1},

( 5 , 5 ')

^ E.

Let E' = {(5,5') e E|M^y = 0mod2}. And consider the skeletal graph r = ( 5 , E \ E ' , M ' X where = 1 if ( 5 , 5 ' ) e E \ E ' and ML = 0 otherwise. Define an equivalence relation on 5 by s

s'

s and s' belong to a connected component of F'.

478

The Weyl Group and Its Geometry

Let [s] denote the equivalence class of s ^ S, and let 5 / ^ = Let G be the group that is the direct sum of card(I) copies of Z /2Z and let {1, be the copy of Z/2Z inside G corresponding to i e I. (a) Show that there exists a unique surjective group homomorphism if/:C G such that ilr.s whenever 5 e 5 is such that s e [5,]. (b) Let C' be the derived group of C. Show that C /C ' = G. (Ob­ serve that C' D ker i/r, and use the obvious inverse map G ^ C /C arising from the defining relations of G.) In the next two exercises we see how to explicitly compute the Weyl group, the minimum coset representatives for the coset and double coset decompositions W/W^ and \ W/Wi, I, K c J, and the Bruhat ordering. 5.5 Let 3 = (A, U , U ^ , V , V • » be a set of root data over IR, W the corresponding Weyl group, and 5 = {rj\j e J} the set of generating reflections. Let F be the fundamental chamber, and let I c J. Let A e F|. As far as this exercise goes it does not matter how A e Fj is chosen, but the canonical choice is
1 ^0

if / ^ I if i G I.

We define a (coset) graph F(A) == (V, E, M) as follows: vertices: V = {wX\w ^ W}, edges: E = {(wA, 5wA)|w e IF, 5 e 5, l(sw) = l(w) + 1, swX ¥= wX], labels: for ijl, v ^ W\, = {j} if (¡i, v) ^ E and v = = (j rel="nofollow"> otherwise. (a) (b)

Show that V is in 1-1 correspondence with W/Wj. Show that (V , E) can be constructed as follows: Define c V, E^ c E, d = 0,1,2,... inductively by (i) Vo = {A},E^ = 0 , (ii) = {rjfJLlfi e V^_1, (fjL, a / } > 0}, E^ = {(/X, v)\fjL e X/_i, V = rj^i e V^}, d = 1, 2 , . . . , (iii) V = U2=oY/,E= U2=oE^. (c) Prove that the sets are disjoint (hence also the sets E^). For /X e V, /X is of depth d if /x G V^. (d) Let IV e IF and let = (A, r A), ^2 = . . . = (rJ k - \ rjXX be a minimal chain of edges connecting A and r,JiA,’ rJk r, is the minimal f l = w \ = rj^ r,J \ A. Show ^that w == r,Jk coset representative of ivIFj (see Proposition 5.2.10).

479

Exercises

(e)

Prove that up to isomorphism the graph r(A) is independent of A e F|. We denote it by r(iT,I). (f) Show that the graph T(W, 0 ) essentially constructs W by induc­ tion on l(w) with 93 ^ determining all elements of W of length d. (g) Let A e F. Show that for w ^ W, j ^ J,

l{rjw) > /(w ) <=> {wX, ay) > 0, l(rjw) < l(w )

(h)

(i)

<=> <wA, a j y ) < 0.

Let K c J be an arbitrary subset, and consider the double coset decomposition Prove that each double coset has a unique representative of minimal length in W and that these representatives may be determined from the vertices v of the graph TOV, I) that have no upward A:-edges, A: e K (i.e., edges (¡JL, v) with ^ e K), from them. Let /1 = wA be a vertex of r(W^, I) with no upward /c-edges, A: e K. Prove that

where K q ==

e K\(ix,

= 0}.

5.6 Show that the following procedure constructs the Bruhat ordering on W by induction on length on the graph r(W, 0 ) of Exercise 5.5. Given w ^ W, v/c determine all predecessors w' < w of w. We can assume l(w) > 1. (a) Let 5 e 5 be chosen so that /(w ) < l(w). Show that for w' ^ W with l(w') < l(wX one has w' < w iff either l(sw') < l(w') and sw' < sw or l(sw') > l(w') and w' < sw (use the Z-lemma). (b) Show that it suffices to determine all w' ^ W such that w' <w and l(w') = l(w) — 1. Show that with s as in (a) and l(w') = l(w) — 1 we have w' < w iff either l(sw') < l(w') and sw' < sw or w' = sw. 5.7 Let = (A, n , n F, F < • , • » be a set of root data over U with dim^V < 00, and let F be its fundamental chamber. Suppose that A is indexed by J X J. Let K c J, and let R = where F = U icj^l(a) Prove that for i e J, iv e PF, l(r^w) > l(w) <=> wF c H^y. (b) Prove that for all i ^ K, R (Z (c) Prove that R is convex. (d) Show that any union of sets of the form wFj^, iv e PF, K c J is closed in the Tits cone 3£.

480

The Weyl Group and Its Geometry

5.8 Let ^ be a set of root data over U corresponding to an indecompos­ able Cartan matrix A of finite type with base II, and finite root system A. Let (f) be the highest root of A with respect to II. (a) Show that ^ F, (b) Let A G h* \ {0} be such that A e F. Write A = e U. Show that > 0 for all i (join to A). (c) Show that all the entries of A~^ are positive. 5.9 In this exercise we show how to realize the Weyl group W of an affine Cartan matrix A of type ( X = A, B , . . . , G) as a group of affine linear transformations on a euclidean space E of dimension /. We will also obtain a description of the Tits cone for a set of root data based on a minimal realization of A. This exercise uses parts of Section 4.4 (that are not explicitly about Lie algebras). We will assume that A is an indecomposable Cartan matrix of finite type II = {aj,. . . , Ui) a base for the corresponding finite root system A with highest root = E-=i«,a,, and that R = (1^,11,11^) is a minimal realization of A over the real field R. We form the extension 5^ = h ® 0 Rd, n ^ = {«0^..., where = (t - (/)'', n = {«o,. . . , c with ioLi^d) = Then R := (r* , n , n ^ ) is a minimal realization of A. We assume that (*1 • ) is a standard invariant form on f)^*, scaled so that (a^|a,) = 2 for all the long roots of 11 c E. In particular (!) = 2. The element 5 := «0 + (/> is null; ( 5 |a /) = 0 for all / = 0 , .. ., /. We set V = r * , V Then 3 := {A, F, F E, E < • , • » is a set of root data for A. Let its Weyl group be W == (r^\i = 0, .. ., /), and let W '•= (r^\i = 1 ,..., /> be the finite subgroup which is (isomor­ phic to) the Weyl group associated with the finite root system A. (a) Prove that 8 and i are PF-invariant vectors and hence that F^:={xeF|<x,(t>>0}, ¿ : = { x e F | < x , ( t > = l}, are IF-invariant. Let 7t:F F/R S be the natural inapping. Show that V/U8 carries the natural structure of a IF-module that makes tt a PF-map. Show that (1 *) induces a PF-invariant bilinear form on F/R 5. (c) Show that E == 7t(E) is a PF-invariant affine subspace of V/U8 and that PF acts as a group of affine linear mappings on E (see Section 7.3 for a definition of affine linear mappings). (d) Prove that by defining the distance between x , y in E by (x - y\ X —yY'^^, E becomes a euclidean space and the elements of PF act as isometries of F.

(b)

481

Exercises

(e) (f)

Show that = E-^iIRa, can naturally be viewed as the group of translations of E. Let t := e W. Show that t is the translation x ^ x (f> and that the normal subgroup T oi W generated by t is the group of translations jc

JC + /X,

where ¡ runs through the lattice L generated by the long roots of A. under the mapping / jjP (see the IBF (g) Prove that L = table in Section 4.4). (Show that any indecomposable root lattice is generated by its short roots.) (h) Let d* e 5* = be chosen so that
jl

P e'^^A => a

p

and

a —j8 e A.

Let ^^"*A := (a e^'^Ala is strictly imaginary} and

(a) (b)

(c)

Show that Recall := [a e 0 + n ( —t^)lsupp(o:) is connected}. Show that if a fl and g A+, then a + /3 e A+ [reason by induction on ht()8)]. Show that is a semigroup.

482

The Weyl Group and Its Geometry

5.11 Let A =
(c)

<0}

and 3£ c — >o0^r [Mx] Prove that if A is of level 1, then "A^= {/3

0 j(/3 |j8 ) ^ 0 } .

(d) Show that if A is of level 2, then A is hyperbolic. 5.12 Let ^ = {A, • » be a set of root data, and let S be its root system. Let ft be a subroot system of 2. (a) Let ft+:= 2 + n ft == Show that there exists a well ordering < in K so that ht()3,) < ht(pj) => i < j for all i, j e K. (b) Let H be the subset of ft+ obtained by the following prescrip­ tion. (i) B, where is the smallest element of K. (ii) If k k^, then e H if and only if ^ © Npj. }< k

Show that H is a base of ft. 5.13 The purpose of this exercise is to prove Proposition 5.3.3. (Show that R^ = R_^, Use Proposition 5.2.7(iii) and the Coxeter group presenta­ tion of W to conclude that there exists a well-defined map R^ , Show that this is surjective.)

Chapter Six

Category & for Kac-Moody Algebras T h u s d o th sh e , w h en fro m

in d iv id u a l sta te s

S h e d o th a b s t r a c t th e u n iv e r s a l k in d s W h ic h th e n r e c lo t h e d in d iv e r s n a m e s a n d f a t e s S t e a l a c c e s s th ro " o u r s e n se s to o u r m in d s .

—Coleridge

In this Chapter we investigate in detail the nature of the representations afforded by category ^ for a Kac-Moody algebra g. An important new ingredient that does not exist in the generality of Chapter 2 is the existence of a “Lie group” G associated with g. We have already seen in Sections 2.4 and 4.1 the advantages of associating the group 5L2(IK) with ^I2(IK), in analyzing the structure of g. Along the same lines we wish to associate a group G with g. This is somewhat complicated by the fact that there are really a number of different, but closely related groups, that one might wish to use. A nice survey on this is to be found in J. Tits’ paper [Ti6]. We have chosen the approach due to Peterson and Kac [PK], which is fairly straight­ forward and by its construction allows G to be represented on all the “integrable” modules of g. It is a historical irony that Lie algebras arose as an aid to understanding Lie groups, whereas here we find ourselves reversing the process and constructing Lie groups in order to understand Lie algebras. Just as Dg turns out to be slightly too small for a healthy representation theory (because it cannot separate the weight spaces that we want) so too we need to enlarge G to a group G. This is particularly important for the conjugacy theorems of Chapter 7 where the groups play a key role. In the classical case (Cartan matrix of finite type) G G.

483

484

Category á for Kac-Moody Algebras

In Section 6.1 we develop the theory of integrable modules for g and the groups G and G hand in hand. Section 6.2 investigates the nature of the weights and weight spaces of integrable modules, although the best results on this direction occur in Section 6.4 where we obtain the important Weyl-Kac and Weyl-Macdonald-Kac formulas. Among other things, these enable one to explicitly compute the weight multiplicities for irreducible modules in the category ^ (when g is invariant). As the names suggest, these formulas were originally discovered by H. Weyl in the classical finite-dimensional theory. In Section 6.3 we establish that, somewhat like g, G also has triangular decomposition (or Birkhoff decomposition). This and the related Bruhat decomposition are important in understanding the structure of G and in the classical situation have important uses, ranging from the study of differential equations to the algebraic geometry of Schubert varities to the construction of abstract geometries on Lie groups. In Section 6.5 we prove the complete reducibility theorem for integrable modules in category <^, and in Section 6.6 we give the explicit formula for the Shapovalov determinant for invariant Kac-Moody algebras.

6.1

INTEGRABLE MODULES

In the classical theory of Lie groups and Lie algebras the connection between a Lie algebra and its Lie group is made by the exponential map exp: g -> G. Ordinarily one expects that representations of g lift (or integrate) to repre­ sentations of G (although there are some subtle points here). We wish to create a group and a class of representations of g for which there is a similar relationship. The primary problem is that for infinite-dimensional representa­ tions 7T one can hardly expect that exp ir(x) will be defined for arbitrary X 0 g. There are two conceivable ways out. One could topologize the spaces involved and require that exp(7r(jc)) converge, or one could restrict the set of a : in g and the class of modules under consideration so that 7t ( jc ) is locally nilpotent, and hence exp(7r(A:)) makes sense. For arbitrary Kac-Moody alge­ bras it is only the latter for which there is a well-developed theory. The x for which we will define exp a: are those in U«ere^g", and the representations are those that admit weight spaces and for which each : g ^^ts locally nilpotently (integrable modules). The group G is essentially defined as the smallest group admitting the action of exp7r(A:), x e Later in this section we enlarge G to a group G that stands in relation to G much as g stands in relation to Dg. Let g be a Kac-Moody Lie algebra over a field IK of characteristic 0 with structure matrix A and triangular decomposition (5,g+, We use the standard notation of Section 4.2. a

U

6.1

Integrable Modules

485

A g-module ( tt, M) is said to be integrable if IMl

M has a weight space decomposition

M=

0

relative to IM2 For all j e J, the elements of 7r(g“>) and 7r(g““>) are locally nilpotent. We speak of tt as an integrable representation of g. The integrable modules form a full subcategory ^ of the category of all g-modules. It is immediate that ^ is closed under the formation of direct sums, tensor products, submodules, and quotient modules. Let £ be a subgroup of 1^* such that 0 c £. We define ^ ( E ) to be the full subcategory of cX whose objects satisfy IM(E)

P{ M) (ZE,

Of course ^ 0 ) * ) = We also use the full subcategory ^fJ<E) of ^ { E ) consisting of modules M for which dim

IM(fin)

< 00

for all Л e 1^*.

Lemma 1 Let Ml and М2 be K-spaces, and let Define a linear map X

:H o n iK (M

i,

e End(,^(M,), i = 1,2, be nilpotent.

М2)

М2)

by X--f^X2f-fXi

for all f e Homj^CMi, М2). Then x is nilpotent and (ехрл :)/= (ехрх2)/(ехрдс,)"*. Proof. Let L (resp. R) denote left (resp. right) multiplication in Hom^iMj, M2) by X2 (resp. Xj). Then X=L - R

and

LR = RL.

Since L and R are nilpotent it follows that x is nilpotent and that expx = exp L exp(—i?) = exp L(exp (Proposition 1.5.2). □

Category ^ for Kac-Moody Algebras

486

Proposition 2 Let % be a Lie algebra, and let tt : g ^ gI(M) be a representation of g on some K’Space M. Let jc e g te such that both ad x and 7t( jc) are locally nilpotent. Then for ally e g, Tr((expad Ac)(y)) = (exp-n-( j:))Tr(y)(exp i7( a:))

-1

Proof Consider K jc as an abelian Lie algebra. Then U(IKa:) = IK © K x © IKjc^ © • • Fix V ^ M and y e g. Define M l •=

IKi; H- IK7r(x)i; + IK7r(x) + • • • = U(IKjc) • v

and M2'^= U( 1Ka:) •7T(y)Mi. Both Ml and M2 are finite dimensional, and 7r(y) : Ml

M2.

Let Xi := 7t( jc)Imi and X2 — 7t( jc)Im2- These are nilpotent. By the previous lemma we have (expad 7r(x))(7r(y)) = exp 7r(jc)7r(y)(exp 7t( x )) Now 77 °ad jc = ad(7r(x))° 77 ((expad

77,

in Hom(M i,M 2).

and hence

x ) y ) = (expad 7 7 (x))(7 7 (y )) = exp 77(x)77(y)(exp77(x))"^

as maps on M^ Since v ^ M was arbitrary the result follows.



Proposition 3 Let (7 7 , M) be a %-module, and suppose that M admits a weight space decomposition relative to Then M is integrable if and only if the elements of 77(g"*') are locally nilpotent for all a Proof Let a Then a = wa^ for some 7 e J and w e PF. By Proposi­ tion 4.1.4 there exists an elementary automorphism n = n{w) of g such that wg"> = g“ and n is a product exp(ad ... exp(ad where each © U a en u (-n )9 “‘ Let y e g“^ and use Proposition 2 to conclude that Tr{ny) is locally nilpotent. Thus all the elements of 77(g“) are locally nilpotent. □

6.1

Integrable Modules

487

Fix a subgroup E of 1^* with Q c.E. We now construct a group attached to g and E that acts on every g-module of ^ ( E ) in a way compatible with the action of g. We begin by recalling the concept of the free product of a family of groups. Let A be a set, and let be a family of groups. By a free product of the family {G}^^j^v/t understand a pair consisting of a group G and a family of mappings :G^ ^ G such that FPl: Each : G;^ G is a group homomorphism FP2: Given any group H and any family of homomorphisms A e A, there exists a unique group homomorphism f : G ^ H that f ' ix = fx A e A.

H, such

As one would expect free products exist and are unique up to isomor­ phism. Furthermore the homomorphisms ¿x are injective and the subgroups ix(Gx) of G generate G. The construction and basic facts about free products of groups are covered in [Ja2]. The uniqueness of free product up to isomorphism allows us to speak of the free product of the family {Gx)x e adenote it by G = *AeA<JANotice that since the ¿x are injective we can identify each Gx with a subgroup of G. We now return to our Lie algebra g. For each a consider the one-dimensional space g"". We think of each g“ as an abelian (additive) group and define G = * We denote the injective homomorphism g" ^ G of FPl by exp^. We also write the group G multiplicatively so that for all a and x, y e g“ exp„^(x + y ) = exp„^(x)exp„^(y) and e x p ^ ( - x ) = exp„^(x) \ Since the subgroups exp^(g^) generate G, a typical element of G is a finite product of the form (1)

exp^"^(^i)---exp^^^(x,)

for some r e where /3, e"A and x, e g^' for all 1 < i < r. If /• = 0, then (1) is understood to be the identity element of G.

Categoiy ^ for Kac-Moody Algebras

488

Let ( tt, M) be a g-module in Then for each a and for all X e g“, exp(7r(jc)) is a well-defined element of GL{M) (Proposition 3). The mapping exp^: g" GL{M) given by x exp 7t( x) is a group homomor­ phism, and hence by FP2 there is a unique homomorphism tt:G

^ GL{ M)

such that exp^

r

GL{M)

ex p ¿

commutes. Let iC := n ker tt where the intersection is taken over all modules ( tt, M) of g which are in ^ ( E ) . Define := G /K ^ . We call the group G^; the derived (Lie) group associated with the Lie algebra g and £. This terminology will be justified in Proposition 15 below. Convention In general, whenever E is understood from the context, we simply write G instead of G^ and refer to the elements of ^ { E ) as “integrable.” a

Let v :G G be the natural quotient mapping. For each x e g“ and we define exp x e G by exp X = r^(exp^ x).

If 77: g tion

qKM)

is integrable, then there exists a unique group representa­ TT: G —> GL(A/)

such that the diagram GL(M )

6.1

Integrable Modules

commutes. In this notation we have for all a (2)

489

and for all x e g“,

exp 7t( jc) = TT exp x.

A particularly important case is that of the adjoint representation a d :g ^ By the above this formula leads to a group representation a d : ^ GL(g). We write Ad instead of ad in keeping with the standard notation in Lie theory: A d :G ^ ^ G L ( g ) . Equation (2) reads (3)

exp(ad x) = Ad(exp x)

for all x e g", a

Since exp(ad x) e Aut(g) and G^ is generated by exp(g“), a e'^^A, we see that A d:

—>Aut(g)

and Ad(G£) = G^^ as defined in Section 4.1. In particular AdCG^) is inde­ pendent of E. We will simply write Ad(G). Using Proposition 2 we have: if (ir,M) e jr(E ), (4)

X ^ Q, and g ^ Ge then tt (A d (g )x ) = Tr(g)7r(x)Tr(g)

Remark 1 Let jc e G be such that ttCx) acts like the identity for every integrable representation tt of g in
> e Z for all

2.4.4 M is completely reducible as an components are finite dimensional. In M and its eigenvalues are integers. Thus, • jc = jc => G Z. □

Category ^ for Kac-Moody Algebras

490

Proposition 5 Let L be a highest weight module with highest weight pair (A, v^) and weight system P(L). The following are equivalent: (i) L is integrable. (ii) For each / e J, L is the direct sum o f integrable {hence finite-dimen­ sional) irreducible -modules (iii) For each j e J, (ii) See 2.4.4. (ii) => (iii) The ^1^2^^-module M generated by is finite dimensional and hence by Lemma 2.4.1 (ii), we have dim M = 1. This shows that e N, and also that 0. (iii) => (iv) Obvious. (iv) => (i) Since L e the elements Cj, j e J, act locally nilpotently on L. We show that L •= [x e Llfor each ; e J there exists nj e Z+ with f p • jc = 0} is all of L. But i; +e L ' by assumption, and so it suffices to prove that f L c L' for all i e J. For this we use the following simple identity in U(9): (5)

m

=

J r

in U(g). This is easy to show by induction on n. Assuming (5), let x e L', and let us show that /¿ • x e L'. Let j e J, and choose mj e I\1 satisfying f^ j • jc = 0. Let n = mj + \A ^ Then for each summand in (5) either k > \A¿^\ + 1 or n - k > mj, and hence fff¿ • x = 0 by Proposition 4.1.8(iii) (applied to fj and f¿). □ Using Proposition 5 we can construct infinitely many non-isomorphic integrable highest weight modules for g. Proposition 6 Let A e g* satisfy (A , аУ } e N for all j e J. Then there exists a {unique up to isomorphism) integrable highest weight module L^^JiA) o f g with highest weight pair (A, i;+) with the property that, for every other integrable highest weight module L of q with highest weight pair (A,¿;+), there exists a unique homomorphism L ^ ^ J ^ A ) L satisfying + z;+. Moreover the irreducible highest weight module L{A) is integrable. Both L{A) and L^^^(A) lie in ^fiJ<E), where E is the subgroup o f generated by A and Q.

6.1 Integrable Modules

491

Proof. Let M(A) be the Verma module with highest weight pair (A, z;^). Let Xj • v+, y ^ J. Then Xj is a highest weight vector in M(A). Indeed for i ¥=j, e¿ • Xj = • ¿5^= 0, while for i = j this result follows from Proposition 2A1 (ii). Set N ■='Lj^jVH^)xj. Then N = E^.^jU(g_)xy c M(A). Set L ^ ^ ( A ) ’•= M (A )/N and v + v^-\- N. Then Lj^^(A) is integrable by Proposition 4. Furthermore, if L satisfies the hypothesis above, then by the universal properties of M(A) there is a surjective homomorphism cp: M(A) L. Its kernel contains N by Proposi­ tion 4. Thus there exist a unique induced surjective homomorphism 9• ^ ^ the desired properties. Since L(A) is a homomorphic image of L^^(A), it is integrable. Clearly L(A) and L ^ ^ ( A) lie in □ Remark 2 The foregoing can easily be applied to obtain analogous results about the lowest weight modules in the category ^finWe now return to the study of the group G = G¿;. We wish to impose some restrictions on the subgroups jE of 1^* that we will consider. These restrictions are partly suggested by Propositions 4 and 5. For each i e J let (o¿ e 1^* be any element such that a / > = 8¿j. Then the set ft := [(o¿\¿ e j} is called a set of fundamental weights of (g, ^ ) . Remark 3 Any set of fundamental weights is K-linearly independent. A subgroup P of is called a weight lattice of (g, if it satisfies the following properties: WLl: WL2: WL3: WL4:

e c P. ^ There exists a minimal regular weight p in P (see Section 4.4). P contains a set ft = ft(P ) of fundamental weights of (g, <9^).

If in addition P satisfies WL4R: P is a free Z-moduIe with a basis 0 consisting of K-linearly independent elements and such that O contains a set of fundamental weights of (g, .9^), then we say that P is a restricted weight lattice of (9, ^ ) . Notice that in any case WL2 and WL4 give = Z. Elements of P are called integral weights (because of WL2). An integral weight fjL is dominant if fjL e P+:= ( a e P| e N for all i e j}.

Category & for Kac-Moody Algebras

492

The standard weight lattice for (g, P== (A

is cZ }.

Remark 4 The standard weight lattice for (g, is clearly a weight lattice. If J is finite, det(>0 4^ 0, and is minimally realized then P is the only weight lattice for (g, In fact and 1^* = where n = e J} is the (unique) set of fundamental weights of (g, Now WL4 and WL2 combine to show that any weight lattice must be exactly = P. This is clearly a restricted lattice and we have P^= Hj^jNcoj, The situation for the cases when d et(^) = 0 is more complicated. The Appendix describes the case of in some detail. Remark 5 If J is finite and P is any weight lattice then the Z-span of is all of P. Let \ ^ P, and define aj •=
As far as the representation theory of g is concerned, there is no need to consider restricted weight lattices, and the standard weight lattice is the natural choice. The representation theory of G is more subtle, and there are instances when the standard weight lattice will be too large (see the introduc­ tion of G later in this section). For this reason we introduce restricted lattices (which really are lattices). We now choose an arbitrary weight lattice P and work in the category ^ { P ) with the group G = G(P). For each a let c G be the subgroup generated by exp g“ and exp g"“ (cf. Proposition 4.1.6). We fix once and for all an § 12-triplet [e^, a ' ^ , f j with e g“, / „ e g Clearly = 5L^2““1 Proposition 7 (i)

Let ( tt, M) be an integrable q-module, and let a e'^^A. Then there exists a surjective homomorphism k(; rel="nofollow">:5L2(K) ^ ' it(5L<2“>) such that for all t g IK, 0

1) ^



1) = '»f(exp if«).

(ii) There exists a unique isomorphism : 5L2(K) ^ 5L<2“^

6.1

Integrable Modules

493

such that for all t ^ K,

and ■ok<“) = k(«).

Proof (i) Identify with ^I2(1K) by <-> o ) ’ ^ (1 o)* ir(e^) and 7t(/^) are locally nilpotent, M is an integrable §l2(lK)-module and, using Lemma 2.4.4, tt integrates to a representation k^“^ of 5L2(IK) in which

®^(^(o

and

(;

;)■

0 ) ) ^ (0

expT7(re„) = ir(ex p ie„)

j)

r(exp tf^). Evidently k^“X5L2(IK)) = tt(SL^2^\

(ii) Let SL^2^ be the subgroup of G generated by exp^ By universal properties = (exp^ 9“)*(exp:i^^ g~“). The homomorphisms exp^

|J

and exp^^ g

^ j, exp:^^ie_^ ^ ( t

l)

mine a surjective homomorphism o) : SL^2^ SL2(K), Let ( tt, M) e ^ ( P ) , and consider the mappings k^"^ of part (i) and TT: G ^ GUM) . From ^(exp^^ te^) = exp(irie„) = k<“>|

J JJ

= k<“><w(exp„^ ie„)

and a similar calculation for exp tf^, we obtain the commutative diagram SLi“^

5L2(K) Thus ker -ir 3 ker ca. This being true for all (ir, M ) e ^ ( P ) , we have 1 ^ ^ 0 5 4 “^ =>kero) and hence an induced homomorphism k^“^: SL2(K) SL^2 ^ with k^“^<«) = V on SL^2 ^ (see above for the definition of v : G -* Gp).

Category ^ for Kac-Moody Algebras

494

This leads to the commutative diagram

Now is surjective since v is. Hence it remains to show that is injective. Suppose a e Choose A e so that e 2Z + 1 (this is possible since \ a ^ ^ Q^X Then ^ ^ ( P ) , and if we let v+ denote a highest weight vector for L ^J iA ), M — E^l’o is the irreducible §I2 (IK)-module of dimension
+ 1. But the correspond­ ing action of 5L2OK) is faithful (Lemma 2.4, Corollary 6). If we denote this representation of g on L ^ ^ (A ) by tt, then our conclusion is that k^“^ is injective and hence also k^“\ If a e ''^A_ we use the same argument revers­ ing the roles of and /^. □ In the sequel, when dealing with representations ( tt, M ) in ^ ( P ) , we will often suppress explicit mention of the mapping tt and write both the action of g and G by an infixed * or even simply by juxtaposition. We will also refer to the representation in J^(P) simple as integrable (omitting the explicit mention of P which is assumed to be fixed in the discussion). For each i e IK^ we define elements n(t) and h(t) of 5L2(IK) as follows:

[see (2.4.9) and (2.4.10)]. For each a we have a fixed il2-triplet {e„, f j and §1^“^= ® © IK/„ = §I2(IK). Define elements n„(0 and /i„(i) of by n , ( 0 = k<“> (n (0 ), ( 6)

/»„(0 = k<“) ( /,( 0 ) . From (2.4.9) and Proposition 6, (7)

n „(i) = ex p ie„ex p (-fY „)ex p (te„).

From (2.4.10) we have

(8)

MO ="a(0««(l)“ ‘-

Ke^

6.1

Integrable Modules

495

From the definitions (9)

n „(í) ^ = n ^ ( - í )

and

‘ = /i„ ( í ^).

We also have (Proposition 4.1.3) A d (n ^ (í))a ^ = - a ^ .

( 10 )

We introduce two subgroups N and H oí G defined as follows: N := {n^{t)\a

t e 1K^>,

H '= {h^{t)\a

t e K^).

Proposition 8 Let ( tt, M ) be an integrable representation o f g with weight system P(M ). Let a e'^^A, and let A e P(M). Let be the reflection in a. (i) Given V e there exists v ' e such that Tr(nJ,t))v = for all t e K^, In particular ir{nJ^t))M^ = (ii) For all t e IK^, Tr(/t^(i)): ^ and irihj^t)) acts as a scalar multiplication by on M^. Proof Fix V e M^. To keep the notation down we suppress the tt. Then from (7), nj, t)v e the only power of t occurring in the homogeneous term of degree Á + k a in njit)v is t^. Thus

k^Z where e • V = -nj<^t) '

Computing *««(0 *v = nj^t) • (A d(n^(-i))a^) • V (see (4)) in two ways gives

E( + from which = 0 unless k = —(A ,a ^ ). Part (i) follows with v' *= ^A-a n = nJ^~t)M'^<^^ C M \] From (9), /t^(r) = « « ( - 0 ” ^ n « (-l), and from part (i), nj^ —t)v = { — Now part (ii) follows directly. □

496

Category û for Kac-Moody Algebras

Corollary

(i) H is abelian. (ii) Every element o fH may be expressed uniquely in the form n¿ ^ where each t¿ ^ and t¿ = 1 for all but a finite number o f i. (iii) For each a the mapping t hj^t) is an injective homomor^ phism of into G. Proof (0 Let a, )8 5, i e K^, and let (v , M ) be integrable. Then for each weight A of M, hj,s)h^(t) acts as on M^. Thus Tr(hJ,s)hp(t)) = Tr(h^U)hJ,t)X and this being true for all ( tt, Af) e <X(P) we obtain hj^s)h^{t) = h^(t)hj.s). This proves (i). We observe in the same manner that hj^s)hj^t) = hj^st). (ii) Let a e'^^A, and suppose that = Hi^jC¿a¡^ (where all but a finite number of = 0). Then for any t and any weight A of (rr, M ) e ^ ( P) , hj, t) acts on as multiplication by 7

This is precisely how Ylh^it^O acts on M^. This being true for all ( tt, M), we obtain hÁ0 = n h 4 n ^ Thus every element of hj^t) may be expressed in the desired form. Since H is abelian and is generated by the elements hj^t), and from our observation in part (i), we see that every element of H can be expressed as required. Applying h = Ylh^it¿) to the weight (Oj, we find that h acts as tj on The uniqueness for the expression of h follows. (iii) Let a e'^^A. We have seen that the mapping 5

h^{s)

is a homomorphism. We write = L c ia ^ , and observe that since is a PT-translate of some is indivisible [i.e., gcd(c¿) = 1]. Now, if hj^s) = 1, we see from L(o)j) that s^j = 1 for all j, whence 5 = 1. □ According to Proposition 8, nj^t) induces a permutation on the set of weights P(M) of any integrable module ( tt, M), namely A r^A. Since each element of A/^ is a product of terms of the form n^(t) [see (6.12)], there is a map [\ : N

6.1

Integrable Modules

497

such that n(M^) = for all n N and for all A e P(M). Indeed, if n = «ajiti) • • • then InJ = Thus IJ is independent of the representation (ir, M). For jv e IF we will use the notation fwl to denote any preimage of w. Proposition 9 The mapping I J is a surjective group homomorphism with kernel H. In particular H < N and N /H = W. Proof. If InJ = w, tn'J = w', then for any (ir, M) e J^(P), nn'M^ = nM ”''^ = which shows that I J is a homomorphism. Evidently H lies in the kernel of L J [Proposition 8(ii)]. We show that H is normal in N. Let a, ¡3 e''*A. Then we claim that ^ = hr^0Ís)

(1 1 )

which obviously will imply the normality of H. To prove (11), apply both sides to a vector u e for an arbitrary ( tt, M) e ^ ( P ) and A g P(M):

since =A, and At this point we have a surjective group homomorphism of N / H onto W, Now we construct its inverse [St]. We use the presentation of W given in Proposition 5.3.3: IF = <w„|a e " A ,

= 1,

Let w^ ■= nJX)H, a e"A . Then by (8), nj. t) e HnJ^i) = which shows that w^ = n J.t)H for all t e IK^. Thus w^ = nJ ^ t ) n J , - \ ) H c H, and this shows that = 1 in N / H . Also ‘ = «a(l)exp Cp cxp( -/p)exp C^n„(l) = exp(Ad n „(l)e ^ )ex p (-A d n„(l)/^)exp(A d n „ (l)e ^ )/f by (4). Now Ad nj. t) e Aut(g) and so by Proposition 8(i), Ad n„(r) maps {e^, ,fp} into an ilz-triplet for that is, {se,^, r„p'^, s~ ^frji for some s e

Category ^ for Kac-Moody Algebras

498

(see Proposition 4.1.6 and also Section 4.1, Remark 1). Thus w,

It follows that there is a homomorphism W N /H with for all a, and this is clearly the inverse of the induced homomorphism N /H W. □ Corollary G is generated by the set S ■= {exp te^, exp tf^\i e J, i g IK}. Proof. Let a and write a = for some j e J. Let n¿^í) • • • 1). Then exp(Ad nitej)) = n exp(tej)n~^ shows that exp g“ is generated by 5. □ As a direct consequence of the foregoing we have Proposition 10 Let (t7, M) e ^ ( P ) . (i) W stabilizes P(M). (ii) I f n ^ N and [n\ = w, then nM^ = particular dim = dimM"^^.

for all A e P{M). In □

Proposition 11 Let ( tt, M ) be module in category 0 and category ^ ( P ) . Then for each A ^ P(M) there exists a unique ¡jl e W \ such that W \ n P + = ill). In the case that IK = [R and J is finite we have ¡i = W \ n F, where F is the closure of the fundamental chamber for i)* relative to II. D Mq = (0) be a Proof Let A ^ P(M), and let composition series of M relative to A (Proposition 2.6.8). Then there is a subset I of (1 ,..,, fc} for which = L(A¿) for some A, > A and such that (p > \ => (p ^ P(L(X¿)) for some i e I. Evidently each L(A¿), i e I, is integrable, and hence A e P(L((p)) for some cp e P_^_. In particular A e
6.1

Integrable Modules

499

v ^ P + n WX then L(v) is integrable and so WX In particular V G WX ^ fi i Q+ and we see that necessarily v = ji. Thus P+Pi WX = {/x}. In the case that IK = R and J finite, lies inside F. □ Let us recall that the derived algebra Dg of g is generated by the elements e¿,ay,f¿, i e J, and that g = Dg + Í), Dg Pi Al­ though Dg is easier to define than g, g is far more convenient for the purposes of their representation theory. This is primarily because i) can separate the weight spaces of any module with a weight space decomposition, whereas ' Li ^j Kay in general cannot. The same problem arises with our group G: It cannot separate the weight spaces of the integrable modules in general. Furthermore the subgroup Ad(G) of Aut(g) is not large enough to produce the ingredients needed in the conjugacy theorems that we wish to prove in Chapter 7. The solution is to embed G in a larger group G. We will do this in such a way that G = (G, G) and that G = GX, where is a group that acts diagonally on integrable modules. In Section 6.3 we will see that if J is finite and the Cartan matrix of g is nonsingular, then G = G whenever g is minimally realized, just as Dg = g. To introduce the subgroup A" in a satisfactory way, we will assume that P is a restricted weight lattice (see WL4R) in 1^*. Let H G = G(P) be the corresponding diagonal group. A typical element of H is h = We have seen in Proposition 8 that for any module M of ^ ( P ) and for any weight X of M, h acts on as multiplication by H /e ^ This leads us to consider the mapping / / A H o m (P ,K ^ ) defined by L(h) where t(/z)(A) = ^ Since P contains a fundamental system of weights, we see that t is injective. We will often identify / / as a subgroup of the group Hom(P, of characters of P. A subgroup X of Hom(P, IK^) is called a separating group of characters if SGC: For all X, fjL

P with X

there exists x ^ ^ such that ;^(A)

Since P is a free abelian group, it is clear that Hom(P, is itself a separating group of characters (a natural choice). In particular such groups exist. However, H need not be separating. Indeed, if P contains weights 5 # 0 satisfying (8, = 0 for all i e J, then H cannot separate 0 and 8.

500

Category ^ for Kac-Moody Algebras

Let X c Hom(P, be a separating group of characters of the weight lattice P. If ( it, M) is any g-module in ^ i P ) , then we obtain a homomor­ phism A ut^iA /), AT where

is defined by (see Section 2.1) x J m> ^ ■= multiplication

by a'( m)-

A simple calculation shows that for all a e ''^A, x e g“,

( 12 )

exp(rr(Arad(-*))) = Ai^exp( 17(01:)) at; ^

Remark 6 Let X c Hom(P, IK^) be a separating group of characters. Let ( tt, M) be any integrable module in ^ ( P ) , and let u E: M, Then the smallest subspace of M containing Xj^u) is the 1^-submodule N generated by u. If u= ^ In particular any jC-invariant subspace of M is an ^-submodule. The argument to prove this is a variation of that of Proposition 2.1.1. Let G •= G(P). We are now going to define a map :X Aut(G) through which we will enlarge G to a semidirect product G >^X. Let a' ^ For each a e '’^A let

be the group homomorphism Ar„ : o:

exp(Arad(-«)) = exp(Ar(a)o:).

By the definition of G this extends uniquely to group epimorphism X:G ^G satisfying X exp^ = a:,,. Let us show that Kp = ker x. Consider a typical element X = expp^(xi) • • • exp^^jxj

6.1

Integrable Modules

SOI

of G. Then

;f(^) = X expp^( Jíi) ■■■ X = e x p ( A T a d ( ^ i ) ) • • • exp(A T ad(

Let ( tt-, M) be an integrable representation of g in ^ { P ) . We have ='^exp(ATad(^i)) ••• 'irexp(;(^3d(^«)) = exp(TTArad(^i)) •••exp(TT;^rad(-^n)) = Ar^exp(Tr(ACi))Ar"' • • •

[by (2)]

exp(ir(jc„));^:-i

[by(12)]

= Ar^exp(ir(xi)) • • • exp(ir(x„))Ar;:* (13)

= Ar^irexp(xi) ••• Trexp(x„))Ar“ ‘ = AT^irv expp^^(xi) ■■■ Ttv exp^„^(x„)Ar“ ‘ = AT>exp^^^(xi) •••
From (13) and Remark 1 it follows that Kp = ker x, as desired. We therefore have an induced automorphism of G making commutative the diagram

We define the group homomorphism - : X - y A ut(G ) by ~ - X ^ X-

and form the semidirect product G* = G XIZ. By definition this means that in G * the composition law is given by { S i , Xi ) { 82, X2) = i 8 iXii82)>XiX2)-

502

Category ^ for Kac-Moody Algebras

Note that for j: g g“, a e "A we have (14)

x{exp^ x) = iv(exp„^ x) = x(exp^ = Xa(^) = X a(^ ) = eXp(ATadAi).

Note also that G* is generated by the elements of the form (exp x ,x ), where X e g“, a G "A, and x ^ Let ( tt, M) be an integrable g-module. There exits a unique representa­ tion (-ff*, M) of G* satisfying for all g G G, g X, and i; g M, (15)

= Tr(g)ox^(u).

Indeed for all ^ e g“, fe g g^, and o-, t ^ X, IT* ((exp fl, o-)(exp fc, t ) ) ( z;) = TT^(exp a{&exp b ) , a r ) { u ) = TTexp(fl) o Tr(i7 exp(fe)) o(o-r)^(i;) = irexp(fl)o(exp(7ra-3d^?))°a-^°T^(i^) = TTexp(iz) 0 0-^0exp 77-(fc)oT^(z;)

[by (14) and (2)] [by (12)]

= Tr*(exp(fl),o-)(Tr*(exp(6),r)(i;)). We now define the Lie group G = G(P, X ) (with respect to a restricted weight lattice P and a separating group of characters J^) of a Kac-Moody Lie algebra g as follows: G — G^/Kp, where Kp •= fl tt*, the intersection being taken over all integrable represen­ tations ( tt, M) of g in J^(P). The group G = G(P) depends on the choice of weight lattice P. (Later in Proposition 6.3.15 we will see that G is essentially independent of P,) In turn G = G { P , X ) depends also on the choice of the separating group of charac­ ters X. For simplicity of notation we will write G and G in the remainder of this section. As above, “integrable representations” will be understood to belong to J^(P). Since no confusion will arise, we will still denote the elements of G by (g, \ ) (instead of (g, There are obviously homomorphisms ic :G

G^

G,

G*

G.

6.1

Integrable Modules

503

We denote the image of in G by X, (Since G actually embeds in G, we will continue to denote its image by G.) ^ Given an integrable g-representation ( tt, M) we have the mapping itx • it Aut[|^(M) with X ^ Xtv;: Evidently factors through X to give itx '• X Auto^(M). Given e ^ we will usually denote its image in A" by then TTxix) = Xv’ which acts on by multiplication by ;^(^) as before. Proposition 12 (i) The homomorphism Iq i G G is injective. (ii) The kernel o f the homomorphism ix • X G is

{x ^

= I for all fi e P ( M ) , and for all

e

In particular if {ix\ix e P{M), (ir, M) e J^(P)} spans the Z-module P, then ix is injective. This always happens if J is finite. (iii) Let ( it, M) be any integrable q-module. Then there exists a unique representation (ir, M ) of G for which

(16)

TTIg = TT, 'ñ’lx = Xtt-

Proof Let ( tt, M ) be any integrable g-module. Let g e G. Then from (15), iXy) = 'ir(g)(i;), so 'ir*(g, 1) = 'ir(g) and (g, l ) e / ^ if and only if g = 1. This proves part (i). Similarly for x ^ X , ir*(A')lw'‘ = multiplication by xil^X so -a^ix) ^ K if and only if x(p-) = 1 for all p e P(M) and for all integrable modules M. In the case that J is finite P^ spans P as a Z-module (Remark 5). Since for all A e L(A) e ^ ( P ) we see that [p\p e P(.M), (ir, M ) e ^ ( P ) ) spans P. This proves part (ii). Now part (iii) follows from (6.18). □ We refer to (ir, M) as the representation of G obtained from (v, M). In particular (ad, g) induces a representation (ad, g) of G. In the sequel we will usually simply write ir f o r ^ . In particular, since ad = Ad, Ad will be denoted by “Ad.” Note that Ad|c = Ad^. Remark 7 X is a subgroup of Hom(P, K^), while H can be viewed as such. Let h e H C\ X. We can view h as an element of G in two different ways, namely

Category 0 for Kac-Moody Algebras

504

and H C \ X ^ X - ^ G. These in fact give the same element of G, In particular, ii x ^ H C\ X, then in G,

( aT>1 ) = ( 1 >AT)Thus G n AT is not trivial in general. We look at this in more detail in Section 6.3. Proposition 13 Let q be a Kac-Moody algebra, and let G be its Lie group. Let ( tt, M) be an integrable representation o f g, and let g ^ G and y ^ Q. Then (0 ir C g M y M g ) - ' = ir((Ad iX y)), (ii) 'ir(g)exp ir(y)'ir(g)~‘ = exp Tr((Ad |X y )) if Tr(y) is locally nUpotent. Proof. It suffices to establish the result for § = (exp x, and X ^ Now * ( exp X, AT)

for x g g“, a e "A,

y ) -n-(exp X, AT) ” ‘

= ir(expx)Ar^Tr(y)Ar“ H'Tr(expx))"' = 'ir(expA:)Tr(Arad>')'>r(expx)"‘ (12) = ir(Ad(exp Jc)ATad(y))

[by (4)]

= ir(A d(expx,A ')(y)). This establishes part (i). As for part (ii) one just has to expand expir(y).



Remark 8 For each x e g“ and a e "A we have defined an element exp X G G with the property of equation (2), namely ir(exp x) = exp tt(x) for all ( t t , M ) g ^ ( P ) . At this point we cannot extend this definition to all X G g for which wix) is locally nilpotent in every integrable representation ( it, M) since we do not know whether or not G contains an element that induces exp tt( x ). In Chapter 7 we will show that, this is actually possible if g is an invariant Kac-Moody algebra. For now, however, we can make the following observation.

6.1

505

Integrable Modules

Proposition 14 Suppose that some x g g has the property that tt{ x ) is locally nilpotent for all (tt, M) G cX(P), and suppose that we have an element exp jc e G satisfying (2) (it is evidently unique). Let g ^ G. Then (0

Tr((Ad gXx)) is locally nilpotent for all ( tt, M )7rexpjc = exp7r(x) G J^iPX GO there is a unique element exp((Ad gXx)) ^ G for which (2) holds {for Ad g{x)\ Gii) exp((Ad gXx)) = g exp{x)g~\ Proof Part (i) follows from Proposition 13G). By Proposition 13(ii), exp-n-((Ai/g)(A:)) = Tr(g)expir(;»:)'ir(g)"‘ for all

{v,M )^J^(P).

Thus, if we define exp((Ad gXjr)) by part (iii), it follows that (2) holds [for (Ad gXj:)]. Evidently (2) guarantees that exp((Ad gX;c)) depends only on (Ad gXjr) and not on the choice of g and x. □ a

Here is an example. Using Proposition 14(iii), for all g e G and for all e IK, exp((Ad g)ie„) = g exp te„g~^ e G

In particular, if

g

for all a e "A+, t e IK.

''^A, 5 g

hp(s)exp te„h^{s)~^ = exp(Ad = exp(s<“’'^''>re^) by Proposition 8(ii). Thus hp{s)exp t e^hp{s)~\ exp tej~'^ (17) = exp((i<“'^''> - l)ie„). We have similar results for

with a

g

'^^A_.

Proposition 15 (i) G < G, G = GX, G /G = X /G n X.^ (ii) (G ,G ) = G. (iii) G is perfect [(G, G) = G)]. ^In Corollary 6.3.12 we will prove that G n X c. H .

Categoiy ^ for Kac-Moody Algebras

506

Proof. Part (i) follows from G < G ^ and G^ = G X. Since G /G is abelian, (G, G) c G. To prove part (ii), we need only to prove part (iii). However, (17) with a = ^ and ^ = 5 gives exp(24fe^) e (G, G) for all a e " and f e K. Since similar considerations apply to /^, and since G is generated by the exp(g“), a g '^^A, part (iii) holds. □ We finish this section by studying in detail some representations of G. These results will not be used until the conjugacy theorems of Chapter 7. Proposition 16 Let be integrable representations in ^ ( P ) o f g, i = 1,2. Let M = Hom|,^(Mi, M2), and let ( tt, M) be the representation o f g given by 7 r ( x ) f •= 7T2( jc )/ —f'TTi(x)

for all X ^ g , / £ M.

Define a representation ( tt, M) o f G by ■w(g)/= Then for fl// X G g“, a e ''^A we have (18)

exp 7r{x)f = Tr(exp x ) f .

In particular, if ( tt, M) is an integrable ^-module, then tt coincides with the representation of G obtained from ( tt, M) by Proposition \2{iii). Proof The argument is a variation of the proof of Proposition 2. Let a e '■^A, X e g“. Let v ^ M^, and define M[ to be the finite-dimensional space generated by the action of 7Ti( a:) on í; and M^ the corresponding space for 7T2( x ) acting on fM[. Then /|^fj e Hom¡,^(MÍ, M ^, and applying Lemma 1 with x^ -= irfx), we obtain exp 7r(x)f = exp 7T2(x)/(exp 7Ti( jc)) ^

on M[.

Since V was arbitrary, exp 7r{x)f = exp 7T2(x)/exp 7Ti( x ) “ ^ == Tr(exp(x))/. Thus (18) holds. Suppose next that M is integrable. We show that X>n‘2f^'Tri

Xvf‘

6.1

507

Integrable Modules

For this we may assume that / e M**. Then for mj e Mj we have

XtT2J ^TTi

XtT2 j^(A + fi) at( a)

/( m i)

[sin ce/(m i) e

= a ( m) / ( " I i )Having established this fact, we see that ■rr(exp X, x

) f

1-1 •= 'iT2(exp x, ;if)/Tri(exp x, at) ' = •rr2(exp x)Ar^^/A-;:/'iri(exp x) =
which is precisely the representation of G obtained from (ir, M).

Proposition 17 Let (tti, M j) and (772, be integrable representations o f g. Then the tensor product representation ( tt, M) == (77^ <S>772, ® M2) o f g is integrable, and the corresponding representation ( tt , M ) o f G satisfies T rC g X m j <S>m 2 ) = TTi(gXmj) 0 'TT2(gXm2) for all g G: G, E: Mj, ¿znd m2 ^ M2. ?roo/. Let jc e g“, a e

Then

IT (exp x)(m i 0 m2) = exp 7r{x){m^ 0 m 2) “ 77(x)”(m i 0 m 2) n\

n= 0

=

£

£ i ” ]^(^i(^)"

„ = 0/ =0 V‘ =

' w i ®'n-2(x)'m2)

e x p ir i(A :)m i ® e x p 7 T 2 (x )m 2

= 'tTi(exp x ) ( m i ) ® 'iT2(exp x ) ( m 2 ) .

Category ^ for Kac-Moody Algebras

508

For

e A",

e M^ \ and

^

'Tr{x){mi ® m2) =

we have ® ^2)

= AT(Ai + A2)mi <S>m 2 = Ar(Ai)mi <S>x(^i)m2

= ^ i ( x) ( f n^ ) ® 'n-2(Ar)('W2). We can now apply Proposition 12(iii). 6.2

WEIGHT SYSTEMS

In this section we study the weight systems P(M) of integrable highest weight modules ( tt, M) of a Kac-Moody algebra g. We give two characteriza­ tions of P(M) as well as algorithms for constructing P(M) and the dominant weights in P(MX Throughout this section g is a Kac-Moody algebra over a field IK of characteristic 0 with structure matrix A and corresponding triangular decom­ position T = (ij, ¡2+7 E denotes the standard weight lattice. We use the notation of Sections 4.2 and of 6.1. Let M ^ J^, the category of integrable g-modules, and let A lie in the weight system P(M) of M. For each a e

the a-weight string through A is defined by

5(A, a ) =

A, O') == (A + ka\ k e Z} Pi P ( M )

If M = g under the adjoint representation, then P(M) = A(g). If j8 e A and a e ''^A, then S(p, a) is the a-root string through p. The terminology is justified by the following (cf. Proposition 4.1.13): Proposition 1 Let A e P(M ), and let a (i)

■"A.

Either Sooi 5(A,o') = {A + koc\k ^ Z} or Sfin* a.) = [k ka — d < k < u]

SI: S2: S3: (ii)

for some d and v in N.

In either case the reflection r^ reflects the string 5(A, a) about its midpoint p := A - a. Moreover, if holds, then d — u = (A, a ^ ), the sequence {dim is increasing up to its midpoint and then is decreasing, and the sequence (dim is symmetric about its midpoint, If M ^ then only the case 5^^ can occur.

A sequence with the properties S2 and S3 is called unimodal. Proof, (i) Since a e ^1^2^ = g“ © [g“, g"“] 0 g““ is isomorphic to ^l2(k) (Proposition 4.1.6X By Proposition 6.2.3, M is an integrable ^1^2^module. Let N ■= Then N is an §I^2“^"S^t>^odule of M and hence also integrable. Furthermore P( N) = 5(A, a). By Proposition 2.4.4 we can decompose N into irreducible ^1^2^^'Submodules. Each of these irre­ ducible submodules has the form K = where acts diago­ nally on by the scalar s - 2i and dim = 1 for each i (Section 2.4). Since acts diagonally on by + 2k. K ^-2i ^

))/2-i] a^

Thus already s = (mod 2). We now repeat the Freudenthal midpoint argument of Section 4.1. The midpoint of this set of weights, as i runs from 0 to s, is 5 - < A , q:'^>

jIA

\

5-

( X , a ^ y

------- -------- —5 a + A + ------- -------- a

= A - -a, which is independent of 5. Note that /x is a weight of the string if and only if (A,q:^> = 0 (mod 2). In any case all the irreducible submodules K involve sets of weights with the same midpoint and they all involve / or all involve ¡JL + depending on the parity of . If the dimensions of the submodules K are not bounded, then 5(A ,a) = {A + ka\ k e Z}. If, on the other hand, the dimensions are bounded, then taking K of maximal dimen­ sion, we have P(K) = P(N). Then 5(A, a) is finite and of the desired form, and {dim is unimodal. Since jl

^(A + ua + A —da)

=

jjl

=

X



|(A ,a^)a,

we have d — u = (A, ). (ii) Assume that M If the dimensions of the irreducible factors used in part (i) were unbounded, then there would be an infinite number of factors. The fact that each of these factors contributes one dimension to either or (depending on the parity of ) contradicts Me □ Remark 1 If M is a highest weight module for g with highest weight pair (A, Ü+), then for any A e P { M \ A A there exists at least one a e II for which A + a e P{M). This follows from the fact that Á¥^A=>Á = A — p, P ^ Q+ and is spanned by elements of the form f ¿^... f¿^ • u+, where * +a¿^ = This trivial remark is extremely useful for inductive proofs on weight systems of highest weight modules.

Categoiy ^ for Kac-Moody Algebras

510

Let A

and consider the Q+-fan A iQ ^ . We define the depth function dj, : A i Q ^ ^ N

by E c , a , .) = E cy . ;e j / yej Let A e F, and let L be an integrable highest weight module with highest weight A. Then according to Propositions 6.1.5 and 6.1.6, A ^ F+ and there are homomorphisms L^J^A) ^ L -> L(A) [the last because of the definition of L(A)]. The next result is an algorithm for constructing F(L). We denote this common set of weights by F(A). Proposition 2 Let L be an integrable highest weight module with highest weight pair (A, i;+), A e P^. For all n let PJiL) denote the set o f weights o f depth n in P (L \ Then (0 (ii)

Po(A) = {A}, A e A i 2+ with d ^ k ) = n > 0, then A e F„(L) if and only if there exists an / e J and a k ^ such that A + ka¿ e P„_^(L) and (A + ka¿, ) > k.

Proof Evidently Pq(L) = {A}, since L = U(g_) *í;+. Let A e P^iL), n > 0. By Remark 1 there exists an / e J such that A + a¿ e F(L). The «¿-string S(k,a¿) through A has the form {A + Then (A + wa¿,«¿^> = (k, 2u = d - u 2u = u d > u. Conversely, if A e A J. 2+ and A + ka¿ e P^_¡fL) for some i e J and A: e Z+, where
k, then 5(A + ka¿, a ^ ) = {A + ka¿ + pcíi)-d^p k . Thus d > k, and hence A e F(L). □ Corollary Let L be an integrable highest weight module with highest weight A e P ( L ^ J A ) ) = P(L) = P(L(A)).

Then

We denote this common set of weights by F(A). Proposition 3 Let A e ]^*, then rad(g)L(A) = (0). Proof This is an application of Proposition 2.7.5(ii).



Integrable modules arise directly in the study of the adjoint representation of a Kac-Moody algebra. We will assume that g = R) is a Kac-Moody

6.2

Weight Systems

511

algebra with structure matrix A = (Ajj), i, j e J. Let 0 # K c J, and set 9k =

e K> + ^ c g.

Then 9 k is a Kac-Moody algebra with structure matrix Ay^ ■= (.<4,^); y^KWe view g as a gK-module by restricting the adjoint representation. Set G k = ® 2 a, c Q, i S K

and note that 9k =

® 9“, ae Ak

where = A (^) n [s®® Section 4.3, Remark 2, and 4.13)]. Thus g^ admits == (^, ®„eAKnA+9“>G k ^ G+^o'lgK^ ^ triangular decomposi­ tion. For each coset a e G /G k define Ms = E 9 ^ We have the following facts. 1* 9 ®a€ Q/Qk^ ^ ' 2. is an integrable If ^ suppose that á = a + Qj^, where a e A. If in addition a e then a e and M- c is an ideal of If a ^ A \ A^, then a + n A c A+, and hence ^ 9 ± according to whether a e A +. 3. For all á for which ^ (0), either is an ideal of g^, or c g_ and e c g_^ and Af^ g

or ^ k)'

It is surprising how little we know about the modules M- when a e A \ A^; not even whether or not they are completely reducible (unless g^ is invariant). However, the modules when / e J \ K are quite accessible. For simplicity we treat the cases M_^.. Proposition 4 Let q be a Kac-Moody algebra with structure matrix A = (.^4¿y), /, j e J, and let K be a nonempty proper subset o f J. Let / g J \ K. Then with the notation above we have M_s. = ad u(9 k )/„ (ii) M_^. is an integrable highest weight module with highest weight pair (i)

(iii)

P(.M_¡¡) - ( —a, -1- Gk )

^

M“ s = g“ for all a e

512

Category ^ for Kac-Moody Algebras

Proof. Set M := ad uCg^)// ^ Froni ad = 0 for all A: e K and ad /t(/¿)= —{a¿,h)f¿, we see that M is a highest weight module with highest weight pair ( —a¿,f¿). To show that c M , we consider any -a¿ - a e A, a e and prove that g““'" “ c M. Certainly a e (Q k ^ Q- ) U {0}. Thus every element of g“"'“" is expressible as a linear combina­ tion of elementary words F = [ f , f j , where . . . , ^ {0 U K and i occurs exactly once in each of these elementary words. However, if i = ip then ^ ^ [//,’ •••’ [fij+i’ [fi’

***]

- -ad/,,...a


We use Proposition 4 to obtain a characterization of P(L) for an inte­ grable highest weight module L. Let g be a Kac-Moody algebra with structure matrix A, and let L be an integrable highest weight module of highest weight A e In determining P(L), we can suppose that L = L(A) because of the Corollary to Proposition 2. By Proposition 3, rad(g)L(A) = (0), so we can suppose that g = of A, R) is radical free. We now carry out an extension trick that allows us to view P(L) as a set of roots of a Lie algebra. Increase J by adjoining a single element /; let j == J U {/}. Define a matrix A = (A¿jX i, ; e J by

Ai¿ = < - A, G Z^o for all i e J, A¿i arbitrary in Z < q subject to ^4/^ = 0 An = 2.

' A ¿I = 0 for all i e J,

Then ^ is a Cartan matrix, and ^ is a submatrix. If A is symmetrized by {e¿}, then Á will be symmetrizable if we set Án = A^Si for each i e J. Now extend to a realization R = (§, H, of Á in which R embeds compatibly with the inclusion J ^ j. Then we can view g(^4, R) as a subalgebra of qf Á , R) (Proposition 4.3.5). Denote g (^ , i?) by g, and let J + § = 9 + § = 9 + § c g. According to Proposition 4, M_is an integrable gj-module of highest weight —a^ Restricted to g, it is then an integrable highest weight module of highest weight A [since —<«/, a f ) = - Á n = (A, a f ) ] and is generated by f¡. The weights of are the roots of g of the form -Ui - 'Lj^jCjUj, Cj e [\1. Let A e 1^*. Let A e A J, ¡2+? and write A = A —a

6.2

Weight Systems

for some a e Q+u{0}. Let supp(a) (Section 5.8), and write “ =

513

be the connected components of

L “ 5,> / = 1, m

where supp(a^) = 5^. We say that A is connected through A if either A = A, or for each \ < i < m there exists some j = ;(0 ^ such that =5^=0. If A = A - a, as above, is connected through A and one draws a diagram of supp(a), then all the connected components of supp(a) are connected to each other “through” A

Proposition 5 [Ka5] Let L be an integrable highest weight module with highest weight pair (A, u+). (0 Every weight o f L is connected through A. (ii) I f k ^ P +n(A i Q^X then A e P(L) if and only if A is connected through A. Proof (i) Suppose (i) does not hold. Then there exists a weight A of minimal depth for which part (i) fails. By Remark 1 there exists a e j2+u{0} and y e J such that A = A - a and A — a ^ P(L). Because of the minimal­ ity of A, the weight A —a is connected through A. Thus aj ^ supp(a), {a, a ^ ) = 0, and = 0. Therefore
= 0 and a - aj ^ ¡2+. Hence A - a + Qfy ^ P(L), and by Proposition 1(0 it follows that A = A - a - ay ^ P(L), a contradiction. (ii) By the extension trick we may take L = in some Lie algebra g = 9j, where j = J U {/} and L certainly have the same weights even if they are not isomorphic g-modules. All the weights of lie in - ai - (j2 +L^{0}X We show that if a e -a ^ - (2+, { a ^ a ^ ) > 0 for all y e J (a is dominant relative to J), a is connected through -a^ , and if we choose the extended Cartan matrix A appropriately then a is a root of §. In that case a e by Proposition 4(iii). “Connected through - a ^ ” is

Category ^ for Kac-Moody Algebras

514

equivalent to saying that supp(o:) is connected. By Theorem 5.8.6 we will be done if we show that a is dominant relative to J (then —a e F). Let a = —a i ~ ^ Now (a , a / > = —2 —'LcjAji, and by assumption CjAji 0 for at^ least one j e J. Since the Aji can be chosen freely, we can assume that Aji = - 2 for each j ¥= /, for which Aji ^ 0. Then (a, a / > > 0, which is what we want. □ A subset 5 of the weight lattice P is said to be saturated if it satisfies the following condition: SAT: If A - S, a \ - ka : 5.

®A, and k is an integer between 0 and , then

If A e 5 as above and a e then r^(A) = A -
Given a positive integer d let P( M) a == {a e P( M) \ d i m^ P ( M) ^ rel="nofollow"> d).

Then P{M)^ is a saturated set. In particular P{M) = P{M)^ is saturated. Proof. The proof follows from Proposition 1.



Proposition 7 Let A e

The following sets are equal:

(i) (ITA> n (A + <2X y^here (ITA> denotes the convex hull o f WK. (ii) The weight system P(A) of L(A). (iii) The smallest saturated subset 5(A) o fP containing A. Proof (i) c (ii) Let A e n (A + Q). Then A = "L^^^^c^wA with > 0 and = 1. Thus A —A = 'Ly^^цrcJ^A — wA) e (2 +Li{0} since A wA e j2+u{0} and A — X ^ Q. Since <^A> n (A + 0 ) and P(A) are both IT-invariant, there is no loss of generality in assuming that A is chosen in its IT-orbit so that djfX) is minimal, or equivalently, so that A e P_^. Finally, A = H^^iyC^wA is connected through A since wA is connected through A for every w e IT. By Proposition 5(ii), A e P(A). (ii) c (iii) Let 5(A) be the intersection of all saturated subsets of P containing A. It is clear that 5(A) is saturated, it contains A, and is the smallest subset of P with these properties. By Proposition 6, 5(A) c P(A).

6.2

Weight Systems

515

Suppose that 5(A) P(A), and choose A e P(A) \ 5(A) so that d ^ k ) is minimal. Since A e 5(A) by definition, A =5^ A. By Remark 1 there exists ; J such that A + ofy e P(A). Let d — u = (A, a^) be as in Proposition 1. Then u > 1 and A + uaj 5(A) because of the minimality of d^(A). Then A + « a j u+ a / >. Since
= ta: 5(A) for all 0 < t < w, A e 5(A). This contradiction shows that 5(A) = P(A), as desired. (iii) c (i) It is clear that n (A + ¡2) is saturated because of convex­ ity, and that it contains A. Thus 5(A) c (WA) n (A + Q). □ Proposition 8 Let A G

and let A e P(A). Then for all ¡jl e (WX)

n (A + Q),

dim L( A)^ > dim L(A)"^

Proof Without loss of generality, we may assume that A e P_^_, Let dimL(A)'^ = d. The set P(A)¿ of weights of multiplicity > d is saturated. (Proposition 6), and it contains A. By Proposition 7, applied to A, {WX) n (A + 0 = (WX) n (A + ¡2) is the smallest saturated subset of P containing A. Thus n (A + G) c P(A)^. □ Proposition 9 Suppose that ( q, ¿s an invariant Kac-Moody algebra and let (*| * ) be a standard invariant bilinear form on 1^*. Let A e Then for all X, p ^ P(A) we have (A|/x) < (A|A) with equality if and only if X = p ^ WA. Proof Using The IT-invariance of ( | • ) we can assume that A e A = A - a and p = A — p where a, p ^ Q + u{0}. Then

Write

(X\p) = (AIA) - (A la) - (A|i8) < (A|A) since (A|a) > 0 and (X\p) > 0. Suppose that we have equality. Then (Ala) = 0 = (A|j8). Now A e P(A) and so A is connected through A. But this means that (Ala) = 0 if and only if a = 0. Thus A = A and now a similar argument gives p = 0. The result follows. □

Category ^ for Kac-Moody Algebras

516

63

THE TRIANGULAR DECOMPOSITION OF G

The derived Lie group G associated with g has remarkable pair of decompo­ sition over the Weyl group W called the Bruhat and Birkhoff decompositions. The latter gives us something resembling a triangular decomposition: G = U ^^цrG_wHG+, and this decomposition is essential for proving the conjugacy theorems in Chapter 7. Both decompositions follow readily from the fact that G can be realized as a Tits system or (B, A/^)-pair. This immediately associates it with a large class of groups that are of this type and for which an abstract chanpiber geometry exists. The theory of buildings, as these chamber geometries are called, and (B, A/^)-pairs was developed by J. Tits [Til, Ti7] in order to provide an abstract geometric scheme in which one could study all the simple (finite-dimensional) Lie groups in a uniform way and over arbi­ trary fields. In this section we prove that G can be realized as a Tits system and exhibit the triangular decomposition. The exposition follows [PK]. The first results of this type for the infinite case are in [MoT]. Throughout this section (g, denotes a Kac-Moody Lie algebra over K. We write ^ = (if, g+, Q+, o r ) as usual. Let P be a weight lattice of (g, ^ ) . All the standard notation previously employed is in use. Let G := G(P) be the derived Lie group of g with respect to P. We recall some important subgroups of G that have already been defined G“ := expg«, a G + :=
t e IK=^),

H--={h^{t)\a e"A , i e IK^). Remark 1 The groups G “ are often called one-parameter groups in the literature on Chevalley groups and are usually denoted by t/“. Lemma 1 Let a, p e^'^A. Then G“ n G^ = {1} whenever a # jS. Proof, Suppose that a p and that z e G" n G^, z ¥= 1, Then there exists X e g“ and y ^ g^ such that exp x = z = exp y, x ,y ¥= 0. Thus exp ad X = Ad exp x = Ad exp y = exp ad y . Since X = expad x (x ) = expad y (x ) = x + [y, x] +

6.3

The Triangular Decomposition of G

517

and (ad y T x g we conclude that [x, y] = 0. Thus [ad jc,ad y] = ad[jc, y] = 0, and hence 1 = exp(ad jc)exp( —ad y) = exp(ad jc —ad y) = exp ad(x: —y). Choose h

with a(h) ^ ¡3(h), Then for all f g IK,

h = exp(ad t( x —y ) ) h = /i + t[x — y, h] + + •••

ad(x —y)^ ------r:------ h 2!

2iá(x-yY --------— h nl

for some n independent of t. This can be true for all t if and only if [x - y,h] = 0. Thus a(h) = contrary to the choice of h. □ Define (resp. 5 _ ) to be the subgroup of G generated by H and G+ (respectively H and G_). Lemma 2 (i)

H normalizes G"" for all a g In particular H normalizes G+ and G_. (ii) H • G^ and B_= H G_, H n G+= {!}, H n G _= {!}. (iii) B ^ n N = H = B_ DN, Proof. Let G g“, a g '^^A. Then for all p g '’^A and i g [Proposition 6.1.14(iii)]

we have

h p ( t ) e x p x ^ h p ( t y ^ = exp{Ad hp(t )x^)

This shows that H normalizes G", G+, and G_, and also that G+ is a normal subgroup of A typical element of G +n / / is of the form exp(xi) • • • exp(x„) = h y t i ) • • • / t J i J , where x¡ e g^', /3, and y, e''^A. Given any integrable module M and any weight vector v e M'^, we have expixj) • • • exp(x^) • v = v + v', where u' G On the Other hand (Proposition 6.1.8),

¿=1

Category ^ for Kac-Moody Algebras

518

Combining these two, we see that • • • hy(t^) acts like the identity on M. From Section 6.1, Remark 1, we have = I q , proving that G +n / / = {1}. Similarly G_D H = {1}. Clearly H (zB+n N. Also G+n N = {1}. Indeed, if p e F+ is an integral minimal regular weight and is a highest weight vector for L(p), then G +*u^= u^, whereas n • +c L(p)^"^^ for n ^ N. But [n\p = p <=> [nj = 1 ^ D N ' =>x = /ix+e N, ^ n ^ Thus G +n N = G + n H = {1}. Now x e B B+n N. Then jc+= 1 and x ^ H. where h ^ H and x , ^ G , , and hence x. □ Similarly for B _n N. Often we denote B+ simply by B. This group is called the Borel group of (g, Recall that if x and y are two elements of a group K then (x, y) ’= xyx~^y~^ is called the commutator of x and y. If and A2 are subgroups of K, then we will denote by (^1,^42) the subgroup of K generated by all commutators (^i, a^) with e A^, i = 1,2. Lemma 3 Let a,

be such that (a,

> 0. Then

(i) (Na + Np) n (A \ {0}) = {a, p ,a + p) n""A,

Proof, (i) Let y = m a +

e A, m, n e I\l. Then

( r , P ^ ) = m( a , P ^y + 2n > 2n > n, which shows that the p-ioot string through y contains y — np = ma (see Section 6.2). Since a e^’^A, we have m < 1. Since (a^p"^) > 0 <=> { p , a ^ y > 0 (Proposition 5.2.8), we have similarly n < 1, and hence y e {a, )8, a + p}. The above argument shows that 2y ^ A. Thus y e'^^A (corollary to Theorem 5.8.6). (ii) Let X e g", y e g^. Then by Proposition 6.1.14, exp X exp y(exp jc)” \e x p y)~^ = exp((Adexp x )(y ))(ex p y) \ Now by part (i). (A d ex p x )(y ) = y + [x ,y ]

6.3

The Triangular Decomposition of G

519

and [y +

[ x , y ] , y] =

0.

Thus (exp jc, exp y) =

exp(y + [x ,y ])(e x p y ) ^

if a + j8 e'^^A,

expy(expy)"^

ifa + )8 ^ " " A ,

exp[x, y] 1

if a + /3



For more on pairs of real roots see [BP2] Remark 2 In the sequel we have many occasions to write down sets that involve elements from the subgroup N, for instance, BnB, n ^ N. Often such sets depend only on n mod H, that is, on [nj e W. For instance, if A e //, then BnB = BnhB, so BnB depends only on nH = [nj. If [nj = iv, it is then convenient, and standard, to replace « by w in the expression. Thus we write BwB even though w ^ G . \ i both n and n~^ occur in this expression, then the convention is to replace n h y w and n~^ by In other words, one must understand that and stand for elements of N that are inverses of one another. For instance, we will write rJ3^r~^ meaning We will use these conventions without further comment throughout the rest of the book. For each a e II define a subgroup y of G+ by 7 “ :=

e G", y e G ^ p e^^AA{«}>.

We note that for p e '^^A+\{a} c Y“,

(1) since '■= r^cxp and r„(A+\{a)) = A+\{a). Proposition 4 For all a ^ Yl we have (i) SL^2^ normalizes 7 “, (ii) G^= G^ Y ^,G ^ (iii) Y“ = G + n r„ G + r;i.

= {!},

^ = exp g'"«^

Category ^ for Kac-Moody Algebras

520

Proof, (i) By Proposition 2.4.5, SL2(K) has a Bruhat decomposition. By Proposition 6.1.7, SLjClK) = by a map with

"’( J

! ) -

expie^

5 ) = e x p t/„ where [e^, a /^} is some fixed, but otherwise arbitrary, ^ 12-triplet for Combining these two results. ( 2)

5L<2“ ^ =

U

where 5(“) := / / “G “, / / “ == {/i„(0k e IK''}, and = }n„(0J = [exp exp - i “ exp re„J [see Proposition 2.4.9]. Now Y “ is clearly normalized by H and G “, hence Thus we need only show that y a

ot

- 1

(- y a

ct

For this we need only show that for all x e G “, for all /3 e''®A \ {a}, r„x G ^x -V -i c y “. If ( a , /3 '') > 0 then from Lemma 3, (3)

x G ^ x 'i c G“+^G^ c 7 “.

In fact from (1) and (2) we may deduce that (3) holds for all x e SL^2^ (still assuming that < 0, then

= x 'G ''« ^ (x ')'‘ c 7 “ from (3) since x' g 5L^2^^ and 0 . This proves (i). (ii) y " is normalized by G“, and hence G ^y" is a subgroup of G^.. Since it contains the generators of G+, it is G+. We show that G" n y “ = {!}. Elements of G^ act trivially on the highest vector of any integrable

6.3

The Triangular Decomposition of G

521

representation L(A). However, if A e is chosen with 0, then [r„](expie„)fr„]~^ = exp tf^ e G ““ for some r e K, and this does not fix v+ if s # 0. Thus e G “ \{1} => i G+=> € 7 “ ^ X ^ 7 “. (iii) Let g e G+, and write g = xy when x e G“, y e y". Then using (1) \fa]g\ra]_ ^ ''al3'r''al ' ^ SinCC G “ € G +, ^ if and only if X = 1. Thus <x+nfr„]G +fr„]~‘ c 7 “. The reverse inclusion is obvious from (1). □ Let 5 := { r j a e II}. Proposition 5 (G, B, N, S) is a Tits system (see [Ti3] and [Soi]). By definition this means that TSl: G is generated by B and N and B N < N, TS2: The elements o f S are of order 2 and S generates the group W == N /B n N, TS3: For all s ^ S and w ^ W, sBw c BwB U BswB, TS4: For all s ^ S, sBs
e A+: Then sBw = sHG“Y “w = sY “G“Hw = sY^ssG^^ww-^Hw c Y ‘‘sG°‘wH = Y “swG”'~'“H c BswB.

Category ^ for Kac-Moody Algebras

522

Case 2.

e A_: Then (sw)~^a = w~^r^a = -w ~ ^a e

Now sBs = sHs-^sG^s-^sY^s-^

c B u BsB by (2). Thus sBw =

5B55IV

c Bsw

U

c

(B

BsB)sw

U

BsBsw

c BswB U BsswB

(by case 1)

= BwB U BswB.

TS4: sG°"s = G “

B; hence sBs € B.



In the main result we go back to the original notation and use B+ instead of B. Proposition 6 (The triangular decomposition of G) G=

U B_wB^

{disjoint union).

In particular G = G_NGj^. Proof. Evidently the right-hand side is closed under right multiplication by elements of B+. We show that it is also closed by right multiplication by elements of N. Then, since G =
6.3

The Triangular Decomposition of G

523

Case 2. wa ^ A^_: Then wsa e A_, and B_wB+s = B_wssB^s c B_ws{B^yj B ^sB ^)

(byTS3)

c B_wsB^\J B_wsB^sB^ c B_wsB^\J B_wB+

(by Case 1).

It remains to prove that the union is disjoint. Now any two (B_,B+)-double cosets are either equal or disjoint. Consider B_wB^. Let L(p) be the representation appearing in the proof of Lemma 2(iii), and let be a highest weight vector of Lip). Then B _ w B B _ i n v ^ ) , where [n\ = w. We have nv +^Lip)"^^ and B_nv +(z K^nu +-\since this last set is stable under G “, a e'^^A_, and H. Evidently, if B_wB^= B_w'B^, we must have wp = w'p, and hence w = w'. □ This decomposition is also called the Birkhoff decomposition. We leave it as an exercise to prove the following analogous result. Proposition 7 (Bruhat decomposition) G = U BwB

{disjoint union).

In particular G = G+A^G^ Recall the group G — G(AT, P) of Section 6.1. We finish this section by taking a closer look at the centers Z(G) and Z(G) of G and G, respectively. Proposition 8 Let (g, ^ ) be a Kac-Moody Lie algebra and Ad: G

GL(g)

the adjoint representation o f its derived group. Then (i) k e rA d c Z(G) (ii) ker Ad = Z{G) if Q is radical free. Proof. Let g ^ G, and let 5 — {jc e g“|a e'^^A}. Then g e Z (G ) <=>g exp xg~^ = exp x <=> exp(Ad g (x )) = exp x Ad g (x ) = X

for all x e 5 for all x e 5 [Proposition 6.1.14(iii)]

for all X e 5 [Proposition 6.1.14(ii)].

524

Categoiy á for Kac-Moody Algebras

This establishes part (i). It also shows that if g e Z(G), then Ad g pointwise fixes Dg. Part (ii) will follow once we establish that (4)

(rad(g) = (0)

and

g e Z(G)} => Ad g (h ) = /i

for all

We begin with two preliminary steps. S t e p 1. Let A e e e {ej]j^j. Then v g

and let v

e

L(A) be such that exp v(e)v = v for all

We may assume v ^ 0 and write y = Uj + • • • + % , where v¡ e L(A)'^“ '*''\{0} and y, < jj ^ i < j. From exp 7t( x ) í; = d we conclude that

Tr(e)vi H

Tr(e)Vi —------ h • • • +v{e)Vfj +

=

2!

0.

Now v(e)v¡^ G L(A)^~‘>''^'^“ for some a g n , and no other term in the finite sum above contributes to the weight space in question. Thus Tr(e)vj^ = 0 and hence g (Ku^ since L(A) is irreducible. It also follows that y^^f = 0 and hence that N = 1. S t e p 2. Let A G P_^. I f g e Z(G), then g acts on (L(A), ir) as a nonzero scalar. Indeed let

e G

[e¡\j^y Then

'»»■(g)y+= Tr(g)exp'ir(e)i;+= ■rr(g)'ir exp(e)t;+ = Tr(g exp(e))ü+= ^ (e x p íc )^ )^ ^ = exp'n-(c)'ir(g)í;+. By Step 1 ir(g)i;^e The rest is clear. We now move to the proof of (4) above. Let /1 g 1^. By (6.14) for all V G L(A), ■Tr(Ad g{h ))v = Tr(g)Tr(h)tr(g~^)v. By Step 2, if A

G

P^ and u

g

L(A)^, then

ir(g )T r(/i)ir(g “ ‘)i; = ( p , h ) v . It follows that Ad g(h) - h annihilates L(A) for all A gih) = h [Proposition 2.7.5(vi)].

g

P^. Thus Ad □

6.3

The Triangular Decomposition of G

525

Proposition 9 Let J c J', and let A c be a subCartan matrix o f the Cartan matrix A e . Let R = (1^, П, П ^), and R' = (1^', П', П' be realizations of A and A respectively, and let т/ = (17^, 7]¡f): R ^ R be an embedding o f realiza­ tions. Consider the Kac-Moody algebras g = д(Л, R) and g' = q'(A \ R ) with their canonical triangular decompositions. Let P' c be a weight lattice and let 17^: ]^'* ^ be the transpose map o f 77^. Then (i) P ’= ri%iP') c ]^* has the structure o f a weight lattice in a natural way, (ii) there exists a canonical homomorphism t|: Gp -> Gp, and furthermore t|((Gp)+) c (Gp/)+ (We will see in Proposition 6.3.13 that t| is an injection). Proof We maintain the notation of the definition of embedding in Sec­ tion 4.3. Let < * , ‘ ):]^ * X ]^ ^ IK b e the natural pairing. (i) P is a subgroup of Í)*, We check the axioms of weight lattices: WLl: Let i e J. For ft e

we have

= {a¡,h}, and hence a, = r,%U'i). Since Q' c P', we conclude that Q
= {P’,r)¡,Q^) cz{P', Q:^ ) czZ. WL3: If p is a minimal regular weight of P', then for all i e J, <77*р',а,"> = < р ',аГ > = 1. Thus rjj^p is a minimal regular weight of P. WL4: Let Í1 = {(o'j\j e j'} be a fundamental set of weights in P'. For У e J define o)j == Then for all i e J,

= {<о),г)цаУ) =

= Sj¿.

Categoiy ^ for Kac-Moody Algebras

526

(ii) Let A and A' be the root systems of g and g', respectively: G =

* g'“

G — * q“ A

K p f ^ C \ ker TT, tt' a representation of g' in Kp = C\ ker TT, 'fr a representation of g in ^ { P ) . By definition Gpf = G/Kp, and Gp = G/Kp. By Proposition 4.3.2 we have a natural homomorphism tj: G —> Gpr, If M is a g'-module and we view M as a g-module via the injection g ^ g', then for all A e 1^'*, v e M^, and h we have h ' v '= r]p(hXv) = (\,7]p(h))v = (7]%(XXh)v, This shows that the representations of g' in restrict to representations of g in cX(P). It is clear therefore that ker Kp and hence that there exists an induced homomorphism Ti: Gp

Gpr.

Finally it is clear that ti(G p)^c (Gpd+-



Proposition 10 Let (g, be a Kac-Moody Lie algebra and let Ad: G GL(g) be the adjoint representation of its derived group. Then the restriction o f Ad to G^ is injective. Proof. First assume that J is a finite set. Let ( tt, M ) be any integrable g-representation, and let v e be any weight vector in M. Let F := ir ( U ( g ^ ) ) i;=

0 /i, e A + ( ( 2 + { 0 } )

and let L «ee+u{o) ht(o:)>;t

k = 0 ,1 ,2 ,... .

Thus K == Kg D Fi 3 F2 D • • • is a filtration of V by g^.-submodules. Let V ) := V/Vj^. Then fs a finite-dimensional Q-gi&d&A g+-module with Jc e g^ acting as the endomorphism m + F* ■rr(,x)u + V^. Fur­ thermore the natural maps 9^: y W are g+-module maps.

6.3

The Triangular Decomposition of G

527

The endomorphisms of determined by U(g^) form an associative algebra = K1 e where is a nilpotent ideal of (since elements of increase the Z-degree each time they operate on Now 7T determines a representation tt of G and hence by restriction a representation ir of G_^. We fix some element g^= exp • • • exp g G+, where Xj e /3^ ; = 1 ,..., r. We are going to show that if Ad g+ = 1, then ^г(g_^_)v = V as well, and hence 'rr(g+) = 1 for all integrable repre­ sentations ( tt, M), whence 1. First, acts on as exp x^^^ • • *exp and since g we may use the Campbell-Baker-Hausdorif formula to write this as exp(y^) for some G of the form (5)

yk = -^1^^ + • *• +x^^^ -h 51 [

+ higher commutators

i< j

(see Section 7.2 for a more detailed explanation of this). The important facts are these: 1. Equation (5) has only finitely many terms that do not vanish. 2. The structure of the terms depends only on the Campbell-BakerHausdorff formula (applied to r exponentials). 3. Consequently ^Ar+iiy^t+i) = yk for all k. 4. There exist elements z . g E,0<;<*9i such that z i ’‘^ = y ^ , k = 0 ,1 ,2 ,..., and such that = z*.+i modEhtaaA:9i- In fact we may define z ^ ~ x ^ + ■■• +x^ + £,
(4)

Let us suppose that some ^k

^ 0 and that ^n,k

^n-\-l yk

^n+s/cy ^ ’

where has degree ; in the Z-grading of and 0. (Of course n > 0.) Then we observe that n < k and =■ is independent of k (for k > n). From (4) we see that [a„,q] = 0.

Category á for Kac-Moody Algebras

528

But this is true for all q ^ and hence lies in the centre Zg. But Zg c gQ, whereas ^ n > 0. Thus = 0, and this contradiction proves that = 0. Now fact 4 above shows that = 0 hence that Tr(g+)u = u, which is what we wanted. If J is infinite, we denote J, g, and G by J', g', and G' consistent with previous notation. Let = exp . . . , exp x„ e G'+; x¿ e g'^' be such that Ad = 1. Find a finite subset J of J' so that ..., belong to the root system of the subalgebra g=

e

© g“, a^Q

where Q •= the last proposition we have a group homomor­ phism ti: G ^ G', where G is the group attached to g. It is clear that has a pre-image g+ in G+. By assumption Adg. t|g+ acts trivially on g' and a fortiori on T7g. Thus Adg g+= 1 e Ad(G). By the finite case g+= 1, and hence g+ = 1. □ Let g ^ G, and let (M, tt) be an integrable representation of g. Then Tr(g) e G L( M ) c E n d (M ). From Section 1.3 we recall that irCg) is homogeneous (of degree 0) if

for all A e 1^*. We say that g is homogeneous (of degree 0) if Tr(g) is homogeneous of degree 0 for every integrable representation (M, tt) of g. Examples of homogeneous elements are those of H and X, Lemma 11

Let (g, 0) e Z(G). Then (g, 6) is homogeneous. Proof Let (M, tt) be an integrable representation of g, and let v e M^. For all AT A r(A )T r(g ,0 )i; = Tr(g,0)Ar(A)¿;

= Tr(g,0)(Tr(l,Ar)i^) = Tr((g,0)(l,Ar))i^ = ir(l,A :)(T r(g,0)i;). Thus, if w := '7r(g, d)v, then w satisfies the equation = Af(A)iv

for all x

6.3

The Triangular Decomposition of G

This forces w e M^. Indeed write w = •••j are distinct. Then At(A)w =

ir{l,x)w

+ • ♦•

= Ar(Ai)Wi + • • • + x

529

where

e M^‘ and

{^n )^n -

Thus ;^(A) = = • • • = x (^ n ^ for x^ ^ind hence N = 1 and Aj = A (since Z is a separating group of characters). □ Proposition 12 Let p be a minimal regular integral weight in P. For g ^ G the following conditions are equivalent: (0 g ^ H . (ii) g acts homogeneously (o f degree 0) on (g, Ad) and L(p). (iii) g is homogeneous. Proof (0 => (iii) and (iii) => (ii) are obvious. (ii) => (i) Let g ^ G, and using the Bruhat decomposition, write g = binb2 with b2 ^ B, n ^ N. Let p be a minimal regular integral weight, and let (p, i^+) be a highest weight pair for L(p). Then g-v^^K ^b,n-v^^L {py'"'’ +

i:

since nL (p y (Z and e B. Furthermore g - v ^ has a nonzero component in L(p)^"^^. Thus, if g acts homogeneously on L(p), then g • +e L ( py , and hence [n\p = p. Since Stab^(p) = 1 (see Corollary to Proposition 4.2.5), [n\ = 1 and we have g ^ B = G+H. Write g = g^h with g + e G+, h ^ H, and apply Ad to obtain Ad g = Ad g+ Ad h. Since Ad h is homogeneous, and we further assume that Ad g is homogeneous, then Ad g+ is homogeneous. But Ad g+ acts on g as a unipotent transformation, and hence Ad g^= 1. By Proposition 10, g+= 1, and hence g = h ^ H. □ Corollary G C ) X c : H , a n d G / G ^ X / X n H. Proof The elements of X are homogeneous. Use now Proposition 6.1.15. □ Proposition 13 Let the notation be as in Proposition 9. The natural homomorphism T|: Gp is injective.

530

Category ^ for Kac-Moody Algebras

Proof. Let g e Gp be such that t|g = 1. The explicit construction of P, il, p, and r\ in Proposition 9 show that g acts trivially on (ad, g) and L(p). [Note that the highest weight vector of L(p') generates an integrable module of highest weight p for g. Both g and Gp act on its irreducible quotient, which is Lip), and g acts trivially on it.] By the last proposition g ^ H, and hence by Corollary 6.1.8(ii)

Since r\g acts trivially on L(a>}) the same argument as above shows that g acts trivially on L((Oj). Thus tj = 1 for all j ^ J {ibid.). Thus g = 1. □ Theorem 14 Let {%, ^ ) be a Kac-Moody Lie algebra. (i) I f P is a restricted weight lattice, then the center Z{G) o f G is given by Z ( G ) = X q : ={ x ^ X \ x (Q) = 1}. GO If g is radical free and P is any weight lattice, then Z (G ) = ( n /ia X i,)|

= 1

for all] e j \ c ii.

Proof, (i) It is clear from (6.1.12) that X q c Z(G). Conversely, assume that (g, d) e Z(G). By Lemma 11, (g, 6) = (g, 1)(1,6) = g$ is homogeneous, and hence g is homogeneous. Thus g ^ H (Proposition 12), and we can write S = Y lhaiti)

By Remark 6.1.7, in G

and it is easy to see that (1, x) ^ Z(G) x ^ ^ q(ii) If g = with = 1> then A d g fixes 1^, all fj, and all Cj, j e J, and hence Ad g = 1. Thus g e Z(G) [Proposition 8(0]. Conversely, if g e Z(G), then g acts like a scalar on Lip) and (g,Ad) [Proposition 8(ii) and Step 2 of its proof]. By Proposition 12 we conclude that g G i/. If we write g = n , ej/ia(t,), then Ad g = 1 clearly forces n , eJ “<''> = 1 for all y G J. ' □

6.4

The Formulas of Weyl-MacDonald-Kac

531

Corollary Let be a minimally realized finitely displayed Kac-Moody Lie algebra with structure matrix A, Let G and G be its group and derived group. Assume det(A) ^ 0. Then (i) (ii) (iii) (iv)

G = G, P /Q Is a finite abelian group o f order |det(^)|, Z(G) is a finite group and |Z (G )| | ldet(^)l, Z(G) P /Q if IK contains all \dti{A)Vroots unity.

Proposition 15 Suppose that (g, ¿s radical free. Let P^ and P2 be any two weight lattices, and let Gj and G2 be the corresponding groups. Then G1 — G2 by the canonical isomorphism that sends exp x exp x /o r a//x e g", a Proof Suppose that P^ d P2. Then by the definition of G,, i = 1,2, we have a surjective homomorphism il/: G^ G2, exp x ^ exp x for all jc e g“, a e'^^A. Furthermore we clearly have e/i ° Ad = Ad° (/r. Now, if g e ker ij/, then Ad(g) = Ad(il/(g)) = 1, and hence by Propo­ sition 8(ii) and Theorem 14(ii), g e Z(G) c H and g = Uh^it^) uniquely. Let j e J, and let (Oj e P2 be a fundamental weight. Then L((Oj) e ^ ( P 2\ so il/(g) acts trivially on L(o)j). But (/r(n/z^(/)) acts as / on L{o)jYK Thus tj = 1, and finally g = 1. Now taking P' to be the standard weight lattice, we obtain in general Gp — Gp> — Gp , all isomorphisms being the obvious ones. □ 6.4

THE FORMULAS OF WEYL-MACDONALD-KAC

The rules are tricky, but they are a much more efficient way of getting the answer than by counting beans. — R. Feynman, QED.

Throughout this section g will denote an invariant Kac-Moody algebra with triangular decomposition and standard invariant bilinear form (• I *). Our object is to prove the beautiful formula for the character of L(A), A e P^. This formula, which expresses ch L(A) as the ratio of two WP^-skew-invariant expressions, immediately gives an auxilliary formula called the denominator formula, which relates W and the root multiplicities of g. As a bonus we obtain the important fact that L ^ J ^ h ) = L(A) for all A e P^\ in other words, L^J^K ) is already irreducible. Recall the ring Z[P I Q which we defined in Section 2.5. In the present context P is a weight lattice (see Section 6.1) of (g, ^ ) , and ¡2+ is the usual positive cone in the root lattice. A typical element of I{P iQ+] is a formal

Category ^ for Kac-Moody Algebras

532

sum / = Em^eCa) whose support lies in a finite number of (2+-fans. Given w E:W [the Weyl group of (g, we have wP = P. Therefore we can define wf = Y^m^e{wa)

e Z [P]^ .

Unfortunately, even if / ^ Z[P i 0+], iv/ need not. However, as we will see, the set

is nontrivial and is clearly a subring of Z[P i 2+]. Evidently W acts as a group of automorphisms on Z ^[F i 2+] and hence also on its field of fractions i 2+)An element / of Qw/(P i 2 + ) is PT-invariant if ^ii w ^ W , An element of / of

J. 2 + ) is W^-skew-invariant if h/ =

fo rall* v e» F

(recall that the map W ^ {± \], w ^ ( —1)'^*^^ is a homomorphism). The simplest example of a IT-skew-invariant is the sum (1)

D := £ ( - l ) ^ ' ^ ’e(wp), w^W

where p ^ is given by WL4 of Section 6.1. [Equation (1) depends on p although this dependence wilt not be indicated]. By Proposition 5.2.5 wp = p - <5^> e p i 2 + , so indeed the sum (1) lies in Z[p 4 2+1 ^ Z[P i 2+1* Note that all the formal exponentials occurring as summands in D are distinct; see Corollary to Proposition 5.2. D appears as the denominator of the character formula. Theorem 1 (Weyl-Kac character formula; [Wy2], [Ka2], [Ka3]) Let g be an invariant Kac-Moody algebra, let P be a weight lattice o f (g, and let A e Let L be any integrable highest weight module with highest

6.4

The Formulas of Weyl-MacDonald-Kac

533

weight A. Then

ch L

I (-l)«*^>e(H;(A + p)) w^W___________________ e{p) n (l-ei-a))**“"«“ ae A+

This formula expresses ch L(A) as an element of are actually W^-skew-invariant expressions.

i Q^.]. Both of these

Corollary 1 (Weyl-Macdonald denominator formula, [Wy2], [Mac])

Z)==

E

i-lf'^^e{wp)=e{p) n

( l - e ( - a ) f " ’«“

Proof of Corollary. It is obvious that L(0) is a one-dimensional module [use Proposition 6.1.5(iii)] whose character is e(0). Since c(0) is the identity element of Z[P J, Q+], the result follows at once from the theorem. □ Theorem 2 Let g be an invariant Kac-Moody Lie algebra. Then for all A e Lmax(^) = LUO. In particular there is, up to isomorphism, only one integrable highest weight module with highest weight A. Proof. The character formula is identical for L ^^{A ) and L(A); that is, dim L„,3x(A)^ = dim L { K Y for all weights p. But L(A) is a homomorphic image of L ^ ^ { K \ and under such a homomorphism L ^ J ^ K Y L(AY- It follows that the homomorphism is injective; hence L^^J^A) = L(A). □ Theorem 3 Let g be an invariant Kac-Moody Lie algebra over C. For all A e the hermitian Shapovalov form < • 1• > on L(A) is positive definite. In fact, given A e ]^*, the hermitian Shapovalov form on L(A) is positive definite if and only ifA ^P ,. Proof. Using the extension trick of Section 6.2, we embed g in an invariant Lie algebra g by adjoining new generators Cf and // (and by making some appropriate extension § of 1^) so that under the adjoint representation of g

Category ^ for Kac-Moody Algebras

534

restricted to g, // generates an integrable highest weight module with highest weight A. By Theorem 2 this is none other than L(A). Now we know that § carries a positive definite hermitian contragredient form < • I * > that is nondegenerate on all root spaces a ¥= 0. Since L(A) = ©g“, summed over those a e A of the form -a ¡ + •**,<* I • ) restricted to L(A) is positive definite hermitian and contragredient. It follows that it is a multiple of the hermitian Shapovalov form, say, c< • 1• >sh- But then c = ifi\fi) > 0 [assuming that we use f¡ as the generator of L(A) in defining the Shapovalov form, so sh = 1], and we are done. Now suppose that A © f)* and that the hermitian Shapovalov form < • I • ) on L(A) is positive definite. Let be a highest vector of L(A). Then for all ; e J and for all n © Z+,

Now

' fp •

n«A , a ^ ) — n

l)/y"

(see Section 2.4.), and hence

J=0

> 0.

This result is possible for all n only if = k for some A: > 0. Thus A ejP + . □ Remark 1 The result of Theorem 3 is usually stated by saying that for all A e P^, L(A) is unitarizable. We now set about proving Theorem 1. Lemma 4 Let XyfjL © P, and suppose that A, /x + p e

and that p, © A —(2+. Then

(A|A + 2p) > (p ip + 2p).

Proof. Write p = A —a,

Then

(A|A + 2p) - (p ip + 2p) = (A + p|A + p) - (p + pip + p) = (A + p|A + p) — (A + p —a|A + p —a) = (A + p |a) + ( a |p + p) > 0



6.4

The Formulas of Weyl-MacDonald-Kac

535

Lemma 5 /:=

“ e( —

is W-skew-inuariant.

Proof, It suffices to show that for each reflection r¿ = n f = - / . Now r if = e{r¿p) n

, i e J, we have

(1

= e(p - a,)(l - e (a ,))

O

(1 - e(-a))'*""® ”

a e A+\{a/}

by Lemma 5.2.1 and the definition of p. Since e(p —a^)(l —e(a^)) = e(pX(e(-a¿) - 1), we obtain r j = - / . □ Lemma 6 Let A e P_^. r/ie« the stabilizer o f K

p in W is trivial.

Proof Let w E: W. Then wA c P ( A) c A i ¡2+ wp = p — (S ^ )

[Proposition 6.1.10(i)] (Proposition 5.2.5)

But <5^> ^ Q+ if w # 1 (see Corollary 5.2.5). The lemma follows.



Proof o f Theorem 1. We are going to assume that J is finite. We leave it to the reader to fill in the details when J is arbitrary. L is integrable with highest weight A. Consider the Verma module M(A). Recall that the Casimir-Kac operator F^(A) acts on this as scalar multiplication by (A + 2p|A). If p e A 1 ¡2+ and [M(A): L(p)] > 0, then (A + 2p|A) = (p + 2p|p) (see Proposition 4.5.3). Now L ^ M {K )/N for some submodule N, and hence by Propositions 2.6.2 and 2.6.12

(2)

ch M( A) = ch L + ch N = ch L + E [ ^ : ¿ (/i)]c h L (p ).

The sum runs over p. e A j, (2+. We may assume that fi ¥= A, since M(A)^. Therefore = (0), and hence [N: L(A)] = 0. Also note that

=

[N: L (p )] = [M: L (p )] > 0 ^ ( p + 2p|p) = (A + 2p|A). Let Aq = A, Aj, A2,... be the elements p of A i (2+ satisfying (p + 2p|p) = (A + 2p|A). We partially order these elements by increasing depth. For

Category ^ for Kac-Moody Algebras

536

convenience of notation we write L(A q) for L, even though we are not assuming that L is necessarily irreducible. Then (2) reads ch M (A o )= E [M (A o ):L (A ,)]ch L (A ,) ¿>0 Now in the same way Proposition 2.6.12 gives (3)

c h M ( A ,) = E [M (A ,):L (A ,)]c h L (A ,),

k = 0 ,1 ,2 ,. ..

i>k

(since only weights of depth larger or equal than that of

occur in

Taken together, the equations (2) and (3) form a system of linear equa­ tions with coefficient matrix 1

[M (Ao) :L(Ai )]

[M (A o):L (A2)]

0 0

1 0

[M (A ,):L (A 2)] 1

where we have used the obvious fact that [M(A^): L(A*)] = 1 for all k. Now this matrix is upper unipotent, and hence the system of equations is formally invertible. Consequently we can express the ch L(Aj.) as formal sums of the ch M(A,.); c h L (A * )= E e* ,ch M (A ,.). i>k

Here the e Z and = 1 for all k, since the above matrix has diagonal consisting of Ts. In particular chL(Ao) = E«/ ChM( A, ) ¿>0 for some e Z, where = 1. Now we use Proposition 2.5.4(ii) and obtain c h L ( A o ) = Ea¿c(A,) П ¿>0 Thus multiplying by e(p) and setting

/:=e(p) П «gA.

(l~e(-a))

-dim g®

6.4

The Formulas of Weyl-MacDonald-Kac

537

we obtain

(4)

/c h L(Ao) = L a,e(A,. + p ), />0

an = 1.

Since ch L(A q) is Pf^-invariant and / is W^-skew-invariant, the left-hand side, hence also the right-hand side of (4), is PF-skew-invariant. In particular W simply permutes the elements (A^ + p) for which ^ 0. Let Q in (4). Then PP^(A^ + p) c (A + p ) i <2^. has an element of minimal depth, which is then dominant, say, >v(A^ + p) = A^ + p, and furthermore Up = ( — Now suppose that Aq # A^. Then we have Aq, A^ + p e and A^ e A q i 2+- Thus by Lemma 4, (A qIAq + 2p) > (A^|A^ + 2p), contrary to the definition of the A/s. This contradiction proves that A q = A^ and hence that A^ + p = w ^(A q + p),

In view of Lemma 6, w that

w'

w(Ao + p) =5^ >^'(Ao + p). We conclude then

/ c h L ( A o ) = E « , e ( A , + p ) = E ( - l ) ' ^ ’^ ^ w ( A o + p)). w^W ¿>0 For another approach to these formulas, see [GLl] and [GL2]. The following examples will give some idea of the appearance of the denominator and character formulas in particular cases, as well as some indication of the amazing amount of information that they contain. The Appendix includes an extensive example of how to use these formulas. Example 1 In the case of ^I2(K), A = {—a, 0, a}, W = {1, r^}, p = a/2. The denominator formula reads

K p ) - e(''«p) = « (P )(l - < - « ) ) = « ( 2 ) “ ^ (“

2

)’

which is certainly true (r„p = p - a)), though hardly enlightening.

Categoiy & for Kac-Moody Algebras

538

The dominant integral weights are na/2, n ^ N, and by Theorem 1, chL

( r ) -

e ( n a / 2 + a /2 ) — e( —( n a / 2 + a /2 ) ) e ( a /2 ) - e( - a / 2 )

_ e ( a / 2)"^^ - e ( a / 2)-^"*^^ e ( a /2 ) — e ( a / 2 ) ^

na \

Í (n — 2)a )•

-

m

This result agrees with what we already know about the irreducible ^Í2(K)module of highest weight na/2. Namely its weights are n a /2 , ( n a /2 ) a, (na /2 ) — 2a , . . . , —n a / 2 and all of its weight spaces are one dimen­ sional. Example 2 In the case of §I/+i(IR) we use the description of A i given in Section 3.1 for the lattice Ai and the description of its roots given in Sections 3.2 and 3.3. Thus ..., is an orthonormal basis for and the roots are ^ = K with simple roots ai

Si

^/+1?

^

1? • • • ?

and positive roots A+= (e,- - Sj\i <;•}. These span the subspace V '= {Ec^eJEc^ = 0}. The Weyl group W acts by permuting the £¿5. Let A e P_^_, and write A = EA,e^. Then 2(A|a,.) (5)

^ í + 1?

(a,la,)

and the condition that A e (6)

A

^

reads ,

.

¿ = 1,...,/.

l?***5^j

6.4

The Formulas of Weyl-MacDonald-Kac

539

Since P + c F, we have the additional condition (7)

L a, = 0.

Together (6) and (7) characterize P^, The fundamental weights defined by (co^\aj) = were worked out in Section 3.1: (Oi = Si -\- • • •



/ +1

, (s>i,

(«1 + ■■■ +«/+i)

where / + 1 —/ /+ 1 i I+ 1

if j < if j > i.

Obviously for all A = e the coefficients A, e (/ + 1)“ ^Z. If we translate each A^ by some real number k, then we obtain a point A' = E(A^ + /:)£• G whose functional value on each a, is the same as before (though in general A ^ F). It is convenient to make use of this to “normalize” the A/s so that A/+i = 0 thus obtaining a 1 — 1 correspondence: {(Ai .A2,---,A,)|A, e N, I = 1 , . . . , / , A, > A2 > ••• >A,}. In particular for p, which has the defining property (p|a^) = 1 for each /, p ^

(/,/ -

We now introduce the lattice L '= ( l / ( / + DXZej + *• • group ring ±1

Z[L] = Z

( i J r l " ....... - ( S i l

Define X, = e(£;), and write

/ = 1, . . . , / + 1,

for e(e,/(/ + 1)). We have an embedding Z [P ]^ Z [L ] e(ct>,)

M

c(a,) ^ x ,x ,+ V

-^/+1

and its

Category & for Kac-Moody Algebras

540

W acts on Z[L] by permuting the variables. As we will now see, the denominator and character formulas have very lovely interpretations in Z[L]. Consider the denominator formula. We have «(p) = (-^1 ••• -^/+1)

^

xi.

where k{p) is the translation of the normalization of the coefficients of p, namely - ( / + l)fc(p) + = 0. This only enters peripherally into the picture. Observe that is fixed by W. Thus the denominator formula reads ••• ^/ + 1)

"

E

cre5/+i

(^1 ••• ^/+1)

Sgn(o-)jct(l)Jf^(2) a(Y)^
= (^1 ••• ^/+1)

-^ y )i< j

Cancelling off we obtain the well-known formula from the theory of symmetric functions for the skew-invariant polynomial of minimal degree. It is even more familiar as the Vandemonde determinant formula:

X2

det

= n ( ^ i -^ y )i<j

*^/+1

-^/+1

Having recognized skew-symmetric sums over as determinants, it is natural to interpret the character formula as the ratio of two determinants. Suppose that A e A <-» (A^, A2, . . . , A^) with translation A:(A) for normal­ ization. Then

£ w^W

+ p)) = (^1 • • X/+1 (^1 ••• ^/+1)

-k (A )-k (p )

o-eS/.i

6.4

The Formulas of Weyl-MacDonald-Kac

541

SO

chL (A) = (ДГ1 •••

det(x-

Here is a specific example. Take §1з([К) which is of type A 2. Consider Л= + й>2 ^ (2,1,0), so k(A) = 1 [see (6) and (7)]: 1 ( ^ 1X2X3) chL(A) =

xt

xl

1

X3



1

-Хз)(Х2 - x ¡ )

A few row operations allow one to divide out the factors of the denominator, and we end up with

ХлХ^Х l^2^3 =

•{xiX2

+

xfx^

X^x^^

+ X 1 JC2 ^ + -^2^3 ^

= e(a^ + «2)

+

X^xl

^(^1)

+

x^xj

+ Jc|x3 +

X 2 XI

^2^1

^

+

2 x ^X2X^]

^1^^3

+ 2

^(^2) “*■^ ( “ ^2)

+ e ( —ai —0:2) + 2^(0). This is exactly as it should be: L(A) is the adjoint representation of ^Í3(R) (the highest weight is the highest root + «2) ±(0:1 + «2), ± ±«2? 0 are the roots, with the multiplicity of 0 being 2 since dim = 2. Proposition 7 (Racah formula) Let g be an invariant Kac-Moody algebra. Let A e F^_, fx ^ P. Then

w^W ^ j (— ,0

if fjL p = v(A + p) for some и ^ W, otherwise.

Category ^ for Kac-Moody Algebras

542

Proof, From the character formula £

(-l)«-^>e(^(A + p ) ) =

£

(-lf'^^e(w p) £

dimL(A)V(A)

wœW

wœW

= L w^W = £ A s ii*

L dim L(A)^e(tvA) Ae]^* Aeb* £

v / ( » v ) J - * ___

( - 1)

r

/

A \ A .

dimL(A) e ( w ( A + p ) ) ,

w ^W

where we have used the fact that dim L(A)’^"' = dim L(A)"' for all w ^ W . Now dim L(A)^ = 1, and hence after cancelling, 0=

£

£

( - l ) “’^Mim L(A) c ( w ( A + p ) ) .

Aei|*\{A} weir

Suppose that p. e P, p i W(A + p). Group together all the terms e(w(A + p)) = c(p + p), namely A = w ' K p + p) - p. By assumption we never have A = A. Thus

w^W Finally, dim L( A) “'’ = dim = dim which is what we wanted to prove. Now suppose that fjL -\- p = u(A + p). Then for all iv e PF, p, + <5^> = p + p - wp = u(A + p) - wp = ¿;(A + Thus dim = dim Since e 2+ if and dim = 0 for all a ^ Q^, only one term survives in the sum of our proposition, namely ( - iy<"> dim U A Y ^ = ( - iy<">. □ This formula can be used to compute the weight multiplicities dim L (A Y by induction on depth. More commonly the Freudenthal formula is used. See the exercises of this chapter for more on this formula.

6.5

COMPLETE REDUCIBILITY

In Section 2.4 we proved a complete reducibility theorem for the finite­ dimensional representations of ^I2(1K). In this section we generalize this result to arbitrary invariant Kac-Moody Lie algebras. The proof is essentially the same.

6.5

Complete Reducíbilíty

543

Theorem 1 [iCPl] Let g be an invariant Kac-Moody Lie algebra over K, and let M be an integrable %-module in category 0 . Then M is completely reducible. In fact

M= e [M:L(m)]L(m)Remark 1 The multiplicities [M: L{¡i)] are defined in Section 2.6 as the number of times L(/i) occurs in any composition series of M relative to p. Remark 2 At the time of writing it is not known whether it is necessary to assume that g is invariant. Proof Let M be an integrable module in category 0 . Recall that the Casimir-Kac operator acts on M as a degree 0 linear operator. It follows that stabilizes the weight spaces of M, which are finite dimensional. Thus, by extending IK if necessary, we can decompose M into a (direct) sum of generalized eigenspaces Mj := |i; G M |(r^ —t)^v = 0

for some k e Z + |,

where t runs over IK (see 7.1). Each space is a g-submodule since commutes with the action of g on M, Since e 0 , if ^ (0) it has a highest weight vector u e M f for some (p e ]^*. Recall from Section 4.5 that Tm ^ = (q>\(p + 2p)u. Thus t = (
0 n,L(p,,.),

where f c P_^, ( p j p , + 2p) = t for all and the n¿ e Z^, We claim that 5, = M^. Indeed, suppose that for some i e IK, S^, Then Mf/Sf has a highest weight vector v e for some p e 1^*.

Category á for Kac-Moody Algebras

544

The highest weight module U(g) * v c is integrable. Hence ii e Let be a preimage of ü in M¡^. From the definition of it follows that + 2p)i; mod 5,. Since V e M,, (p |p + 2p) = t. Now, if ^ 0 for some generator of then ej • u ^ S ^ \ {0}, and hence fi ^ v - a for some v e some a ^ Q+. However, from Lemma 6.4.4, 0 = Í - Í = (i'll' H- 2p) - ( mIm + 2p) > 0

and

since jjl, v ^ P+.

This contradiction shows that ej • v = 0, so g + - = 0 and t; is a highest weight vector. Thus U(g) • z; is an integrable highest weight module, hence isomorphic to L(/i) by Theorem 6.4.2. But then U(g) • i; c 5^ contrary to V ^ Sf. This completes the proof that = S^, and hence M is completely reducible. The uniqueness statement of the theorem is a consequence of the results on composition series in Section 2.6 (or see Proposition 2.6.11). □ Corollary 1 Let g be an invariant Kac-Moody Lie algebra, and let L(A) 0||^L(p) is completely reducible.

X , ijl

^ P+. Then □

Corollary 2 If g is an invariant Kac-Moody Lie algebra over C, then any integrable module in category 0 is unitarizable. Proof Use Theorems 1 and 6.4.3.



Applying the theorem to the adjoint representation we obtain the follow­ ing proposition: Proposition 2 Let g^ := R ) be defined by the Cartan matrix A = (yl,y), у realization R . Let A = (^¿y)^ y ^ j be a symmetrizable submatrix o f A , and let g := R) be a subalgebra o f g^ obtained by restriction from A to A {see Remark 4.3.1, and Proposition 4.3.2). Set M д(у4')±\а(>4)±91* (i) gi = M _0(g + f|) e M+. (ii) M_ {resp. M+) is a completely reducible q-module [in category 0 ( q) (resp. 0 4 q))1

6.6

The Shapovalov Determinant Formula for Kac-Moody Algebras

545

Proof. Part (0 is obvious. For part ii we use the facts that M_ is an integrable g_ module in category and that g is iiwariant. Similar consider­ ations apply to M+. □ 6.6

THE SHAPOVALOV DETERM INANT FORMULA FOR KAC-MOODY ALGEBRAS

Recall that the Shapovalov form bilinear form

on the Verma module M(A) induces a

M(A) XM(A)

K.

This is defined as follows: If v+ is a highest weight vector of M(A) and X= y = «2 ■ where «2 ^ U(g_), then

where ^:U(9) ^ U ( 5 ) is the projection onto the first factor of the decomposition U(g) := U (^) e(g_U(9) +U(9)9+). In this section we prove the Shapovalov-Kac-Kazhdan determinant formula for invariant Kac-Moody algebras. This is an explicit formula for the determi­ nant detSh.y, -y e g^u{0} of Section 2.8. The formula involves the Kostant partition function K defined in Section 2.5 by ch(U(g_))=

L K(p)e(-p). /3ee+u{0}

An essential ingredient in this section is the notion of Jantzen filtrations discussed in Section 2.9. Theorem 1 Let 9 be an invariant Kac-Moody Lie algebra with triangular decomposition (^,Q+,Q+, o’)- Let K be the Kostant partition function and Sh^ the Shapovalov form with value Sh^(A) on the weight space MiX-Y ^ for each A e fi*, y e <2+u{0}. Then “ / («1«) detSh^ = C - n n U “ + P (« ) - " — ^ aeA+n=l\ ^

K(y-na)

Category û for Kac-Moody Algebras

546

where . the determinant is to be understood as follows: M(A) =: U(g)//(A), where /(A) is the left Ui^ymodule defined in Section 2.3. is an ordered basis o f U(g_)”'^ then {w, mod/(A)} is a basis o f under the identification with U(9)//(A), and detSh^(A) == det((F|^(«¿, My))(A)) [see (2.8.3)]. Then detSh^ is a polynomial function on ij* whose value at each A is det Sh^(A). . is defined by (4.4.8), . the product is over A+ with roots repeated according to their multiplicities, . p G ]^* is chosen so that
Y\ i8eÁ+ n =l

6.6

The Shapovalov Determinant Formula for Kac-Moody Algebras

547

The proof of lemma requires some preliminary discussion. Let Pi < P2 ^ ^ total ordering of Â+ made in such a way as to respect increasing height. Usmg Proposition 4.7.4, we can find a basis of 9+ SO that ep e g^, (cre^lcp,) = 8^^,. In order to apply Proposi­ tion 4.7.4, we need our field to be ordered. We can overcome this_by taking the basis from some rational form of g; see Section 4.3. Thus for /3 = /3' we have [a-ep,ep,] = -8 ^^,^^ (4.4.10). Let y e 0+u{0}, and let iK y) denote the set of all partitions of y into elements of Â+ (note the convention mentioned above). Then card (ii(y)) = iC(y). For each partition w = {/3,^ < /3,^ < • • • < /3,} of y, set ■= o'(efl.)cr(e«. ) • • • a-fcg.) G U fg .)“"^.' Then {Ar„,|w g 0(y)} is a basis for U(q_)“'^ (see the proof of Proposition 2.5.3). The length of a partition w is the number of parts in it. By definition ft(0) consists of the empty partition 0 and ~ 1• Lemma 3 Let w, w' e fKy), y e ¡2 + u{0}. Then the leading term o f qiX^X^r) has degree less than or equal to 5(iv, w') •= \{length{w) + lengthiw')}. Furthermore equal­ ity occurs if and only ifw = w \ and in this case if w = [ô^ < 82 < *** < 5^}, then the leading term o f q (X ^X ^) is C n[=i5? for some positive integer C. Proof It is useful to begin with the following observation which is easily established by induction onr:If jL Ci, .. .,/ x^ eA+ , then for every permuta­ tion 77 of {1, . . . , r} (in particular for 77 so that m^(1) < • ** < M-Trcr)) have e

•**e

=e

***e

+i?,

where R isa linear combination of products e^^ • • • e^^ and ..., e A+ and s < r. We prove the result for all y at once by using induction on 5(w, w'). If s(w,w') = 0, then w = 0 = w' and q(X^X^r) = 1, so the result is true in this case. In general we write w = {5i ^

• •• ^ S J ,

w' = { e ^ < € 2 < ■■■ <e,) , where Z 8¡ = y = Ee,-. Since q(X^X^,) = q(X^>X^) (Proposition 2.8.1), we may assume that < 8i. We write e_^_ instead of o-(e^), j = 1,..., 5. We have (t ( X J X ^ , =

■■■ Cs

= «3^ • • • es^[ese_,}e. +

. . .

g

e_,_ =-A + B.

Category á for Kac-Moody Algebras

548

We consider the two terms separately. If and A = 6s^

then [e^e_^^] =

•••

= e, - ( £ 2 + ••• +e.)(5?)(es, •••

•••

Set Z := e,8r . By the induction hypothesis q(Z) has leading term of degree less than or equal to s(w, w') — 1, and equality occurs only if r = s, Si = 8i for all i. In this case the leading term of q{Z) is C e Z+, and hence the leading term of q{Z8^) is Thus A will contribute precisely C 'n[= i8i to our proposed lending term if w = w', and otherwise nothing with degree this high. If ¥= then w ^ w', and either [e^^, e_^^] = 0 and ^4 = 0 or [e^^, e_^^] is a linear combination LCj-e^, (positive roots because Sj > e^). Thus by the observation at the beginning of the proof A expands as a linear combination of terms o-(X^)X^,, where s((p,cp') < s(w,w'). By the induction hypothesis we may dismiss these terms from our consideration. Now consider B. If r = 1, then ^(B) = 0. If r > 2, then B = e s ^ - - esj_es^e_,^]es6_,^ ■■■ =-A' + B'. We deal with A' as with A above. If we obtain a contribution of ^8/ ” ^82^81^-62 *** ^-Ss^2 terms that cannot contribute to a leading term of degree s(w,w'). The partitions < ^3 < ••• < 5^}

and

{£2^

^^5}

can be equal only if £2 ^ ^1 ^ ^2 ^ hence w = w'. In that case we obtain by induction a contribution of a positive integral multiple of IT-=i5f again. If £5^ we obtain [e^^, e_^^] = 0 or [e^^, e_^^] is a linear combina­ tion and, as before, we are able to dismiss A' by the induction assumption! The term B' is treated just like being moved leftward again. The process repeats until reaches the leftmost position, where­ upon q kills the corresponding term. The lemma now is clear. □ Proof of Lemma 2. For 7 = 0 the result is trivial, so we suppose that 7 0. According to Lemma 3, the leading term of det(Sh^) = 0(7)) comes from the diagonal and is a multiple of (1)

n

U 8?.

{ S J s i K y ) (S,)

6.6

The Shapovalov Determinant Formula for Kac-Moody Algebras

549

We have to count how many times a particular 8^ will occur. If 8 appears as a part, say, exactly n times, of some partition w e il(y), then what remains of w after removing these n occurrences of 5 is a partition w' of y - n8 with no occurrences of 8. Now we have a bijection ilr. (w'} from the partitions of n (y - n 8) to the set of those partitions of fi(y) with at least n8’s, and similarly a bijection [w") ^ {w",8} from partitions of iKy - (n + 1)8) to the partitions of fl(y - n8) with at least one 8. Thus if/ maps the K(y — n8) — K(y - (n + 1)8) partitions of il(y - n8) with no occurrences of 8 onto the set of partitions of fi(y) with exactly n occurrences of 8. The number of occurrences of 8 in (1) is E n { K ( y - n8) - K { y - (n + 1)8)) n>0

= ( K ( y - 8) - K ( y - 28)) + 2{ K ( y - 28) - K{ y - 38)) + ■■■ = Y . K ( y - n 8). n>0

This concludes the proof of Lemma 2. Define Q+A+= {aa\a e Q^, a e A+}. Elements of (Q+A^.) U called quasi-roots (see Kac-Kazhdan).

□ are

Lemma 4 Up to a nonzero scalar factor in IK, detSh^, y ^ Q+, is a product o f linear factors o f the form

where ^ is a quasi-root. Proof For the purposes of the lemma we can assume K is algebraically clo^d, for otherwise we can extend IKto an algebraic closure K, replacing 1^* by IK®!,^]^*, and so forth, to obtain the result. We view det(Sh^) as a polynomial function on i}*, and let its zero set be denoted by V. For any A e 1^*, (det(Sh^))(A) = det(Sh^(A)) vanishes only if the unique maximal submodule MA) of the Verma module M(A) meets the weight space nontrivially (Corollary to Proposition 2.8.3). For this to happen, MA) must contain a highest weight vector with weight A - j8 for

550

Category ^ for Kac-Moody Algebras

some P ^ Q+ with A - y e (A -have

Using Proposition 4.5.3(ii), we

( A + 2 p |A ) = (A - ^ + 2p |A - j8),

which simplifies to (A+p|/3) = 103|i3), or equivalently (A +p)()80)-i(/3|/3)=0. Let ~ it acts as

+ p(^°) “

e 5(1^). As a polynomial function on

^p(A) = (A +p)()8°) - A(j8|)8). What we have proved is that for a fixed y, det(Sh^) vanishes only on the union U of the hyperplanes of f)* defined by the zeros of the £^,/3 0 !2 +’^{0}, A - y e A - j S i Q^, i.e., y - jS e (2 +U{0}. The set of ¡3 satisfying these conditions is finite and independent of A. Thus V
6.6

The Shapovalov Determinant Formula for Kac-Moody Algebras

551

Proof. (0 By Lemma 4, M(A) is reducible <=> det Sh^(A) = 0 for some y e Q+=> E^(X) = 0 for some quasi-root p. (ii) By part (i), Af(A —p) is irreducible. The sum N of all the irreducible submodules of M(A) isomorphic to M(A —/3) [possibly N = (0)] is a finite direct sum of such modules. To prove that N = MA), we prove that L — M { \ ) / N is irreducible. If it is not, then by Lemma 2.6.3(ii) applied to L, M(A) has a primitive vector v of weight k — 8,8 ^ Q^, with v ^ N and c AT. By Proposition 4.5.3(ii), (A + 2p|A) = (A —5 + 2p|A —5), from which we have = 0. Thus 8 = p, and v e Now U(g+) • v contains a highest weight vector v'. If v' e K^v, then v itself is a highest weight vector and generates a copy of M(A — p). Then contrary to assump­ tion, u ^ N. If u' ^ K^v, then u' ^ N by the definition of u. But N has no weight spaces above X - p, and we again have a contradiction. Thus L is irreducible as claimed. □ Lemma 6 For fixed a e A+ the functions Q + Z defined by K¿J,y) •= K(y — ¿a), / = 0,1,2,..., are linearly independent {over Z). Proof. Suppose that La¿K¿^ = 0 for some a¿ e Z. With y = 0 we obtain 0 = L a¡K{- i a ) = aoü:(0) = üq. ¿^0 Then with y = a we obtain 0 = E a¡K(<^ - ia) = a,K(0) = a„ i > l

and so on. Lemma 7 Fixz so that for all s e A+, z(e^) 0. For each A e 1^* yei A — A + zt, where t is an indeterminant. Following the construction o f Section 2.9 {applied to our Lie algebra g), form the Verma module M(A) for IK[f ] ^i^g, and let (JFl)

M( X) = M q Z>M^z>

and (JF2)

M(A) =Mor>Mi =)M2 =)

be the corresponding Jantzen filtrations [see (JFl) and (JF2) o f Section 2.9]. Then for all y e Q^, detShr(A) = constant X

El S=quasi-root

Ky,S)

Category ^ for Kac-Moody Algebras

552

where detSh^(A) = constant

X 5 = quasi-root

Remark 3 We already know that det Sh^(A) has the form indicated here. However, we do not know the exponents /(y, 8). At the end of the proof of the Theorem 1 we will have 00

detShy(A) = constant X aeÁ+"=1 Proof. Let 7 G (2-b) weight space

consider the Shapovalov matrix Sh^(A) for the of M(A) (M(A) being treated as a lK[i]-module). Let M(A) ^ M ( A )

be the usual map determined by the specialization t ^ a, a E: K. We have (Lemma 2.9.3) E^(Shr(A)) = Sh^(A + za) and E^(detShy(A)) = detSh^(A H-za). But det Shy = constant

X

(5^ + P ( ^ ° )



/(y,5)

8 = quasi-root

Thus detShy(A + za) = constant

X

This being true for all a e K, we have det(Shy(A)j = constant

X n ( ^

5

('^) +

Proof o f Theorem 1. It is useful to assume that K is uncountable for the purpose of choosing suitable A e ]^*. We can always replace IK by an uncountable extension, if necessary, to allow us to make this assumption. Let y ^ Q+. We know two things: first, that the leading term of det Shy is n n aeA+"=1

6.6

The Shapovalov Determinant Formula for Kac-Moody Algebras

553

and, second, that det Sh^ is a product of factors

where jS® runs over various quasi-roots. Our object is to show that the factors in the leading term are precisely explained by corresponding factors in det Sh^: (n, a^) ^ na^ + p(na^) — \{na^\na^)

= n |a ° + p (a °) The conceptualization of what is going on is complicated by the fact that if a then na so + p(a^) - n{a^\a^)/2 occurs for several ‘‘reasons” in the factorization of detSh^. The proof avoids analyzing this in detail. We introduce the notion of a root ray. Let a be a quasi-root. The root ray through a is Q+a n 0 +j (the set of all quasi-roots p that lies in the same ray of 1^* as a). For each root ray R the leading term of + must correspond to We deal with the problem one root ray at a time. Now one part of the product of Theorem 1 is easily disposed of. If R is the quasi-ray through a and (ala) = 0, then for all P ^ R we have ip\p) = 0 and p^ + p(p^) — n(p\p)/2 = H- p(p^) = c(a® + p(a®)) for some c = c(p) e Since the factors of detSh^ that can contribute factors a® to the leading term are precisely those of the form p^ + p(P^), P^ ^ R, we must have for each a e A+ and n e Z+ a factor (a® + p(a^) —n (a |a )/2 ) in det(Sh^), and this accounts for all factors of det(Sh^) related to the ray R. Now suppose that R is a quasi-ray through a with (a |a ) 0. Let be a quasi-root on R, so (p\p) ^ 0. Suppose that we prove that for all y e 0+, P^ + p(P^) - HP\P)

( 2)

occurs n ^ K ( y - p) times

as a factor of detSh^, where is a positive integer independent of y. Then up to a scalar factor, the contribution of this quasi-ray R to det Sh^ is n

- k m )

rifíK(y-p)

Comparing with the leading terms and using Lemma 2, we find that up to a scalar factor, n

= constant X

n

n á^R

n= l

Category € for Kac-Moody Algebras

554

that is, 'L n J K (y -l3 )=

L j:K (y-n a ) n ae A+, a^R = l

fo ra lly e e ^ .

By the independence result (Lemma 6) equals card{(a, n)\a e A+, na = p}, and hence the factors a® + p(a^) - n(a\a)/2, na = p occur with exactly the correct multiplicity in detSh^. It remains to prove (2). By definition ^^(A) := A(5") + p(8^) - ^{8\8),

8 e 2^u{0}, A e r •

Since we have (p\p) # 0, we can easily check that none of the hyperplanes £g(A) = 0, 8 p, and £g(A - /3) = 0, of 1^*, is the hyperplane E^iX) = 0. Then, since K is uncountable, we can choose A e 1^* satisfying the three hypotheses of Lemma 5 (ii). For this choice of A, M(A) has maximal submodule MA) = 0M(A - p) (finite sum, conceivably empty), and M(A - p) is irreducible. Fix z g i)* so that for all s e A+, z(s^) ^ 0, and set A = A + zt, where t is an indetermi­ nant. Following Section 2.9, we obtain a filtration M(A) = M d M i d A?2

•••

and a corresponding Jantzen filtration defined by evaluation of t at 0: M(A) = M d M j 3 M2 => ••• Since Ml = N(X) (Theorem 2.9.4), each Af^, A: > 1, is a direct sum of, say, n/^ copies of M(X — p) (which explains why the series is finite). Applying Lemma 7, we see that the power of t dividing det Sh^(A) is pre­ cisely the number of quasi-roots 8 occurring in the product [taken Ky,8) times] for which ^^^(A) = 0 (note the choice of z). By the choice of A the only quasi-root with this property is p. Thus the number of factors of t in detSh^(A) is equal to the number of factors of (p^ + p(P^) ~ j(P\P)) in detSh^. However, by Theorem 2.9.4(i) we know that the power of t dividing det Sh^(A) is E d im M r" = k=i

L n ,\K {y -p ). \k=i

I

This proves (2) and concludes the proof of the theorem.

6.6

The Shapovalov Determinant Formula for Kac-Moody Algebras

555

Remark 4 Note that we obtain as a result of the proof that /(y, 5) = K{y - 81 Given A e

define

A+(A) == {(a, n)\a e

n e Z + , 2(A + p )(a ° ) = n(a°|a«)}

(don’t forget that a itself is already an ordered pair). The next result is the basis for Section 6.7. Corollary Under the hypotheses of Theorem 1, and with M(A) D

=) M2 =5 • • •

the filtration appearing in the proof, we have 00 £chM ^= Y. c h M (A -n a ). (a ,n )e A + (A )

Proof. We see from Lemma 7 and Remark 3 that ord,(detSh (Á)) is pre­ cisely the number of factors (a° -I- p(a^) for which = 0, where a e n e Z^.. Now = 0 -«=> (A -l- pX«°) ~ n(a°la°)/2 = 0, and we conclude that ord,(detSh^(A)) =

£

K (y-na).

(or, / i ) s A^_(A)

Using Theorem 2.9.4(ii), we have 00

£chM *= k = l

=

£ ord,(detSh^(A))e(A - y) reG+UtO) £ y s Q ^ U iO )

=

£

K { y - n a ) e { \ - y)

(a ,„ )G Á + (A )

L

L

K (y-na)e(A -y).

(a ,n )e A + (A ) r e 0 ^ u {O }

Now K(y — na) = 0 unless y = /3 + na for some ¡3 e Q+G{0}. Replacing y by /3 + no: in the last sum, £chM , = ^= 1

£ ( a , / z ) e A + (A)

=

£

K i P ) e { \ - na -

IB ^ Q + u {0 }

X) ch M { \ - n a ) (a, «)e A+(A)

^

Category ^ for Kac-Moody Algebras

556

6J

THE B G G THEOREM A N D GENERALIZATION

In this section we derive a characterization of the weights e i)* for which L(/x) is a subquotient of M(A). The original theorem of this type is known as the Bernstein-Gerfand-Gerfand (BGG) theorem and was proved in the context of finite-dimensional semisimple Lie algebras [BGGl]. The general­ ization to the invariant Kac-Moody case occurs in two steps over the papers [KK] and [DGK]. The notation here continues that of Section 6.6. In particular (g, is a finitely displayed invariant Kac-Moody algebra: A+ (A) := [{a,n)\a e Á+ , n e Z + ,2(A + p ) ( a ° ) = = [{a,n)\a E:

e Z + , 2(A + p\a) = n{a\a)],

and A+ is simply A+ expanded so as to take account of multiplicities. P is standard weight lattice. Let A,p, e 1^*. We write A^— ¡i if A = p, or if there is a pair (a, n) e A+(A) so that 11 = \ - na. We extend this relation transitively so that A>— fi means that there exists a sequence of elements ^ P^ so that

Proposition 1 Let g be an invariant Kac-Moody algebra with triangular decomposition (Í), 0-). Let A E r . Then for e M(A) ^ M ( f i ) <=> [M(A): L(fi)] > 0

A > -/i.

Proof The first equivalence is proved in Theorem 2.11.1. For the second we use induction on ht(A —¡i) (simultaneously for all \ , f i E i j * for which \ - fi E (2+U{0}). The result is true if \ = fi. From Proposition 2.6.12 and the corollary of Theorem 6.6.1 we have E E [M,: L(,x)]ch L ( n ) fc=i IJ.SÍ)*

=

E L [ M ( A - n a ) :L ( M ) ]c h L ( /i), (л,«)еД^.(А)/*е6*

where M(A) э Afi э Л/2 э • • • is a Jantzen filtration of M(A). Since the

6.7

The BGG Theorem and Generalization

557

characters chL(^t), e 1^*, are linearly independent (Proposition 2.6.11), the coefficients of ch L(^t) on both sides of this equation are equal. In particular 1. [Af^: L(jLt)] > 0 <=> [M(A - na): L(/x)] > 0 for some (a, n) e A+(A). 2. Using the corollary to Proposition 2.6.13, since [M^: UiJi)] > 0 <=> [M,: Ufi)] > 0. 3. Since = MA) and we have the exact sequence 0 we have for \

-^M (A ) ^ L ( A ) ^ 0,

fi, [M(A): L( ijl)] > 0 <=> [M^: L(^l)] > 0.

Now using our equation and the induction assumption, we have for A [M(A): L(/x)] > 0

/jl,

[M(A - na): L(fjL)] > 0 for some ( a , n) g A+ (A) <=> A - na>— IX

for some ( a , n) e A+(A)

<=» A>— IX,



The preceding result suggests an interesting equivalence relation on 1^*: A

/X <=> there exists a sequence A = Aq, A^,. . . , A^_j, A^ = /x

so that for each / = 1 ,..., A:, -A, or А,-

^/-1

For each equivalence class A we introduce the full subcategory of ^ whose objects are those modules of & all of whose composition factors L(^t) have /X G A. Evidently contains all sums, submodules, and quotients of its modules. □ Proposition 2 For all A G ]^*

have M(A)

g

Consider the case when dim q < oo. Every nonzero root is real, and hence for a G A^_, w G Z^, ( a ,n )

G

A+(A)

2(A + p\a) (a la )

=n

= n. If (a, w) G A+(A), we see from the definition of (see Proposition 4.4.7) that X — na = rJ^X + p) —p. Because of the frequency of expressions like w(X + p) - p in this context it is useful to introduce the dot-action of the

Category ü for Kac-Moody Algebras

558

Weyl group: For \ ^ t)*, w ^ JV, w ' X '•= vv(A + p) —p. It is trivial to check that this is a group action (although it is not a linear action): { ^ 1^ 2) *A = Wj • W2 • A

for all Wi, vv^2 ^ W, X e 1^*.

The expression above can be thought of as the action resulting from shifting the origin to the point —p. Define for each A e ]^* a set c'^^A and a.subgroup of W: A^ :=

[a

G'’^A| e Z},

:= . Proposition 3 (i) A'^ is a subroot system o f A, and is its Weyl group. (ii) For all w/Xf = A’^^ = A^^ and wW^w~^ = (iii) I f w ^ then A^-^ = A^ and = W^. Proof (i) If a, j8 e A^, then ( X ,r ^ P ^ ) = ( X , p - - ( a , p - } a - ) ^ Z . This proves that A^ is a subroot system of A. Then W^ is its Weyl group by definition (see Section 5.6) (ii) Trivial verification (note that wp — p ^ P). (iii) Follows from part (ii), since W^A^ = A^. □ In this case that dim g is finite we obtain a precise description of the -equivalence classes. Proposition 4 Suppose that dim g < 00. (i) The equivalence class A 0/ A ш 1^* is • A. (ii) jy A e ]^* and w El W, then the equivalence class ofw • A is (wW^) • A. (iii) I f К = U and F c ]^* is a chamber o f the Tits cone, then the map Лs —p -\-F

wW>^ is a bijection (here F is the closure o f F).

wW^ • A

6.7

559

The BGG Theorem and Generalization

Proof, (i) Let A e 1^*, and let a e A^. Then n —

A or

In either case • A A. Using Proposition 3(iii), we now see at once that w • A A for all w e W^. Conversely, suppose that /x e A. It will evidently suffice to show that if — A or A rel="nofollow">— jjL, then p = • A for some a e A'^. But in either case fi = Á — na, where a e A+, 2(A + p\a) = n{a\a), and n e Z. Since a equation can be written

this last • A = p,.

• A = wW^w-^w • A = {wW^) • A. (iii) Consider the map U

^ f)* /'-

A s —p + F

wW^ •- rel="nofollow"> wW^ *A We need to prove that ^ is 1-1 and onto. onto: Let p , p e 1^*, be an arbitrary equivalence class. Then by Proposi­ tion 5.6.9 there exists a (unique) w ^ W with wifi + p) e F. Set A + p = w(fjL + p), and observe that • A = p. Thus p e • A, and -p+ F. 1-1: Let A,p e —p -h F. Suppose that wW^ • A = w'W^ • p. Then wW^ • A = w'W^ • p => p e IF • A => p -h p e W ( \ + p) = > p + p = A+ p = > p = A (Proposition 5.5.9). Thus vw • A = (w'u) • A for some u e W^, and we have w • A = (w'u) • A => w~^w'u • A = A => w~^w'u(\ + p) = A + p => w~^w'u e Stabp^(A + p) => w~^w'u e
= 0 rel="nofollow"> c

where we have used Proposition 5.6.11 to describe Stabpj^(A + p). Thus ylr(y^;W^) = ^(w 'W ^) => A = p and wW^ = w'W^. □

Category á for Kac-Moody Algebras

560

To generalize Proposition 4 to the infinite-dimensional case DeodharGabber-Kac restrict the class of allowable elements of i)* and Introduce a correspondingly restricted class of g-modules. We assume IK = R (the case K = C is a minor variation, see the Exercises). Let F be the fundamental chamber for i)* relative to n = {aj\j e j} and set Fo--=F\ U iV , where 5 == {/ c J]3a e A+, supp(a) c I, (a\a) = 0}. Thus A e F q if and only if (0 > 0 for all i e J, and (ii) {(A|a) > 0 whenever a e A+ and (a |a ) = 0}. Define K = \ J wFo c X, w^W := - p + K, F := - p ^ Fo. Observe that K' is closed under the dot-action of W: \ ^ K* => \ + p ^ K => w(\ p) ^ K => w ' X ^ K \ Certainly / g 5 implies that the subroot system A^ of roots supported by I is infinite, since finite root systems do not contain isotropic positive roots. (The converse is not true, however, as any rank 2 hyperbolic root system shows). Thus / e 5 implies that the points of Fj have infinite stabilizers in W (see Proposition 5.6.14) and hence are boundary points of the Tits cone 3£. Thus is 3£ with some part of its boundary removed. is the full subcategory of ^ whose objects are those modules of Û all of whose composition factors L(p,) have p, e K \ This “good” category has a theory similar to that of Û in Propositions 2 and 4. We begin by introducing an equivalence relation « on K \ For A, p, e K \ write A>—p, if there exists a sequence of elements p,j,. . . , p^ = p e K' so that -P i^ P 2 -

6.7

561

The BGG Theorem and Generalization

and define \ ^ /jl if there is a sequence A = Aq,A j ,...,A ^ = of elements of K' so that for each i = A^_i > A, or Evidently A - /i, => A

A^> A^_i.

However, the converse is false.

Proposition 5 (i) A G K \ A^ -p. => ¡JL = (ii) k ^ f l <=>¡1 = W ^ -k .

' k for some a

and p e K \

Proof (i) By assumption p = k - na for some (a,n) e A+(A). Now we prove that a e''^A. Since A e K \ there exists w ^ W with w(k + p) e F q (or IV• A e F). If (ala) < 0, then by the definition of A+(A), (A + pla) < 0 [with equality if and only if (a |a ) = 0]. Since a (see Proposition 4.4.8), we have wa e^'^A^ and (w(A + p)\wa) = (A + p|a) < 0. This contradicts the definition of Fq. Thus (a |a ) > 0 and a Since a g '^^A, g W . From the definition of A+(A), g and rj ^k + p) = p + p, that is, k = fjL, Since K ' is closed under the dot-ac­ tion, p G K \ This proves part (i), and part (ii) follows in the direction (=>) immediately. We prove (<=) in Proposition 4' below. □ Beware k ^— p and p g FT’ do not imply that A g K \ For each equivalence class A^ , A g K “, we may introduce the full subcate­ gory of whose objects are modules of ^ with composition factors L(p) that have fi ^ k ’^ , Proposition 2' For all k ^ K' we have M(k) characteristic subset o/

g

Proof [M(A): L(p)] > 0 => k ^ p

, In particular M(A) p

G

g

and K' is a

and p ~ A by Proposition 5. □

Proposition 4' (i) Every equivalence class o f ~ on K ‘ has the form • A, A g (ii) The equivalence classes o f ~ are in bijective correspondence with the disjoint union o f the cosets U W /W ^ AgF*

by

wW’^ ^ (wW ^) • A.

Category ^ for Kac-Moody Algebras

562

Proo^ Use the proof of Proposition 4 for replacing all occurrences of « , F by F q, and ii* by K \

by □

Proposition 6 Let g be an invariant Kac-Moody algebra and let \ ^ F+. Then for all p e ]^* and for all w {M{w ' A): L(^l)] > 0 <=> /i = H'' • A, where w'

and w < w'.

Proof Note first that since A e F^., we have A+ p G \^ F

f a K\ = W.

Also note that the map W ^ defined by m m ♦A is injective. By Proposition 4' the « equivalence class of A is x-= w ^\ =w \, and by Proposition 2', [M{w ' k) \ F (p )] > 0 = > p e A * = > p , = w'*A for some unique w' e W. Thus we have to prove that for Wy w' e W, (1)

[M{w • A): L(w' • A)] > 0

Suppose that [M(w • A): L(w' • A)] > 0 and w Proposition 1, and by Proposition 5, w' - \ = r, for some )3i,. . . , /3^ A,- ==

w < w'. w’. Then w • A>—w' • A by

r^^-wX

where, if we set r^.

■ ■ ■

K p ^ - w

X ,

i = 0 ,...,k ,

we have A;1-1 It will suffice then to prove that for « e IF, )8 (2)

u • X^rpU • A =» M < r^u.

6.7

The BGG Theorem and Generalization

563

By definition of the Bruhat order, the latter condition is equivalent to l(u) < Kr^u). Now using the strong exchange condition (Proposition 5.3.2), we have l{u) < l(rpu) <=> w

e A+

<=» (Л + p\u~^p) > 0 « (w(A + p)|/3) > 0

(3)

<=> <m(A + p ),)3^> e Z + и *X ^ r ^ u ' A. This completes the proof of (1) in one direction. Since [M{u • A): L{r^u • A)] > 0 <=>M{r^u • A) ^ M{u • A), by Proposi­ tion 1, it suffices to prove that и <

•и

[ M ( w • A): L[r^u - A)] > 0

for u, p as in (2). But by (3), и <



и ' X ^ r ^ u • A,

and by Proposition 1 this is all that we need. It is a fact [R-C,W] that for A e



w, w' g W,

dim Horng(M(]v' • A), M(w - A)) < 1. In other words, there is up to at most one scalar embedding of M(w' • A) in M{w • A). (Exercise 6.12). We combine this with Proposition 6 as follows: Proposition 7

Let A G Then there is an order reversing isomorphism of partially ordered sets between W under the Bruhat order and the set of Verma submodules of M(A) under inclusion: w ^ M (w - A).



Corollary

Let Q be a Kac-Moody algebra of finite type. Let A e P_^. Then M(A) has only finitely many Verma submodules. Furthermore, ifw^^^ is the opposite involution in W, then M(Wqpp • A) c M{w • A) for all w ^ W , and • A) is irre­ ducible.

Category ^ for Kac-Moody Algebras

564

6.8

TRANSLATION FUNCTORS A N D THE GENERALIZED CHARACTER FORM ULA

The Weyl-Kac character formula has a generalization due to Kac and Wakimoto [KW] that allows “fractional weights” to appear. Although we have no need of the formula here, its proof is a very interesting use of the results of Sections 2.12, 5.6, and 6.7 and gives us an opportunity to introduce the translation functors of Jantzen. In its general plan the proof of the generalized formula parallels that of the Weyl-Kac character formula. The novelty is that to keep track of the different terms and to prove that the coefficients are just alternating + l ’s, we need to invoke a considerable amount of the machinery of subroot systems and embeddings of Verma modules. Since chamber geometry is an essential ingredient in our exposition, we will assume throughout that we work over R. The transition to C is not difficult and is left as an exercise. The assumptions are 1. (K = R, 2. g is a finitely displayed invariant Kac-Moody algebra with triangular decomposition ^ = (g+, Q+, depths => i > j. Then M L has a highest weight series (0) = /?o

^1 ^ ^2 ^ ***.

= M <S>L,

where each Rj/Rj_^ is a highest weight module o f highest weight A H- dj. I f Mis a Verma module, then each R^/R^_^ is a Verma module, namely Rj/Rj_^ == Mix + Oj). Proof Let Rj be the U(g)-module generated by [v+(S> f j , . . . , f Vj}, Clearly Kv^<S> L c \JJ=iRj- Let U„(g) be the subspace of U(g) generated by all products of at most n elements of g. Suppose that (C/„_i( 9 ) i; ^ ) ® L c

\J

r

..

Then for u e U„(g), y ^ L, u ■

y) e (m• y+® y

+

(U„_i(9)y^) ®L) n ( U R j ) ,

and so by induction u • v+® y ^ U R j and U„(9)y^® L c U Rj- Thus M ® L = U Rj.

6.8

Translation Functors and the Generalized Character Formula

565

Now g+-(y+® D,) c v+® g+t), c R i-\- Thus u, + i?,_i is a highest weight vector for RJRi_^. Thus is a highest weight module. By induction on i we observe also that .R, = Ey^,U(g_) ■ Vj. Now suppose that Af is a Verma module. We show that R, is a free U(g_)-module with basis {y+® Indeed suppose that Mj, . . . , u, e U(g_), not all 0. Consider the filtration {U„(g_)}“^o> p e Z+ be the smallest integer for which Mj, . . . , « , e Up(g_). Let I <J q < i be such that Then W : = Wj •

+ ® i^ i) +

* * *

+ U ¿



(v ^ (S >

U¿)

00

+ E w* • +® k = \

where each lies in Then == Vj + u'jJ o V V¡^ =h 0, since M is a free C/(g_)-module. Since M ^ L = 0 IK¿;^ and Wq is the component of w in M <8) Jo' we see that w ¥= 0. This proves freeness. The result is now clear. □ Proposition 2 Let fi e K \ V e P^. Then L{p)

lies in

Proof. Form a filtration (0) = c c —• of L ip) <S>L(v) using a basis {i;y} of L(z/) as in Proposition 1. We have Rj/Rj_^ - M ( ¡ + SjX j = 1 ,2 ,..., where dj is the weight of Vj. Now Oj e P(i/) and L(v) integrable (since z/ e imply that Oj is in the Tits cone 3£ and hence that (0y|a) > 0 for all a e"'”A+. Since also jx + p ^ K, we have for any a with (a\a) = 0, (p -\- p\a) > 0, and hence (fi + p 6j\a) > 0. This shows that p 6j p ^ K \ and hence /x + 6>y e K \ By Proposition 6.7.2', Mip, + 6j) e Now we can prove that L(p) If [L(p) ® L(v): L((p)] > 0, then [Rj/Rj_^: L((p)] > 0 for some j, and hence [M(p + 6j): L( 0. By the definition of this means that


Proposition 3 If M e

and A

P+, then M <8>L(A)

Proof Suppose that [M <8>L(A): L(A)] > 0. We have to show that A g K.. The weights of M <8>L(A) lie in the fans (cp + A) i Q+, cp e P(M). In particular X ^ (


Category ^ for Kac-Moody Algebras

566

Let M = *** 3 ries for M at A - A. Each isomorphic to L(Ay) for some Ay e We have

D Mq = (0) be a local composition se­ that involves weights f i > \ - A is

M 0 L( A) = M, 0 L(A) D

0 L( A) d

and for some j\

[Mj 0 L(A)/My_i 0 L(A): L(A)] > 0. Then \ — A ^ (p i successively,

for some weight cp of Mj, so

> A —A. Thus,

Mj 0 L(A)/M,._i 0 L(A) = L{Xj) 0 L(A), [L(A^) 0 L ( A ) ; L(A)] > 0. Since [Mj-. L(Xj)] > 0 => [M: L(Ay)] > 0 have by Proposition 2, L(Xj) 0 L(A) e

Xj ^ K ' (Proposition 6.7.2'), we and hence A e A'. □

We are now able to define the Jantzen translation functors. First we recall Section 2.12. According to Proposition 6.7.2', K' is a characteristic subset of 1^* and the equivalence relation ~ is what is denoted as « in Section 6.7. By Theorem 2.12.4 for any M e ^ ' = M = ®M^, where e and ft runs through the equivalence classes of K' under = . For simplicity we will often denote by if A e ft. We denote by 17^ or the projection functor

M ^M ^. Let A, /X e K ‘. We assume that A, /i satisfy the condition ( 1)

¡X - X ^ di n p.

Then W(/x - A ) n F n P # ( ^ and W(fi - A) n P+= {A} for some unique Ae (Theorem 5.9.2). Furthermore (/x - A, a'^> g Z for all a g ''*A, and hence = A**, (see Section 6.7 for the definitions).

6.8

Translation Functors and the Generalized Character Formula

Let M e

567

Then we define (see [Jz, Section 2.10])

(2)

m M )= 7гJ^M ® L{^)).

According to Proposition 3, M ® L(A) g defines TJ¡^ as a functor Tr-

so (2) makes sense. It obviously

^

Furthermore it is exact: If 0

M'

M ^ M" ^ 0

is exact, then so is 0 ^ M' ®rL(A )

M ®r L(A ) ^ M" ®rL(A ) ^ 0,

which we rewrite as 0

®(M' ® L( A )) n ^ ®(M ® L ( \ ) ) a ^ ®(M" ® L ( \ ) ) a ^ 0.

Since g-maps preserve the types, we have exactness of 0 ^ (M ' ® L (A ))^ ^ (M ® L (A ))^ ^ (M " ® L (A ))^ ^ 0. Proposition 4

(i)

Let M, M' e

M ' c M. Then

and c h T t i M ) = chT>t{M') + chT/^CAf/M'). (ii)

If M G

and M =

■■■ D M,_y z>M, = (0)

is a sequence o f submodules of M, then c h T ^ M ) = E chTJ^{Mj/Mj_,). ; =i (iii)

For all M e c h 7 7 (M )=

E [M :L (c.,)]ch r,^(L (a,)). 0)^P

Category ^ for Kac-Moody Algebras

568

Proof. The proof of part (i) follows from exactness, and the proof of part (ii) follows from part (i). For part (iii) we choose any cp and let M = Mo d M i D

= (0)

be a local composition series at cp. Now either Mj_^/Mj - L{(o) for some has no weights o) > cp A. Thus

(o > (p or

c h M = L ch(My_i/My) y=i = i ; [ M : L(o))]chL(a>)

(mod IK[f)* iG+](
(see the proof of Proposition 2.6.11), and ch r / ( M ) = E chTJt{Mj_,/Mj) = Z [ M : Lico)]chTi^{Lia>))

(mod K [ r i C+li^+A))-

Since this is true for all (p e fi*, we obtain part (iii).



Proposition 5 Let A, ju ^ K' with pt —A e 3£ Pi P. Suppose that for some chamber C of the root system A^, we have A+p^C,

p+p^C.

Then T f{ M { w • A)) = M{w • p)

for all w e W \

Proof Let W{p - A) n {A}. For each w g W^, M { • A) e (Pro­ position 6.7.2'), and Tf{M{w • A)) = 7t^(M(w • A)) 0 L(A)). Let {z;y} be a basis of L(A) as in Proposition 1, Vj e L(A)^>. Then M{w • A) 0 L(A) has a HWS with factors Miw • A + 0y), ; = 1 ,2 ,... . Thus we will be done if we can prove that for exactly one Sj e P(A), w • A + 0y lies in the equivalence class /i* of p, and that for this dj, w • A + 0y = w • p. Since p* = *p = • p (Proposition 6.7.5), we have to solve w

(3)

w • A + 0y = w ' • p

6.8

Translation Functors and the Generalized Charactek form ula

569

for fixed w € and for the variables w' e W^, 6¡ e P(A). Set A' — A + p, ff ■= p! ■•=p + p. Then (3) reads (4)

A' + 0' = vpi,

where ff e P(A) and v e

are variables. If 0' and v solve (4), then

w f = \ \ n ' f - 2 i v p : \ x ) + "^'»^ Use C to define a base for (Exercise 5.12). By assumption A' and are dominant integral for 11^. In particular the weights of the irreducible g^^^-module lie in jj! 1 ( í2 + ^ X s o v / i ' = ¡j ! e N, and {vi¿\X) < (/x'|A') with equality if and only if vjj! = ¡j! (A is strictly dominant). Thus l|0'll" >

Wp’ f

- 2(p’\X) + IIA'II" =

Wp' -

A'll"

with equality if and only if u^j! = However, 6' e P(A) and by Proposition 6.2.9, and the fact that )l¿' - A' = jLi - A e WK, we have 11011" < IIMI" = \\p! - All" with equality if and only if 6' e WA. Comparing the two inequalities, we see that there is only one possibility: 0' e WA and

Vfj! = ij!.

Thus (4) has at most one solution: = w-^Sj =

- A' = /X - A,

6j = w (p - A). Since this is indeed a solution of (3) (with w' = w), we are done.



The proof of the main theorem that follows depends on the clever choice of translation functors. The next result is used in making this choice. Lemma 6 Let A G K \ and assume that (A + p, ^) > 0 for all e n A^.. Assume that A^ ^ 0 a n d that I I is a base for A^ that lies in A+ (Exercise 5.12). Fix any a e n^. Then there exists p e 1^* such that (i)

= 0,


'^> > 0 /or all p

{a},

Category ^ for Kac-Moody Algebras

570

GO W ill - x ) n p ^ i ^ 0 . Proof. It is easy to see that P n is a group that spans Fix any y o ^ P with <7o> ~ Z), and set ¡jlq ■= X yQ — p. Then ^0 + P ^ liQ -X ^P . Let be the Tits cone defined by the subroot system of A (see Section 5.6), and let C be the chamber of 3E^ defined by the base 11^. By the definition of 3E^, C n x 0 , where 3£ is the Tits cone of A. Let be the face of C corresponding to the root a. If B is an open ball in C n x, then the convex hull of B U r^B contains an open subset of lying in n X. The union of the rays from 0 through produces an open cone in lying in C^. Let := i4 ^ P- This is a semigroup. It is nonempty since D P is 2l group that spans and contains open balls of of arbitrarily large size. Let m e M+. For all N ^ Nm e n X, and hence for large enough N, /¿0 + p +

^ ^4’ o

Po

P

~

p) ^

Set jLi := )Lto + Nm. Then p satisfies part (i), and p - X e F n i . Some IT-translate w(p — X) of p — X lies in the fundamental chamber F of A that defines II. Thus w(p —A) e and part (ii) holds. □ Theorem Let q be a finitely displayed invariant Kac~Moody algebra over IR. Let X e K\ and suppose that < A + p ,a^)> 0

for all a ^

C\

Then ch L(A) =

det(iv)ch M(w • A)

— \ dim g®

Proof. Let A denote the equivalence class A of A, and order the elements of A n (A J, 0 + ) according to increasing depth A n ( A i Q + ) = (A = Aq, A j , A2, ...}.

6.8

Translation Functors and the Generalized Character Formula

571

Now we know that chM (Ao)=

E

[M(Ao);L(M)]chL(M),

and since Ag e K \ [M(Ao):L(^t)l

Ag =» /i e {А,|г e 1^}.

Thus (5)

chM(Ag) = E [ A /( A g ) :L ( A ,) ] c h L ( A , ) .

and [M(Ag): L(Ag)] = 1. Since A, e K \ we can repeat this process to obtain chM(A,) = E[ M ( A ,) :L ( A , ) ] ch L ( A ,. ) , ( 6)

[M (A ,);L(A ,.)] = 1,

i=

We may view (6.46) and (6.47) as a system of linear equations whose matrix is of the form 1 * *

1 *

1

We may now formally invert this system to obtain chL(Ao)= ^m ¿chM (A ¿), / =0

e Z, mo = 1.

If = 0 , then of course = {!}, A = {A}, and (5) already gives M(A) L(A). So there is nothing to prove. Suppose that ^ 0 . We rewrite the preceding formula as chL(Ao)=

12 ^(w^)ch M(iv • A),

m(l) = 1,

There remains to prove that m(w) = ( — It is tempting to invoke If"'^-invariance, but ch L ( A q) is not in general WT^-invariant (see comments at the end of this section).

572

Category ^ for Kac-Moody Algebras

Fix a e and choose according to L ^ m a 6. Then A + p e C (C is the fundamental chamber of H^), / ¿ + p e C , —A e X n P . Thus is defined, and by Proposition 5, T¡t{M{w • A)) = M(w • !i)

for all w e WK

We have from Propositions 6.7.1 and 2.11.4, • A => [M(A): L(r„A)] > 0 ^ M ( r ^ A ) -^M(A), SO we have an exact sequence

M(A)/M(r,A) ->L(A) ^ 0 . Now r/(M (A ))

and since Tj^ is exact, we obtain T a L { \ ) ) = (0). Thus 0 = chrr(L(A)) = =

Tj^M{w • A) 53 w(w)ch M(w • p,).

From the independence of characters we have in particular for each w e W^, 0=

52

f n{ u) .

VfJi=WfX However, fi + p lies in the face of F, and hence Stab,^A()u. + p) = {1, r„}. Thus v - p = w - p < ! ^ v ^ [w, wr^, and we obtain 0 = m { w ) + m{wr^).

6.8

Translation Functors and the Generalized Character Formula

573

Starting from m(l) = 1, we then have m(H-)= where /' is the length function for in terms of the generators {r^la e II''}. However, (-1 )'^ ^ is the unique homomorphism of into {±1}, that is, -1 on reflections. Since the length function 1: W ^ [ ± \ ) when restricted to has the same property, we obtain m(w) = ( - 1 )

IM

We have proved that chL(A)=

E

( - l ) ' ^ ’"^chM(w • A).

The rest of the theorem follows from ch M(w • A) =

e(w • A) g“ *

If A e P, then = A, and the formula reduces to the usual character formula (Section 6.4). An example for A ^ P appears in the example of the Appendix. It is somewhat paradoxical that ch L(A) can fail to be PT^-invariant, even though it is the ratio of two PT'^-skew-invariant expres­ sions. This happens in the example of Section 6.7. The following example shows clearly what the problem is. Let Q := Za be an abelian group of rank 1, and set Q +— Z+a. Then K[G >1G+] is an associative (K-algebra and lK[j2] is a subalgebra (Section 2.5). The latter has an involution r defined hy a —a, e(a) <-> e(—a), but this clearly does not extend to K[Q iQ+], Consider e{ —a) — e(a) /== e ( —2a) — e(2a) This is evidently the quotient of two r-skew-symmetric elements of K[Q]- But e(a) — e(3a) / =

1 - e(4a)

= ( e ( a ) — e ( 3 a ) ) { l + e { 4 a ) + e ( 8 a ) H- *• • } = e ( a ) — e ( 3 a ) + e ( 4 a ) — e ( 7 a ) + e ( 8 a ) *• • on which r is not defined.

Category û for Kac-Moody Algebras

574

EXERCISES 6.1 Let A be an indecomposable Cartan matrix of finite type, and let (g, be the corresponding split simple finite-dimensional Lie algebra. Let P be the (unique) weight lattice of (g, (a) Let A e P^. Using the characterization of P(L(A)) of Section 6.2, show that L(A) is finite dimensional. (One can also use the character formula.) (b) Let M e ^ ) . Show that the following are equivalent: (i) M is finite dimensional. (ii) M is integral. (iii) M = 0/!^ i L(A¿) for some Aj,. .. , Ay^^ in P+. (c) Let A e Show that L(A) has a unique lowest weight A* [i.e., A* - a¿ ^ P(L(A)) for all fundamental roots a¿] and that this is a highest weight for g with its opposite triangular decomposition. (d) Show that A* e WA. In fact A* = WqA, where Wq is the opposite involution of W, (e) Let A e Prove that 0 e P(L(A)) if and only if A e g . (Show that A e g+U{0}.) be an indecomposable Cartan matrix. Assume that 6.2 Let A = J is finite. Let P be a minimal realization of A, and consider g := g (^ , R). Let P be the standard weight lattice of g, and let A e P+\{0}. Show that the following are equivalent: (a) g is finite dimensional. (b) L(A) is finite dimensional. 6.3 Let (g, ^ ) be a split simple finite-dimensional Lie algebra over I Let P be its (unique) weight lattice. (a) Let E = and F = Show that there exists an ele­ ment such that ( P , 2 p E) is an § l2-triplet. Let § = KF 0 [K2p^0 [KP [called the principal §I2 subalgebra of (g, 3^)]. (b) Let A e P+. Define the depth of L(A) by dL(A) == max{d(p)|p G P(L(A)}. Consider L(A) as an ^-module to show that dL(A) = + l. 6.4 Let (g, *^) be a finite dimensional split simple Lie algebra over IK: g = Í) e © g“ , aeA where ^

and A c 1^* is a finite root system. Consider the natural

Exercises

575

W^-invariant nondegenerate IK-bilinear form k

: ij X Í) ^

K{x,y) ■■= ^

K,

(x,a)(y,a).

ae A

(a)

Let t : -> 1^* be the isomorphism defined by k. Let ( | • ): 1^* X 1^* ^ IK be given by (T(x)|T(y)) = k( x , y) for all ,y e i. Show that (T(x)|T(y)) = E „ s 4(T(x)|a!XT(y)|a). (b) Show that (;u.|iu.) = for all ¡x e b*. (c) For each ¡x in the weight lattice P, define £>(/x) == e I[P]. Show that D(p) = (e(a/2 ) -e (-a /2 )). (d) For each A e F define I[P] IK[[r]] by e(p) = Show that for A,p e F, f,D (n) =

+■■■,

where AT = 1A+|, and that =

n

OtS A^.

( f 1«) == d^,

^N+1 “ 0, d„

(e)

Let L(A) be the finite-dimensional irreducible g-module of high­ est weight A e P_^, Apply to both sides of the character formula D(A + p) = £>(p)ch(L(A)) to conclude that (a) <¿A+p ^ dp dim L(A) (Weyl’s dimension formula), (b) E c^ÍmIp )^ = (dim L(A)/24)(A|A + 2p), where ch(L(A)) =

(f) Let be the highest root of A (the highest weight of the simple adjoint g-module g). Use the Casimir-Kac operator to conclude that (\ + 2p) = 1. (g) Show that (pip) = dim g/24 (Strange formula). (h) The dimension formula dimL(A) =



n asA+

(A + p|a )

(Pl^)

Category ^ for Kac-Moody Algebras

576

is independent of the choice of PF-invariant bilinear form (*| *) on Í)*. Compute the dimensions of the modules L(A) for the simple Lie algebra of type G2 for the following A: A = (l,0): = 1,

= 0,

A = (0,l): = 0,

= l,

A = (l, l) :< A , ai ^ > = 1 = . 6.5 Let (9, be a minimally realized Kac-Moody Lie algebra. Let Ae Show that the weight system P(A) of L(A) lies in the interior of the Tits cone 3£ iff 5 — {/ e J|
U

C (r,

running over all sequences i^< • • • < in [1, p]. In the next two exercises we obtain a recursive formula (due to Dale Peterson) for the root multiplicities mult(o:) = dim 9", a e for any invariant Kac-Moody Lie algebra and then use it to obtain the Freudenthal formula for the weight multiplicities mult^(A) = dim L(A)^ for any integrable highest weight module L(A). The Peter­ son formula (unpublished) first appears as an exercise in [Ka5]. It appears in more detail in [KMPS]. The Freudenthal formula for the finite-dimensional case is very well known. It is a recursive formula (on depth) and is the basis of most computer algorithms for weight multiplicities. Our proof of it here fully uses the infinite-dimensional setup, even for the finite-dimensional case. For the conventional proof in the finite-dimensional case, the reader may consult [FdV]. 6.7 Let (9, y ) be a minimally realized invariant Kac-Moody algebra with structure matrix A. Begin with the denominator formula (corollary to Theorem 6.4.1), and denote the common value of these formal series by D. Let {a^,{a') be dual bases for relative to (*| *). Then for all a, e ij*, (a\p) = E(o:|«^)()3|a0. Define derivations d-, d' on Q iP iG Jby d^e'^ = ()a|a,)e^

and the “Laplace” operator by

= 'Ld¡d‘.

Exercises

(a)

577

From the sum version of D show that d^D = (p\p)D.

(b)

Compute d‘D /D using the product version of D, expand the terms c(—aXl —e(—a ))“ *, apply д¡, and sum over i to obtain

-

= E mult(a)(a|a) E

(c) Using d^id‘D / D ) = did‘D /D - a‘Da,.D/D^ obtain ^ k rel="nofollow">l

^

mult(a){A:(Q:la) — (a|2p)}e( —¿ a )

asA+

=

E

E

(d)

Set Cp := > i(l/A:)mult()8/ k ) [mult()8/ k ) is understood to be 0 if p / k ^ A+]. Show that (c) can be rewritten as E

C pim -2p)e(-l3) =

(e)

m u lt(a ')m u lt(a " )e (-p a '- ^a").

a',a"eA +

p,q>l

E

c^,c^»(i3'l/3")e(-/3'-r)-

Deduce that for P ^ Q+, (p\p - 2p)c^ = E(i8'li8")c^^V

(f)

when the sum is over all pairs (p',p") ^ Q+>^ Q+ such that P' P" = p. This is the Peterson multiplicity formula. Show that (P\P — 2p) < 0 if j8 is a root and hi p > 1 and hence that the formula effectively determines root multiplicities recur­ sively beginning at mult(a,) = 1, / e J.

6.8 Maintain the notation of the previous exercise. Let A e and use the extension trick outlined after Proposition 6.2.4 to form § based on an extension ^ of >1 so that § has a generator / q that generates L(A) as a g-module. (a) Apply the Peterson formula to obtain for p = ^ G ., (P\p - 2p)mult()3) = 2 ^ m ult(a) ^ (a\p - ka)mu\t(P — ka), aeA+ k>\

Category ^ for Kac-Moody Algebras

578

(b)

Now letting A e A i

and writing P = X, show that

((A + p|A + p) —(A + p|A + p)}mult(A) = 2 ^ muIt(o:) aeA+ k > l

(c)

+ fca)mult(A + ka).

(Note that one first obtains this with p, so it is necessary to see that replacing p by p makes no difference.) This is the Freudenthal multiplicity formula. Prove that (A + plA + p) - (A + plA + p) # 0 if A A, so the formula does recursively define multiplicities.

6.9 Write a program for the Peterson multiplicity formula, and use it to compute some root space and weight space multiplicities. Even for small examples like ^ is quite instructive. 6.10 The theory of category was developed for K = IR. Show that this theory can be generalized to K = C by redefining Fq as A G Fq (a)

Re 0 for all i e J a n d I m ( X , a y ) > 0

(b)

ifRe = 0; (A|a) =5^ 0 if a e A^_ and ( a |a ) = 0.

6.11 Let IK = IR. Given an example of a pair A,p, e 1^* for which A^—p, p e a:-, A ^ K \ Let g be an invariant Kac-Moody algebra over IR with triangular decomposition R = (g+, ij, Q^, a), and let A e We wish to prove that if w, iv' e PL with w <w' in the Bruhat order, then (1)

Honig(M(M'' • A), M ( h' • A)) = 1.

This will complete the proof of Proposition 6.7.7. This extended exercise runs from 6.12 6.30 and except for the final part is based on the paper of Enright [En]. Exercise 6.30 comes from [R-CW]. We fix once and for all j e J, and let ^ == = Cej + Chj + C/y c C ® 55g. We will usually suppress the subscripts j. Many of the exer­ cises depend only on § (not on g) and hence should be considered as part of § 12-theory. We will use the following notation for a e C, M(a) is the Verma ^-module of highest weight a. Its C/z-weight spaces are ie If V is any ^-module then for all n e C, •= {x e V"\ex = 0}.

579

Exercises

The category consists of all g-modules V such that as an ^-module by restriction, El: K is a weight module for Ch, E2: / acts injectively on V, E3: e acts locally nilpotently on V together with all g-module maps between these spaces. When g = ^, we write for Note that for all A e Mix) e A module V of is complete if induces a bijection of onto for all n ^ N . Let K be a module of ^ ( ^ ) . A C/z-weight module Q( K) is a completion of V if the following axioms hold: Cl: Q (F ) is a g-module and there exists an embedding of gmodules i:V --C ,iV ) by which we identify F as a submodule of Q (F )) such that C2: For each n e N for which there is ^-module injection M ( - n - 2)

F,

there is a unique extension to an ^-module injection M (n)^Q (F ). C3: Q ( F ) / F is Ui^)-\oceA\y finite (i.e., each element of the quotient space lies in a finite-dimensional ^-module). 6.12 (a)

For a, b ^ C, a b, Mia) ^ Mib) as ^-modules iñ b ^ N, a = - b - 2. For a e C, Mia) is complete iff « ^ {-2, - 3 , - 4 , . . Any direct sum of complete modules is complete. Let F be a g-module and W a g-submodule. Set F ' := {í; e V\e^v = 0 for some m F" = {i; e Fl/'^z; = 0 for some m ^ N } , V'" = (z; e F|(U(^)z; + W ) / W is finite dimensional}.

(b)

Prove that F', F", F'" are g-submodules of F.

Category ^ for Kac-Moody Algebras

580

6.13 Let V be an §-module that is a C/i-weight module and on which e acts locally nilpotently. Then the Casimir operator 2Y = + 2ef + 2fe = (A + 1)^ — 1 + 4/e acts on V. (a) Show that V = ®^^(V[c], where V[c] is the c-generalized eigenspace of V (see Section 7.1). (b) Show that if x is a highest weight vector in V of weight a and y G 11(5) is a highest weight vector of weight b, then b ^ - a 2. (c) Suppose that X c F is a submodule of V and V / X is U(i)-locally finite. Prove that V is generated by X and [V"\n g N} as an d-module. 6.14 Let V G We construct a completion of V. Let n suppose that z g 2 # 0. Define L , ■■=U(g)

y, and

- 2),

and let be a highest weight vector of M ( —n — 2). (a) Show that there is a g-module map L , ^ U ( g ) -z c F (b)

defined by 1 ® z Let z vary over a basis Z of all the spaces z e Let

« e N, say,

L' == F© e L ,. zeZ

Using (a) construct the obvious map k = L'-^V ,

(c)

k\y=idy.

Let K ’ ■ = ker k so that K' n V = (0). For each t/(g) ®u(g)M(m(z)). Show that there exist g-module embeddings

and L'

== F ©

© L^. zeZ

(d)

Set K q ■■=image (AT') c L, and define K ~ {x ^ L \ f ”x

G

K q for some m

Set F = L / K . Show the following:

z

g

Z let



Exercises

(e)

581

V is embedded in V under the maps

U ^ L

(f) V / V is U(ê)-finite. (g) K is a completion of V, (h) V is in ^ ( ^ ) . (i) V is complete. 6.15 Show that if C is any completion of F, then there is an isomorphism (p\ C of g-modules with (p\v= \dy. [Exercise 6.13(c) is useful here.] Conclude that any completion of V is in and is actually complete. 6.16 Using the uniqueness of completion given in Exercise 6.15, prove that if F is a g-module and we treat it just as an ^-module Fg, then C /F^) has exactly one g-module structure by which it becomes C^(F). 6.17 Show that if 0: F^ F2 is a g-module map, then 0 has a canonical extension to a g-module map 0: €^(¥2). 6.18 Set A = {(¿;, d u ) \ u e F J = graph of 6. Let A = {(jc, y) e Q (F j) X C^(V2)\(x, >0 generates a finite-dimensional i7(ê)-module modulo A}, Show that A is the graph of a function, thus defining 0, (Again Exercise 6.13(c) is useful.) 6.19 This exercise is about § and the category <J^(ê). The main result is to determine the indécomposables in Let n e N. In U(§) define

= U(§){/i + n +

(2ru(,) - «2 _ 2nf } ,

= U(g){/i + n + 2,c'’-"2}, T(n) == U (i)/2W „,S(«) := U(ê)/5R„. There is a natural surjective ^-module map S(n) Tin). For each e C, let := a} + 2a. Let n ^ N. (a) Let L == linear span {/'e^|0 < ; < n H- 1, /, j ^ N}. Prove that U(§) = L 0 9in and Sin) is a free C[/]-module. (b) For 0 < / < n + 1 define to be the C[/]-modulo generated by {e\ . . . , Show that this leads to a filtration of Sin) = 5 q ^ 5i D • • • D + i Z) 5„+2 = (0) whose factors are M i - n - 2 + 20, i = 0 , .. ., n + 1.

Category ^ for Kac-Moody Algebras

582

(c)

Set c := c„ = «^ + 2n. Prove that the c-generalized eigenspaces of the filtration of (b) lead to a filtration of S(nXc] in which S(n)[c] 3 S„^i[c] D(0)

(d)

with S ( m)[ c ]/ S „ + i [c ] = M ( —n — 2) and S(n + iXc] = M(n). Prove that 5(/i)[c] T(n) and hence that there is an exact sequence 0

M(n ) -> T(n)

M( —n — 2)

0.

(e)

Prove that T(n) is indecomposable [use the fact that M(n) and M ( —n — 2) are indecomposable and T(n) is monogenic]. (f) Prove that T(n) e cX(§) and is complete. and A = A[c] (c = c„) and if v e (g) Show that if ^ e then the mapping x xu of Vi(ê) into A factors through T(n).

6.20 In this exercise we determine that the M(a), a ^ C, and the T(n), n Ei Ny are the indecomposable objects of cX(ê). Let A e We wish to decompose it into indécomposables. For this we can suppose that A =A^ for some c = a'^ + 2a ^ C. (a) If a ^ I or a = - 1 , then A^ and A~^~^ are composed of highest weight vectors, whence y4 is a direct sum of modules of the type M(aX M{—a — 2). (b) Suppose that a ^ N . (This covers the remaining cases from (a) since, if ÎÏ e Z_, we can replace it by -¿z - 2). Set L — N := A^. I f N = (0), ^ is a direct sum of modules M { —a - 2). Assume that N ^ (0). All elements of N are highest weight vectors. Let and let N2 be a subspace so that N = N 1 ^ N2- Let Li any subspace of L mapped isomorphically onto N 1 by Let L 2 = Prove that

n L2 = (0) and that L = Lj 0 L 2 ® L 3?

where L 2 0 L 3 is some subspace of L consisting entirely of highest weight vectors. (c) Prove that for any nonzero element x e L^, U(^)x ^ T(a), and hence that U(§)Li is a direct sum of r ( a ) ’s. (d) Prove that U(^)Li + U(^)N2 is a direct sum of ^-modules iso­ morphic to T(n) and M(a), (e) Prove that U(^)L3 is a direct sum of modules M{ —a — 2).

583

Exercises

(f)

Prove that A = U(ê)Li e U(ê)N 2 ® U (ê)L 3 .

Conclude A is decomposable into summands that are of the types Mia), M i - a - 2), and Tia) if a ^ 6.21 Fix n ^ N, and let Lin) be the irreducible ^-module with weights I := { - n , - n + 2 , .. ., Let V Œ C, and form F — Lin) ®^Miv). In this exercise we prove that F e ^ ( ê ) and determine its indecom­ posable components. (a) Set b ■= Ch Ce. Let be the one-dimensional b-module of weight V. Show that L(n) (b)

0 c C ,).

Set Li = 'L/ç^iLin)^, i e I, thereby giving rise to a filtration

where F^ — U(ê) i e I. Show that + 0. Prove that Lin) ®^Miv) e cX(§) and hence that Lin) ®^Miv) is a direct sum of indécomposables, as in Exercise 6.20(f). (d) Write F = ©^^^F[c] (generalized eigenspaces). Prove that if 1/ e Z, then r is injective and hence that F ^ + r). (e) Suppose that v ^ Z. Show that for r,s ^ I, => (after possibly interchanging r and s) (c)

V

+

s = ~iv (f)

r

>

—1 ,

r) — 2 — V.

Set / ' := [r e I\v + r > 0, 5 — —(ï/ + r) —2 — e /}, /" := {5 e I\s occurs in /'} , /" = / \ ( / ' U / " ) .

(Note that if v

r = —1, then r occurs in /"'.) Show that © P[c^+r] ® ®

re/'

+

k ^ I'"

and show that each factor F[c^+i^] == M(/a. + /c), /: e

Category ^ for Kac-Moody Algebras

584

(g)

Prove that for r e /', is indecomposable and hence that T{v + r). [To show that is indecomposable, let v e L(n)“'^ be a lowest weight vector of L{n) so that z; <8> gener­ ates F as an ^-module, and consider the projection tt: F ^

(h)

For n e N, v e C, L(n) M(v + r).

+ r) ®

6.22 Show the following: ©

r(2i)

if n is odd,

©

7(1 + 2i)

0 < i < ( n —l ) / 2

(a)

L{n) ® M( —1) =

M (-l)e

0
if n is even. (b)

if 1/ e N, then © M{v - n

2i)

if V — n > 1,

0
©

T(2i) ®

0<(fi-2)/2

L(n)

<S>M{v)

©

M(2j)

-fji/2<j<(nu+n)/2

if fji '•= V — n is even and < -1 ,

= <

0

M( - 1 ) ®

T(2i + 1)

0siS (/x-3 )/2

©

M(2j + 1) if /i ~ V — 1 is odd and < - 1 .

(c)

Prove that in (a) and (b) above, L(n) ® M(v) is complete.

6.23 Let V G ^ ( § ) , and let L e ^ ( q, T ) be an integrable module. We wish to prove that L ® F e ^ ( § ) and C(L ® F ) = L ® C(F). (a) Show that L ® F e ^ ( ^ ) . (b) Show that C(L ® F ) =) L ® C(F), since L ® C (F )/L ® F is U( §)-locally-finite. (c) Prove that L ® C (F) is complete. [By Exercises 6.16 and 6.20(f) we may assume that g = § and that C (F) is indecomposable. Now use Exercise 6.22.] 6.24 Let A G ]^*(]^ = g° ). Let § = Then prove that Mg(A) is complete if \(hj) ^ - 2, —3,...} and that the completion of Mg(A) is MJitjX) if X(hj) G { - 2, - 3 , . . . } . [Prove that as a ^-modules Mg(A) = ® c W (^ X ]

Exercises

585

6.25 We are now in a position to prove the Horn result (1). By Proposition 6.7.6 it is enough to prove that Honig(M(w' • Л),

M{ w • Л)) < 1.

Show that we can restrict to the case on /(w'). Prove that Z (ry) > /(w ')

= 1, and reason by induction

-A e { - 2 , - 3 , . . . } ,

using the completion function C^. to complete the induction step. 6.26 Establish the Bruhat decomposition of Proposition 6.3.7. 6.27 Prove the corollary to Theorem 6.3.14. 6.28 Let G be the derived group associated with a Kac-Moody algebra g. Prove that Z(Ad(G)) = 1. 6.29 Let ^ be a Cartan matrix and R a minimal realization of A, Form the Kac-Moody algebra g = g(^4, i?). Let G be the associated derived group. (a) Show that the restriction map res: Ad(G) ^ Aut(Dg) is injective. [Write g = f © Dg, i c 1^. Prove that g e ker(res), k => gk = k -\- a^^Kg), where a^^Kg) e Zg. Finally, argue that ker(res) is central.] (b) Suppose that in addition A is symmetrizable. Prove that there is a natural mapping
A ut(D g/Z g).

Prove that (p is injective. 6.30 Let ( tt, M) be an integrable representation of g, and let tt: G ^ GL(M) be the corresponding representation of G. Show that if kerCrr) c i) then keri-rr) c ker(Ad) = ZG. In particular G is a central exten­ sion of Tr(G), and there is a natural surjection tt(G) Ad(G) whose kernel is central. 6.31 Let g be a finitely displayed Kac-Moody Lie algebra. A g-module is said to be weakly integrable if it satisfies condition IM2 of Ch 6.1. Show that the following are equivalent (i) g is perfect (ii) Every weakly integrable g-module is integrable (That (i) => (ii) was communicated to us by Jun Morita)

Chapter Seven

Conjugacy Theorems T h e r e is in f in it e h o p e ; b u t n o t f o r u s.

—F. Kafka

One of the most useful concepts in the theory of finite-dimensional Lie algebras is that of a Cartan subalgebra, a nilpotent subalgebra that equals its own normalizer. A central result of the classical theory is that (in the algebraically closed case) all Cartan subalgebras are conjugate. The main objective of this chapter is to generalize this to the case of invariant Kac-Moody Lie algebras. The discussion is based on Peterson and Kac’s cryptic [PK]. Our treatment is self-contained save for some key parts of Section 7.4. There we need to use the conjugacy theorem for finite-dimen­ sional Lie algebras (the necessary result may be shown by following Exercise 7.6) and some results from algebraic groups, particularly the Borel fixed point theorem. 7.1

L O C A LLY FINITE ENDOM O RPH ISM S A N D JORDAN-CH EVALLEY DECOM POSITIONS

An endomorphism jc of a vector space V over K is locally finite if each v lies in a finite-dimensional x-invariant subspace. A considerable amount of the finite-dimensional theory of linear transformations extends without dif­ ficulty to the locally finite setting. In this section we develop the locally finite theory as far as we need it. Our main result is the locally finite version of the Jordan-Chevalley decomposition theorem. We give a completely self-con­ tained proof of this theorem. This is preceded by a proof of the finite-dimen­ sional version and by a short development of some basic linear algebra, both of which are undoubtedly familiar to many readers. The importance of locally finite endomorphisms from our point of view is that they arise completely naturally in the study of integrable modules of a Kac-Moody algebra g. Locally nilpotent endomorphisms are locally finite.

586

7.1

Locally Finite Endomorphisms and Jordan-Chevalley Decompositions

587

and so are their exponentials. Thus the generators of the derived Lie group G of g are locally finite. In addition the diagonal algebra of g is locally finite, in the sense that it consists of elements that act locally finitely on any module of and hence all the generators of g are locally finite. A few words about the nature of the base field K. For convenience and consistency of notation, K will still denote a field of characteristic 0. How­ ever, in this section such an assumption on K is not necessary. The key to the existence of a Jordan-Chevalley decomposition of a given endomorphism x is that the roots of its minimal polynomial lie in a separable extension of K, and this is the only assumption that we use in the proof. Let F be a K-space, and let x be an endomorphism of V, Consider the polynomial ring lK[i] in one variable t with coefficients in K. Evaluation at x fit) --fix)

determines a ring homomorphism ^ E n d ^ (F ). Notice that makes V into a K[i]-module via f(t)v = f( x X v ) for all v If Endj^(F) is finite dimensional, our map must have nontrivial kernel. On the other hand, K[t] is a principal ideal domain, and it follows that there exists a unique nonconstant monic polynomial p^^yU) ^ K[t] called the minimal polynomial of x such that k e r ( e j =

where < ) stands for “the ideal generated by.” The subalgebra IK[a:] of End^fF) generated by x is evidently

Thus IK[j:] is a field if and only if p^^yit) is irreducible. Let X e End(F). For each polynomial /( i) e K[i] define ■■= (u e F |/ ( Evidently F^ is j:-invariant.

= 0 for some n e N}.

588

Coivjugacy Theorems

Proposition 1 Let V be a finite dimensional K-space. Let x g Endu^(K), and let Px^y(i) be its minimal polynomial. Then V=Y® i=l

where p^^yO) = pft)^^ **• is the decomposition o f p^y{t) into monk irreducible relatively prime factors. Each is x-inuariant and p¿(tY‘ is the minimal polynomial o f x viewed as an endomorphism of Proof. Suppose that / ( 0 = a{t)b{t\ where a (0 and b{t) are nonconstant and relatively prime. We claim that ® V^. In fact, write 1 = a{t)a{t) + p(t)b(t) for some a(t) and p(t) in K[t]. Let V e V f Then V = a(x)a(x)v + p(x)b(x)v. Now b ( x ) a { x ) a ( x ) v = a ( x ) f ( x ) v = 0, so a{x)a{x)v e V^. Similarly p(x)b(x)v e V . Thus V = V V^. Further­ more V Ei C\ V ^ ya(t)aO)+p(tMt) ^ yid ^ showiug that the sum is direct. The first part of the proposition now follows easily by induction (note that for any polynomial /, Finally, let q¿(t) be the minimum polyno­ mial of X acting in V^‘. Then qfOlPiitT for some n, and since p f t ) is irreducible, q f t ) = p¿(tY‘ for some l¿ > 1. Since qf^x) • • • q„(x) annihilates V, we have PxyiOlqft) • • • qJ^O, whence k ¿ < f . But both Px,y(0 and p¿(ty^ annihilate hence also their greatest common divisor which is pftY^. Thus k¿ = /¿. □ The decomposition of V given by Proposition 1 is called the primary decomposition of V relative to x. Let F be a K-space (not necessarily finite dimensional) and let x be an endomorphism of F. x is said to be semisimple if the action of x in F is completely reducible. That is F=

yej

where each Vj is jc-stable and no nontrivial subspace of Vj is jc-stable (i.e., each Vj is an irreducible x-space). x is said to be diagonalizable if there exists a basis of F and a family of scalars {A¿}¿g, such that XV:

=

X:V:

for all i e I.

In other words, there exists a basis of F consisting of eigenvectors of x.

7.1

Locally Finite Endomorphisms and Jordan-Chevalley Decompositions

589

To say that x is semisimple is equivalent to saying that V is completely reducible lK[jc]-module. Thus by Proposition 1.6.2 we have Proposition 2 Let V be a K-space, and let x e End[j^(K). The following conditions are equivalent: (i) X is s e m i s i m p l e , (ii) V is the sum o f simple IK[jc]-modwfe5. (iii) V is the direct sum o f simple ^x\-modules, (iv) Every ^x^subm odule M o f V admits a supplement. That is, there exists a submodule N o f V such that V = M ^ N. □ Proposition 3 Let V be a K-space, and let x be a semisimple endomorphism of V. I f W
for all f { t ) e K[t],w g V.

The map a: K[i]

V,

given by fiO

= f{x)(v).

is a surjective K[/]-module homomorphism. Since IK[i] is not irreducible as a K[t]-module, ker a # (0), so ker a = (p (r)), where p(t) is monic and irre­ ducible. Also p(x)(V) = 0, since /?(a:)(í;) = 0 and i; generates V. Thus p(t) is the minimal polynomial of x in V. Finally, V « K[t]/(p(t)}, and hence V is a finite dimensional K-space.

590

Coi\jugacy Theorems

Conversely, choose ü e F such that IK[;t]i; = V, and define a: K[t] V as above. Since the minimal polynomial pit) of x is irreducible by assump­ tion, we see from pit) e k era that k era = (pit)). Thus F « K[t]/(pit)}, which shows that V is an irreducible K[r]-module, that is, an irreducible x-space. □ Proposition 5 Let V be a finite dimensional K-space. Let x e End^iF). Then for x to be semisimple, it is necessary and sufficient that each o f the irreducible factors of its minimal polynomial has multiplicity 1. Proof. Using Proposition 1 we see that F is a semisimple x-space if and only if each of its primary components is semisimple. Thus we reduce to the case where the minimum polynomial has the form p i t Y , p i t ) irreducible. If h = f, then F is a IK[t]/]. It follows at once that it is completely reducible. If k > 1, then W ••= [v ^ V\pixY~'^v = 0} is a nonzero proper x-invariant subspace of F. If W were to admit an ;c-invariant supplement N, then p i x ) N c ATn IF = (0) from which p ix Y ~ ^ V = p ix)'‘~ \W + N ) = (0). Thus IF has no such supplement, and hence F is not completely reducible. □ Let F be a K-space, and let F be a field containing K. Let Fp = F ®^V. If X e End^CF), then there exists a unique F-linear extension Xp of x to an endomorphism of the F-space Fp that satisfies Xf-. a ® V

a ®x(v)

for all a e F, u e F.

When F is finite dimensional we let char^ p.(t) and p^ yit) denote the characteristic and minimal polynomials of x on F. Proposition 6 Let Vbe a finite-dimensional K-space. Identify K[i] inside F[i] on the natural way. Then (i) char_, p,(i) = char^^ (ii) Px.v^t) = p,,^yft). Proof Since p^^yixj:) e EndpiFp) annihilates F, it annihilates Fp. Thus p^p j/p(i)|P;c.F(i)- On the other hand, let {A,} be any basis for F over K, and write p^p ,/f(0 = EA,/,(i), for some unique f f t ) e K[i]. We have 0=Px,.Vf(x^) = EA,./,.(xp) e Endp(Fp). Restricting to F, we have 0 = EA,/,(x) from which f f x ) = 0 for each i.

7.1

Locally Finite Endomorphisms and Jordan-Chevalley Decompositions

Thus exercise.

591

leave part (i) as an easy □

The next result is well known and easy to prove. Lemma 7 Let V be a finite-dimensional K-space, and let x e End[j^(K). Let K be the algebraic closure o f IK, and consider e End(IK<S>(|^i;). Then the roots of p^ y{t) in IK are the eigenvalues o fx ^. □ The roots of Px,y(0 together with their multiplicities are called the spectrum of x. Proposition 8 Let V be a K-space, and let x e Endj^(F). The following conditions are equivalent: LFl: Every element o f V belongs to a finite-dimensional x-invariant subspace ofV, LF2: For all v the span o f the family is finite dimensional. LF3: There exists a family {Vj)j ^ j o f finite-dimensional x-invariant subspaces of V such that V = Ey^j^Proof Clear.



An endomorphism x of a IK-space V is said to be locally finite in K if x satisfies the equivalent conditions of Proposition 8. Proposition 9 Let X be a semisimple endomorphism o f a K-space V. Then x is locally finite. Proof. By definition K is a sum of x-invariant irreducible spaces and by Proposition 4 each of these irreducible spaces is finite dimensional. Thus x satisfies LF3. □ Lemma 10 Let X be a locally finite endomorphism o f a K-space V. I f x is injective, then the restriction of X to every x-invariant subspace o f V is surjective. In particular x is an automorphism o f V. Proof. If W is an x-invariant subspace of V, then clearly x is locally finite in W. Write W = E y ej^? where each Wj is finite dimensional and x-invariant. Then xWj = Wj for all j, and hence xW = Lj^jxWj = W. □

592

Coi^ugacy Theorems

Proposition 11 Let ¥ be a field containing (K, and let x e End,,^(F). Consider Xp = 1 0 EndpiKp). Then x is locally finite if and only if x^ is locally finite.

e

Proof If Xis locally finite, then write V = (LF3). Then = E/eiF ® Vi, and each F 0 is finite dimensional (over F) and x^ invariant. Thus x^ is locally finite. Conversely, if x is not locally finite, then there exists v such that the K-span of [x^v\n e l\l} is infinite dimensional. Let be an infinite linearly independent set of this span. Then {1 0 ^ {( X ( p )''( l 0 u)\n e N } is an infinite linearly independent subset of over F.

□ Proposition 12 Let Vbe a K-space, and let ¥ be a field extension o f K. Let x End|,^(F), and consider the endomorphism x^ ofV^ = ¥ 0| kI^* Then forx to be semisimple it is necessary and sufficient that x^ be semisimple. Proof If either a : or X p is semisimple, then either a : or X p is locally finite (Proposition 9), and hence both x and jcp are locally finite (Proposition 11). We can therefore assume that V = E/eil^, where each is A:-invariant and finite dimensional. Thus Kp = E¿ei(^)F» (I^)p is JCp-invariant and finite dimensional (as an F-space). Now X is semisimple <=>x|i/ is semisimple for each i <=>JCp|(K,)p is semisimple for each i <=>jcp is semisimple. The only nontrivial equivalence is the middle one. However, by Proposition 6, x\y. and ^ pI(i/) f have the same minimal polynomial, and the equivalence now follows from Proposition 5. (Here we need to know that irreducible polyno­ mials over IK do not have repeated factors in F. This is true as long as F is a separable extension of IKand happens in the characteristic 0 case.) □ Proposition 13 Let Vbe a K-space and x an endomorphism o f V. The following are equivalent: (i) X is diagonalizable. (ii) X is semisimple, and all the eigenvalues of x lie in K. (iii) X is semisimple, and its irreducible subspaces are one dimensional. Moreover, if these conditions hold then x acts diagonally on every x-invariant subspace o f V.

7.1

Locally Finite Endomorphisms and Jordan-Chevalley Decompositions

593

Proof, (i) => (ii) Suppose that x is diagonalizable. Then there exists a basis of V consisting of eigenvectors of x. The corresponding eigenvalues are all the eigenvalues of x. Part (ii) then follows. (ii) => (iii) Since X is semisimple, V = where each is an irreducible jc-space. Let p f t ) denote the minimal polynomial of x restricted to V¿. By Proposition 4, p f t ) is irreducible. By Lemma 7 and by assumption p f t ) = t — a¿ for some e K. Thus x acts on like scalar multiplication by so is one dimensional. (iii) =» (0 Clear. Finally, if PT c K is an jc-invariant subspace of V, then x is semisimple on W, and all eigenvalues of x in PT are eigenvalues of x in V. Thus x acts diagonally on W. □ Proposition 14 Let X be an endomorphism of a K-space, and let IK be the algebraic closure of K. Then for X to be semisimple j t is necessary and sufficient that be a diagonalizable endomorphism o f 1K<S)[|^K Proof The result follows from the last two propositions.



Proposition 15 Let V be a K-space, and let S c End|,^(F) be a set consisting o f semisimple endomorphisms that commute with each other. Let E be the subspace o f End[,^(K) spanned by 5, and suppose that E is finite dimensional. Let A be the associative subalgebra o f End,,^(F) generated by E. (i) (ii) (iii)

Every element o f A is a semisimple endomorphism o f V. I f E admits a basis consisting o f diagonalizable endomorphisms, then there exists a basis o f V on which all elements o f A act diagonally Let ^ = Lie(^) be the Lie algebra o f the associative algebra A. Then is an abelian Lie algebra. I f the assumption made in (ii) above holds then the ij-module V admits a weight space decomposition.

Proof, (ii) Let {xi,. . . , jc„} be a basis of E, and suppose that all x^ are diagonalizable. It is clear that A is generated hy x ^ ,. .. , jc„ as an algebra. We establish (ii) by induction on n. If n = 1, then A = !K[jcJ, and the result is obvious. Assume that the result holds if E is of dimension n - 1. Let S' = {^2, . . . , x^}, and let A' be the subalgebra of End„^(F) generated by S'. By the case n = 1 we can write AGIK

where i; e P^ <=>x^v = \v.

594

Coixiugacy Theorems

Fix A Then A' stabilizes V^, since v E: and / ' e A' implies that X if 'v = f'x^u = Xf'v. Since are diagonalizable, it follows from the induction hypothesis that we can find a basis of in which A' acts diagonally. Since each of these basis vectors are eigenvectors of and x^ and A' generate A, the result follows. _ (i) Let JCi,. . . , be a basis of Fi’jionsisting of elements of 5. Let IKbe the ^gebraic closure of K. We set_F = 1K0 F, and let = 1 0 jc- e E^jj^(F). If A is the subalgebra of Endjj^(F) generated by the 3c/s, then >1 = 1K0^. By Proposition 14_all the x /s are diagonalizable, and hence by part (ii) we conclude that A consists of diagonalizable, hence semisimple, elements. Now part (0 follows from Proposition 12. (iii) f) is abelian, since is generated by commuting endomorphisms. If assumption (ii) holds, we can find a basis {Vj}j^j of V such that hvj = \j(h)vj, Xj(h) e IK, for all j e J. It is immediate that the mapping Ayi h Xj(h) is a linear functional on and hence V = □ Locally nilpotent transformations were defined in Section 1.5. Evidently they are locally finite. Lemma 16 Let F be a field containing IK, and let x e Endj^CF). Then (i) for X to be locally nilpotent it is necessary and sufficient that Xp be locally nilpotent, (ii) if X is both semisimple and locally nilpotent, then jc = 0. Proof (i) The proof is straightforward. (ii) Since X is semisimple, x ^ is diagonalizable (Proposition 14). By part (i), x^ is locally nilpotent, so 0 is its only eigenvalue. Thus x ^ = 0, and hence X = 0. □

Let F be a finite dimensional IK-space, and let x e End,,^(F). By a JordanChevalley decomposition of x we understand a pair (s, n) where 5 is a semisimple transformation of F, n is a nilpotent transformation of F, s and n commute, X = s n. Note Observe that in such a decomposition both s and n commute with jc.

7.1

Locally Finite Endom orphism s and Jordan-C hevalley D ecom positions

595

Theorem 17 Let V be a finite-dimensional K-space and x e Endu^(F). Then there exists a unique Jordan-Chevalley decomposition ( 5 , n) o f x. Moreover (i) s and n are polynomials in x with zero constant terms, (ii) a subspace U of V is x-invariant if and only if it is s and n invariant, (iii) every endomorphism o f V that commutes with x commutes with both s and n. Proof Let K be the algebraic closure of IK. Then Px,viO = ( i - “ 1)*' ■■■{ ( where a^,. . . , a ^ e IK are all distinct. Case 1. . . ., e IK: By the Chinese remainder theorem applied to IK[i], we can find a polynomial f( t) e IK[i] such that f ( t ) = a, mod(r —

for all i,

f ( t ) = Omod t. (The last congruence is redundant if V-=^vEi V\{x — ol^Y' v = 0

= 0 for some /.) Define for some n e Klj.

Then by Proposition V= where each is jc-stable. Define s = fix), and note that 5 is a polynomial in x with no constant term, and hence each is 5-stable. To compute the action of s on write / ( 0 in the form / ( 0 = « ,i + Since g^ixXx - a^)^‘ annihilates (Proposition 1), it follows that s\Vi is scalar multiplication by a,, so s is diagonalizable and hence semisimple. Define n = x — s. Then n is a polynomial in x with no constant term. If e then nv^ = (x - s)(Vi) = (x - a¿)(v¿) so that n^‘ annihilates Thus n^ = 0 where k •= max{A:/,. . . , k j , and hence n is nilpotent. We have shown that x admits a decomposition of the required type. It remains to be shown that such a decomposition is unique. Suppose that X = s' n' is any other such decomposition. Note that s' and n' commute with 5 and n because the latter are polynomials in x and that s' and n' commute with one another. We have s — s' = n' - n, and by Proposi­ tion 15, 5 — 5 ' is semisimple. It is obvious that n' — n is nilpotent. Then by Lemma 16, s = s' and n = n'.

Coiyugacy Theorems

596

Case 2. The general case: Let F = , a„), then F is a finite Galois extension of IK. Let Vp == F and consider e EndpCKp) = F End|}^(F), By Case 1 we have a Jordan-Chevalley decomposition Xp = Let [e^,. . . , 6/} be a IK-basis of V, Then {1 0 , 1 ® c j is an F-basis of Fp. Let X, S, and N denote, respectively, the matrices of Xp, 5p, and Wp with respect to this basis. Observe that since jcp(l 0 F ) = 1 0 x(V) c 1 0 F, the matrix X has all of its entries in IK. For all a e Gal(F: IK) and for all matrices M with coefficients in F, let denote the matrix obtained by applying cr to each of the entries of M. We have X = X ^ = {S

= S^ +

Since 5 is diagonalizable (see Case 1), it is clear that so also is 5"^. Similarly is nilpotent, since = ( N ^ y . Finally, = ( S N y = ( N S y = N^S^, By the uniqueness of the decomposition of Xp into semisimple and nilpotent parts, we have S =

and

N =

for all o- e Gal(F, K) ,

and therefore both S and N have all their entries in IK. This shows that 5p and «p determine endomorphisms of F, which we will denote by s and n, respectively. Then 5p = 1 0 5, Wp = 1 0 n, jc = 5 + n, and sn = ns. By Proposition 12 and Lemma 16 it follows that s is semisimple and n is nilpotent. It remains to be shown that both s and n are polynomials in X with no constant term. Choose a basis {Aq, A^, . . . , A^} of F over IK such that Aq = 1. By Case 1 there exists / ( 0 e F[i] such that 5p = jCp/(jCp). Write f{t) in the form /(0 =

¿ A , ® / , ( 0 e F ® ^ K [ i ] = F[/] ;=o

for some (unique) fj{t) ^ IK[i]. We have 1 ® s -

(1 ®

a: ) ( 1

® / o( ^ ) ) =

(1 ®

D

A; ® / y ( j : ) j .

Now the left- and right-hand side of this equality are linearly indepen­ dent elements of F 0 IK[jc] over IK. Hence both sides vanish, and therefore s = xf^ix). Similarly for n. It is clear at this point that parts (i), (ii), and (iii) hold. □

7.1

Locally Finite Endomorphisms and Jordan-Chevalley Decompositions

597

Remark 1 Let W (z V be an x-invariant subspace. Let {s, n) be the Jordan-Chevalley decomposition of x in V, Then both s and n stabilize W, We know that s acts semisimply and n nilpotently on W. Thus n\w) is the Jordan-Chevalley decomposition of the restriction x \ w Next we generalize the concept of Jordan-Chevalley decomposition to locally finite endomorphisms. Theorem 18 Let V be a K-space, and let x be a locally finite endomorphism o f V. Then x decomposes uniquely as a sum X

=s

n .

where s is locally finite and semisimple, n is locally nilpotent, s and n commute. (i) if W
and

n{v) = (Jilt/)N (f)-

If U' is any other such space to which v belongs, then v s U + IT and U + U' is j:-invariant and finite dimensional. By Remark 1 we have (^l£/)i =

and

(Jtlt/Oi =

Thus

This shows that s is well defined, and similarly for n.

598

Coi\|ugacy Theorems

Since X is locally finite, we can write V = in LF3. Because of the way in which s and n are defined, it is easy to see that s stabilizes and acts semisimply on each l^, and hence s is locally finite and semisimple as an endomorphism of V; n stabilizes and acts nilpotently on each and hence n is locally finite and locally nilpotent as an endomorphism of K; X = s n and s commutes with n, since this is the case in each K. Next we prove parts (i) and (ii). (i) Let W be an jc-invariant subspace of V. Let w ^ W, and consider a finite dimensional ^-invariant subspace Í7 of F to which w belongs. Then in U both s and n act like polynomials in x. Thus sw and nw belong to U <^W, showing that W is 5-invariant and Az-invariant. In addition {s\w,n\w) is the Jordan-Chevalley decomposition oí x\w because of the way in which s and w were defined. (ii) Let y e End|}^(F) be such that xy = yx. We have to show that y commutes with both 5 and n. By LF3 it will suffice to show that ( 1)

sy\u = ys\u and

ny\u = yn\u

for all finite-dimensional jc-invariant subspaces U of V, Let U be such a subspace. For convenience set x = x\u, and let x = s + n ho the JordanChevalley decomposition of x in U. Let x = x\yu. Note that x stabilizes yU and that the diagram

u ‘1 u

y

y^

yU

yU

commutes. If f( t) e K[t], it follows that (2)

f ( x ) y u = yf { x ) u

for all u ^ U,

Let gU) and h{t) in K[t] be such that s = g(x) and ñ = h(x). Define s = g (i) andñ = h(x). We show that s is semisimple and ñ a nilpotent transformation of yU, First observe that both s and ñ leave yU stable, since they are polynomials in x. To show that s acts semisimply in yU, write U= where U¿ is 5-stable and irreducible. Then yU = Eyt^, and 5 will be semisimple if we can show that each yU¿ is 5-stable and irreducible. Let u¿ e Then by (2) (3 )

syu¿ = g(x)yUi = yg(x)u¿ = ysu¿ e yU¿,

7.1

Locally Finite Endomorphisms and Jordan-Chevalley Decompositions

599

Furthermore, if N czyU¿ is an 5-stable subspace, then, using (3), we see that M := {u¿ e U¿\yu¿ e Ñ} is an 5-stable subspace of U^. Hence either N = ( 0 ) or N = yU¿, showing that yU¿ is an irreducible 5-space. This estab­ lishes that 5 is semisimple (Proposition 2). To see that ñ is nilpotent, choose k ^ N such that n ^ U = 0 . Then n'^yU = h { x Ÿ y U = y h ( x y u = yn*i/ = (0). Having established our claim, we observe that (5, n) is the Jordan-Chevalley decomposition of x i n y U . Indeed, if y u ^ y U , then (5 +

n )y u

=

g ( x ) y u

=

yxu

=

+

h ( x ) y u

= y (g (jc ) +

h ( x ) ) u

Scyu.

Thus Jc = 5 + Я in y U . We can now finish the proof of part (ii). For this we have to establish (1). If MG [/, then syu

=

{x\yu )^yu

=

y g ( x )u

=

=

syu

=

=

ysu

g ( x ) y u

=

y {x \u )sU

ysu .

From this it follows that y n = n y . Uniqueness is established as in the finite-dimensional setting of the theorem. □ Given a locally finite endomorphism x we will denote its semisimple and nilpotent parts by x^ and Xj^ respectively. If no confusion is possible we may simply denote this by 5 and n . Proposition 19 L e t X b e a lo c a lly f in it e e n d o m o r p h is m J o r d a n -C h e v a lle y d e c o m p o s it io n . I f

o f a K -s p a c e

F is

an

is t h e J o r d a n - C h e v a l l e y d e c o m p o s it io n o f x ^

K,

a n d le t x

e x t e n s io n o f in

th e n

=

s +

n b e it s

= 5p + «Р

F

By Proposition 11, x ^ is locally finite, and hence the Jordan-Chevalley decomposition exists. Now use Proposition 12, together with Lemma 16 and the uniqueness of the Jordan-Chevally decomposition, to complete the proof. □

P ro o f.

We briefiy recall some basic results about eigenspaces and generalized eigenspaces. Our objective is Proposition 23 which says that, just as in the finite dimensional case, a locally finite endomorphism of a vector space over IK is triangularizable if and only if all its eigenvalues lie in the field IK. Let x be an endomorphism of a IK-space V . For each A e IK define the A-eigenspace V \ x )

:=

{v

e

V \x v

=

\v )

600

Coiyugacy Theorems

and the generalized A-eigenspace V^{x) :=

e V\{x - A)”i; = 0 for some n = n{v) ^ N]

of X in V, If X is understood from the context we sometimes write instead of V^(x) and V \ x ) , respectively.

and

Proposition 20 Let X be an endomorphism of a K-space V,and let IK be an extension of K. Let K := IK K and jc = 1 <S>jc e End^iV). Then for all A e K, (i) Vfix) and V \ x ) are stable under x, GO V^(x) = k ^ V , ( x X (iii) I f X is locally finite and x c is the semisimple component o f x then = ^ "(^ 5)Proof (i) The proof is straightforward. (ii) Let be a basis of the K-space K. Any u ^ V can be uniquely written in the form V=

® /el

Thus for A e K, (x ~ \)^u = (1 <S>X — 1 <8>A)”l5 = (1 0 (jc —A))”C = E a , ® (ac /el from which part (ii) follows. (iii) V^ix) is x-stable, and hence jc^-stable. By Proposition 5 we see that X5, which is locally finite, acts on K;^(x^) like scalar multiplication by A. Thus Vjf^x) c K/X5) = ^^(x^). The reverse inclusion is clear since for v e ^^( a:^), ( x ~ X)^v = ((^5 - A) + Xj^)^u = 0 for k large enough, given that Xp^ acts locally nilpotently.



Proposition 21 (i) The sums tmd direct. (ii) if V - ^AeiK^A^-^) tmd U is an x-stable subspace o f V, then U =

7.1

Locally Finite Endomorphisms and Jordan-Chevalley Decompositions

601

Proof, (i) Since V \ x ) c it will suffice to show that the sum is direct. Let Aq, Aj , . . . , A„ be distinct elements of K, and let j;, e i = 0 , . . . , r. Assume that ^0 =

+

+ Vr-

We want to show that Vq = 0. Let « q. be chosen so that (x A,)"'f, = 0 for all 0 ^ i < r. Consider P(t) and Q(t) in K[i] given by ^ ( 0 = n ( i - A , ) " ', 1= 1

Q(t) = ( t - x , y \ Then P( x ) vq = Q( x ) vq = 0, and hence Vq = 0, since P(t) and Q(t) are relatively prime. (ii) Let u e U, and write u = where 5 c K is finite and e F^(x). We show that each g U; the result is then clear. We choose N ^ N so that (x — = 0 for all A g S. Choose A g 5. By the Chinese remain­ der theorem we can find a polynomial p (t) g K[i] so that p ( t) = 0mod(r -

for all ¿li e 5 \ {A}

and p{ t) = lm o d (t - A)^. Since p(x) stabilizes U, we have p(x)u = e U.



Proposition 22 Let V and W be vector spaces over K, and let X, y e EndOF). Then ^"a(^ ) ® WJ^y) c

p.

^ K. Let x

g

End(F),

( F ® W)j, +^(x ® 1 -I- 1 ® y), (F® ® y).

Proof. The proofs of both statements are similar. We prove the second. Let u ® w G F;^(x) ® W^(y). Then (x ® y) —X p ) ^ ( v ® w) = [(ji ~A) ®y -l-Al ® (y —ju,)]^(i; ®w) in \

= N

=

- A) ® y)^(Al ® (y - p ) ) ^ ~ \ v ® w)

N y J(JC - A)'A^ ^v<&yj(y -

and this latter expression is 0 for A » 0.

•'w,

Coi\jugacy Theorems

602

Here is a typical application of this result. Suppose that 9 is a Lie algebra of derivations of an algebra A. Suppose that V, W are g-submodules of A under this action. Let дг e g. Then Vj(,x)Wj^x) c (V W \^ J ix ). In fact we have the commutative diagram V®W

------------------------- »

V(»w

X ~ { \ + f x)

where m is the multiplication m: A the proposition.

A ^ A, and the result follows from

An endomorphism x of a vector space V over IK is called triangularizable if there exists a totally ordered basis B of V such that XV ^ ^ K m u^B

(4)

for all v e B.

u
We then say that x is triangular with respect to B. We say that x is strictly triangularizable if XLJ e ^ u^B u
Ku, for a\\ u ^ B

Proposition 23 Let X be a locally finite endomorphism o f a vector space V over IK. Then the following are equivalent Tl: T2: T3: T4:

X is triangularizable All the eigenvalues o fx {in some algebraic closure o f IK) belong to IK F= V=

Proof. Let K be an algebraic closure of K. The result being obvious for V = (0), we assume that V (0). Tl_=> T2: Let B be a basis with respect to which x is triangular. Let y e K® F be a A-eigenvector for 1 ® jc, and write y = ® u for some u<.v

V E: B, where c^. = 1,

e IK for all w, almost all c,^ = 0. Then

Ay = (1 ® x ) y = L U < V

Hence ACy = c^,a^J^ and A e IK.

® E ^wu^W
7.1

Locally Finite Endomorphisms and Jordan-Chevalley Decompositions

603

T2 =►T3: If X is semisimple, then by Proposition 13 x is diagonalizable, and T3 obviously holds. In general, write x = x^ + Xj^. Then we have from Proposition 20(iii), K ( x ) = V,(xs), and the result follows. T3 => T4: Use Proposition 21. T4 =* Tl: Let ^ be the set of all totally ordered linearly independent sets B of vectors in V for which (5)

for all V ^ B.

XV

u&B u
Let us first see that ^ is not empty. Since x is locally finite, any nonzero vector y e K lies in a finite dimensional subspace F that is stable under x. By T4 and Proposition 21(ii) we have F = © F / jc). A s is well known there is a basis of each F / jc), and hence F, for which x has a triangular form. Briefly (x —A) is nilpotent on F/jc), and hence F /x ) has an ordered basis for which (x —A)i; c E IKw for all v g B^. Stringing these bases together ueBx gives us the required basis B of F. Thus B satisfies (5), which shows that Partially order ^ by an order-respecting inclusion. Then, in choosing a maximal element B^^^^ in apply Zorn’s lemma to If B ^ ^ were not a basis of V, we could choose y e K, which is not in the linear span ( B ^ ^ ) of FjnaxF containing y with basis B, be chosen as above. Choose a subset C = {ci,. . . , c^} c F so that C U B^^^ is a basis of F + and for all ; = we have xcj e L^^jKcj + ( B ^ ^ ) , Then C U B ^ ^ may be to­ tally ordered by using the orderings of C and B^^^ and by decreeing that w > y for all w © C, z; © It is easy to see that C U B^^^ © which contradicts the choice of B ^^. Thus B ^ ^ is a basis of V and part (i) is proved. □ In the sequel we will find it necessary to work with Lie algebras of linear transformations. We are interested in extensions of the classical theorems of Engel and Lie that tell us that certain Lie algebra of transformations are simultaneously triangularizable. Let t be a Lie algebra over IK and let (ir,V) be a representation of t. Then t is ( tt, F)-triangularizable, or triangularizable on V if there is a totally ordered basis F of K such that F satisfies (5) for all x = ttUX í ^ t. It is convenient first to introduce a more restrictive concept. Let F be a vector space. A flag in F is a sequence F = subspaces of F such that (Fl) (F2)

K ^K -i^

^ y i ^ y o = (0), dim - j.

604

Coi^jugacy Theorems

By abuse of notation we will often identify F with its top space For example, when we say that e F, we mean that v ^ Let t be a Lie algebra, and suppose that tt is a representation of t on V. A flag F = {FJ}/Lo ^ said to be t-stable if 7r{i)VjdVj

forallO
We say that t is ( tt, K)-hoistable if every element of V belongs to a t-stable flag in V, Observe that if this is the case, then the elements of t act on V as locally finite endomorphisms. If t is a subalgebra of a Lie algebra g, then we say that t is hoistable in g if it is (ad, g)-hoistable. Let t be a Lie algebra, and let ( tt, F ) be a representation of t in which every element 7r(x), jc e t, is locally finite. We say then that V is 7r(t)-locally finite. Proposition 24 Let ( tt, K) be a representation of the Lie algebra i. I f i is {7r,V)-hoistable, then it is ( tt, V)-triangularizable. Proof The proof is a simple adaptation of the proof of T4 => T1 in Proposi­ tion 23. □ Proposition 25 Let t be a finite-dimensional Lie algebra, and let ( tt, F ) be a locally finite representation of t. Then

(i) 7r(t) is locally finite in the sense that for each v (ii)

(iii)

^ V, v lies in a finite-dimensional Tr{t)-stable space, (EngeTs theorem) I f for all jc e t, 7t(jc) is locally nilpotent, then t is ( tt, F ) = hoistable. In particular t is ('Tr,V)-triangularizable, In fact it is strictly triangularizable, and for all x g t, tt{ x ) has only the eigenvalue 0. {Lie's theorem) I f 7r(t) is solvable and for each x G t 7t(jc) is triangularizable, then t is {Tr,V)-hoistable,

Proof, (i) Let V theorem.

F, and let [t^,. . . ,

be a basis for t. Then by the PBW

ir(U (t))(t;) = u (U (K O ) • • • 7t(U(K íi ) ) ( í^), and this is clearly finite dimensional and 7r(t)-stable.

(ii) Let i; G F. Then U '= 7r(U(t))(i;) is finite dimensional and 7r(i)-stable. By the finite-dimensional Engel theorem (Exercise 1.22), there is a flag F= with U^ = U such that Tr(t)L^ c ; = 1 ,..., n, and part (ii) follows from Proposition 24.

7.1

Locally Finite Endomorphisms and Jordan-Chevalley Decompositions

605

(iii) Since for all X e t, 7t( a:) is triangularizable, all the eigenvalues of all the 7t( x ) lie in K. Let v ^ V, and let U ■= 7r(U(t))(i;). Then by the finite­ dimensional Lie theorem (Exercise 1.22) we can find a 7r(t)-stable flag F for U, □ The notion of t-hoistable is far more restrictive than t-triangularizable. For instance, let K be a vector space with basis {?;oj • • •)? define endomorphisms i = - 1 , - 2 , . . . of K by

a^Vj = 0

ii j

0,

Then t := is an abelian Lie algebra of nilpotent locally finite transfor­ mations and is visibly triangularizable. But t is not locally finite and hence not hoistable. Proposition 26 Let A be an algebra over IK. Let x be a locally finite endomorphism of A (as a K-space), and let X=s +n be its Jordan-Chevalley decomposition, (i) (ii)

I f X is a derivation o f A , then both s and n are derivations o f A, I f X is an algebra automorphism o f A , then both s and 1 s~^n are algebra automorphisms o f A.

Proof. Extending the field if necessary, we can assume that IK is algebraically closed. Indeed, let F be a field containing (K, and let x^ and A^ be as above. By Proposition 19, X^ — 5|p

/Ip

is the Jordan-Chevalley decomposition of x^ as an endomorphism. Evidently, if 5p (resp. /ip) is a derivation of A^, then s (resp. n) is a derivation of A. Likewise, if s^ is an automorphism of A^, then s is an injective homomor­ phism of A. Since s is locally finite (Proposition 9), it follows that s is surjective (Lemma 10). Thus s is an automorphism of A. Assume then that K is algebraically closed. Let U and V be finite-dimen­ sional x-stable subspaces of A. Let UV= [Zuv\u G i/, z; e K}. Then UV is finite dimensional, and it is j:-stable whenever x is a derivation

606

Coi^jugacy Theorems

or an algebra homomorphism of A. Let m

(6)

u=

n

0 c/,, ¿=1 '

v=

P

© 1 / , UV= ® ( U V ) y „ ;=1 k=l

be the generalized eigenspace decompositions of U, V, and UV with respect to X. Suppose that ;c is a derivation of A. Using Proposition 22 (see in particular the remarks following it), we obtain

Thus, if u ^ U and £; e F, we have (7)

s{uv) = (A + fi)uv = Xuu + ujjLV = s{u)u +

By (7) and LF3 of Proposition 8 we conclude that 5 is a derivation of A, and therefore n = x - s, being the difference of two derivations, is also a deriva­ tion. Next suppose that x is an automorphism of A. Once again by Proposition 22 we have c (C/F),^. It follows that for all u ^ and v e F^, s(uv) = XjjLUU = s{u)s(u) and hence that 5 is a homomorphism of A. To show that s is surjective, it suffices to show that s is injective, and this is clear because the spectrum of s is the same as that of x and 0 is not an eigenvalue of x. We have therefore shown that s is an automorphism of A. Finally, 5(1 + s~^n) = jc, so 1 + s~^n is also an automorphism of A. □

7.2

LOCALLY FINITE ELEMENTS IN KAC-MOODY ALGEBRAS

In this section we investigate the relationship between (1) ad-local finiteness and (2) local finiteness on integrable highest and lowest weight modules for a Kac-Moody algebra g. Remarkably (1) => (2), a result that is important for the conjugacy theorem of Section 7.4. In the meantime we use it to establish an abstract Jordan-Chevalley decomposition of locally finite elements of finitely displayed Kac-Moody algebras. Lemma I Let Vbe a K-space, and let x ,y ^ End|,^(F) be locally nilpotent. Then (i) if V ^ V, the linear span o f the set {exp tx(u)\t e K} is the smallest x-invariant subspace o f V containing u; (ii) if exp tx = exp ty for all t ^ K, then x = y.

7.2

Locally Finite Elements in Kac-Moody Algebras

607

Proof, (i) Let n e Z^. be such that x"v = 0. Then the smallest x-invariant subspace of V containing v is spanned by {x'l; | i = 0 ,1 ,..., n — 1}. Let / q, t i , . • •, t„-i be any n distinct elements of IK^, and consider the n vectors exp tjx(v) = v + tjxv +

tfx^

tj

+

We then have the matrix equation V XV

1 (1)

.n-\

tn

X^V

(expi^x(i;)) =

:= M n —\

X^V Jl

''n —\

(n -l)! and since the Vandermonde matrix M is invertible, part (i) follows. (ii) Given V ^ V, choose n e Z+ such that = 0 and let io,... ,tn-i distinct elements of IK. Define M as above. Then (1) gives M

x^v

=M

y^u

7T

so XV = yv because M is invertible. Lemma 2 Let I be a Lie algebra and let t and a be subalgebras o f I such that [t, a] c a. Let ( tt, V) be a representation o f I and suppose that (i) ad Í : a ^ a is locally finite for all t (ii) there exists a finite dimensional subspace S of V which is 7r{i)-invariant and generates V as an a-module. Then t is TT-locally finite. Proof Let F be the subspace of V consisting of all elements that lie in some finite-dimensional 7r(t)-invariant subspace of V. The lemma will follow if we show that F = V. Let V ^ F and x e a. We show that ( ) e F. Set tt

x

v

M = 7r{U(t))v(zV

Coivjugacy Theorems

608

and A^:= ad(U (t))jc c a . By assumption both M and N are finite dimensional. Thus the space Tr{N\M) spanned by all elements of the form 7r(n)(m) with n ^ N and m e M is also finite dimensional. If i e t and Tr(n)(m) e Tr(N)(M), then Tr(t)Tr(n)(m) = 7t([í , n])(m) + 7r(n)Tr(t)(m) e Tr(N)(M), since [t, n] ^ N and TrCtXm) e M. This shows that 7t(N)(M) c F, In particular irixXu) e F, and hence F is 7r(a)-invariant. On the other hand, F contains S, and 5 generates V as an a-module. Thus V = F. □ In what follows we use the notation that was introduced for Kac-Moody algebras and groups in chapters 4 and 6. Lemma 3 Let q be a Kac-Moody Lie algebra, and let G be its derived Lie group. Then U j^ j(A d G^)ej spans Q+. In particular is spanned by elements which are locally nilpotent on every integrable representation o f g. Proof Let 5 be the subspace of g spanned by all elements of the form Ad g+{ef) such that g+E G+ and j e J. Clearly S is an Ad(G+)-invariant subspace of g+. Let i e J and i; e 5. Then exp(ad te¡){v) = Ad exp te¿{v)

e

5

for all i

e

K.

By Lemma 1 we conclude that [e^,v] e S. On the other hand, ej e 5 for all E J, showing that g+c 5. If ( tt, V) is an integrable representation of g, then by Proposition 6.1.4

j

7r(Ad(g)e¿) = 7r{g)Tr(e¿)Tr{g)~^

for all g ^ G.

Since the right-hand side of this identity is locally nilpotent in V (by definition of integrable), the last assertion of the lemma follows from the first. □ Remark 1 It is clear that in the above lemma G+ can be replaced by G_ (and the ef^ by /y’s). Proposition 4 Let Q be a Kac-Moody algebra, and let m be a subalgebra o f codimension. Let P be a weight lattice for g. Then for any A ^ P+, ann^(^)(m) := [v E L(A ) | m • i; = 0} is o f finite dimension.

o f finite

7.2

Locally Finite Elements in Kac-Moody Algebras

609

Proof. Let < • I • > be the Shapovalov form on L(A) defined by our anti­ involution a (See Ch. 2.8). By Lemma 3 there exists jc^, . . . , e U yej Ad(G+)ey such that m together with these x¿, span g+. Then ax¿ e U Ad(G_)/y, and so using Proposition 6.1.13, a ( x f ) , ... ,a(xf^) act locally nilpotently on L(A); in particular they are locally finite. Let V ■= U(IKc7-(jc^)) • • • U(lKcr(xi)) • £;+ where v+ is a highest weight vector for L(A). Then dimu^CF) < oo. By PBW we have L ( A ) = U ( c r ( g ,) - : ; , = U(o-(m)) • U(J
= U (o -(m ))I/cU ^ (o -(m ))L (A ) + F.

Let z e L(A). Then 2Gann¿(A)(m)

>m • z = (0) « < U ^ (m ) - z |L (A ) ) = 0 « < z |U + ( a ( m ) ) •L (A )) = 0.

Thus by (2), each z e ann^^^^Cm) is determined as a function on L(A) by its values on V. Since ( • I • > is nondegenerate and dim F < oo, dim(ann^(^)(m)) < oo. □ Proposition 5 Let q be a finitely displayed invariant Kac-Moody algebra with weight lattice P. Let t be any finite dimensional ad-locally finite subalgebra o f g. Then for all Ae t is 7T^ and Tr^-locally finite. In particular ad-locally finite elements are 7T^ and Tr^-locally finite for all K E: P^ (for the definition of see Proposition 2.3.5). Proof. Fix an arbitrary A e P^, We show that t is Tr^-locally finite. The idea is to construct a finite dimensional 7r^(i)-invariant subspace A of L(A) containing v^. The result then follows by Lemma 2. We construct A as the subspace of elements annihilated by an ad t-invariant subspace of finite codimension in g+. Since dim t < oo, t c Eht(a>>-A/9“ some M ^ N. Set b = ]^ + g+. Then [t, b] c Eht(a> > so b + [t, b] = b + a for some fi­ nite dimensional subspace a of g. Let F := ad(U(t))b d b. Then dim F /b < oo. Indeed ad t(b + ad(U(t))a) c b + a + (ad U(t))a = b + ad(U(t))a, and ad(U(t))a is finite dimensional. Thus b c F c b + ad(U(t))a (in fact we see that F = b + ad U(t)a). Consider F-^ relative to the proper invariant bilinear form assumed to exist on g. Since g““ and g“ are nondegenerately paired for all a e A+, and since F D b, we have F c b c b. Furthermore F c Eht(a)> some

610

Coiyugacy Theorems

N > 0 , so Eht(a)>N9^ showing that dim (b/K ^) < 00. V-^ is ad t-invariant, but we need an ad t-invariant subspace of g+. To this end set M = V nD g, which is also t-invariant because dq is. Now M c b PiDg c To prove the last inclusion, simply note that b and Dg are both b-invariant, so it suffices to show that (b n Dg) n b -^ = (0). From Section 4.4, IBF, we have b n Dg = for k e \ {0}, {k lb) = (A:®, b> ^ (0). Thus M c g_^, so M = F P i g ^ . Since the projection K b obtained by annihilating the g+ component has kernel M and dim b < Qo, M has finite codimension in hence in g^.. Let m denote the subalgebra of g+ generated by M. Then m is t-in­ variant and of finite codimension in g+. By Proposition 4, A — ann^^^^fm) is of finite dimension. Also A is Tr(t)-invariant: For a y e m, t e t, Tr{y)Tr{t)a = 7r([y,í])í2 + Tr(t)7r(y)a = 0. Since v +^ A and L(A) is generated as a g-module by 7r(t) is locally finite by Lemma 2 (applied with I = g = a, 5 = A). To show that t is Tr^-locally finite, we apply what we have proved to the locally finite algebra □ Corollary Let % be a finitely displayed invariant Kac-Moody algebra with Cartan matrix A. Let A be a sub-Cartan matrix of A , and let q be a subalgebra o f g obtained by restricting A to A (Section 4.3, Remark 1, and Proposition 4.3.2 and 4.3.3). If i is a finite-dimensional diá-locally finite subalgebra o f g, then t is an did-locally finite subalgebra o f g. Proof Let b be the diagonal subalgebra of g. It is clear^ that t is a (finite-dimensional) subalgebra of g + b- Moreover, since [t,b ] c g, t acts ad-locally finitely in g + b- By the reduction result of Proposition 6.2.4 and Proposition 5 we conclude that t is ad-locally finite in g. □ We will eventually prove that locally finite elements of finitely displayed invariant Kac-Moody algebras have Jordan-Chevalley decompositions. We have here a weak form that only involves the adjoint representation. Proposition 6 Let q be a finitely displayed invariant Kac-Moody algebra. Then every adlocally finite element jc g g decomposes as (3)

a:

= a;5 +

7.2

Locally Finite Elements in Kac-Moody Algebras

611

where is 2id-semisimple, is locally 2id-nilpotent, and = 0. This decomposition is unique up to addition of elements from the centre of g. Furthermore (i) For any subspace M of [ a:, M] c M <=> [jc^, M] c M and GO g"" =

n

[ x j ^ , M] ( z M,

(see Section 1.1 for notation).

Proof Let A be the structure matrix of g, and suppose that A has dimen­ sion / X /. If ^ is singular, let ^ be a symmetrizable nonsingular Cartan matrix of dimension (/ + corank X (/ + corank A ) in which A is embed­ ded as a sub-Cartan matrix (see Lemma 4.2.1). Then the minimally realized invariant algebra g with structure matrix A has a Cartan subalgebra § of dimension (/ + corank A). Use Proposition 4.3.2 to embed g in g. Because of the dimension of the Cartan subalgebra of g must be all of If .^4 is nonsingular, then we set g = g. In either case g is centerless, andhence all derivations of g are inner (Proposition 4.1.15). Since X is ad-locally finite, it is also ad^-locally finite (corollary to Proposi­ tion 5). Then by Theorem 7.1.18 and Proposition 7.1.26. ad x is uniquely expressible as where X^ and Xjs^ are, respectively, semisimple and locally nilpotent derivations of g and [X^,Xj^] = 0. Since they are inner derivations ad X = ad ^5 + ad Xj^ for some unique (g is centerless) x^, Xy^ e g and [x^, Xj^] = 0. Let n be the normalizer of g in g. Then n z> g Z) 6, and so n = ©Ofe A ^ But, ii a ^ Q and x e n “, then g z> [x, if] = (Kx. Thus n = g. Now, since x^ and Xy^ normalize g (as x does), we see that x^, Xj^ e g. The remaining parts (i) and (ii) follow from Theorem 7.1.18(0 and (ii). □

Proposition 7 Let Mj, M2 be integrable Q-modules in ^ ( P ) , and let S be a G-invariant subset of Mj. Then M5 := {/ e Homj^(Mi, M2) I /(5 ) = (0)} is a q-submodule o f H ohI kÍM i , M2). Proof. It suffices to prove that c and that for all a e and e g", e^ • c M^. We use the subgroup 2Í of G to establish the first and the subgroups G “ == exp(g") for the second. Let / e M5 . Let F^ c Mj be a finite dimensional A^-invariant subspace. Since /(F j), is finite dimensional and the action of X is locally finite, we can

e^

Coixjugacy Theorems

612

embed / ( jPj) in an A^-invariant finite dimensional subspace F2 of M2. Then we can consider f\f^ as an element of the A"-invariant finite-dimensional space Homj^CFi, F2). By Remark 6.1.6, and F2, hence also Hom^(Fi, F^), are ]^-modules. Thus for h ' f)\r^ = h • ( / I fj) ^ ^om^(Fi, F^)- Fur­ thermore M^l/Tj is an AT-invariant subspace of Homu^ (Fj, F^), and hence by Remark 6.1.6) again, it is 1^-invariant. In particular h ' / \ fi ^ Now every element of Mj lies in some finite-dimensional ^-invariant subspace Fj of Mp and hence any g e Homj^(Mp M2) is determined by its restrictions to such spaces. Since h - f E: M^I fi spaces, h •f ^ M5. This proves that • M^ c M5. For the second part repeat the argument using the groups G“, but this time invoking Lemma 7.2.1. □

7.3

THE KOSTANT CONE

Throughout this section (g, ^ ) will denote a finitely displayed invariant Kac-Moody Lie algebra over K. As usual ^ = (i), g+, Q+, cr). Let P+ denote the set of dominant integral weights of some weight system F. If A e F+, the g-module L(A) is integrable (Proposition 6.1.5), and L(A) ® L(A) is com­ pletely reducible (Corollary to Theorem 6.5.1). Moreover, if (A,i;+) is a highest weight pair for L(A), then (2A, i; + 0 1;+) is a highest weight pair for L(A) 0 L(A), and we see that

(1)

L(A ) ® L(A ) = L (2 A ) ® © n^L(yii) <2A

for some nonnegative integers n^. Given A e P+, we define the Kostant cone T(A) by ( 2)

r ( A ) = {y e L ( A ) It; ® v g L(2A)} \{ 0 } .

In this definition it is understood that v ® v is decomposed according to (1). 5^(A) is a cone in the sense that V(A) c 3^(A). Let G be the group associated to g (Section 6.1), and let G be its derived group. Then G acts on L(A), hence on L(A) ® L(A), and stabilizes the decomposition (1). Hence for g & G,v ^ T(.A) => gv ® gv = g(v ® u) g |( L ( 2A)) = L(2A) =» gi; G T(A), so V{A) is stable by G. Define an action of the group IK^X G on T(A) by ( a , g ) v = a(gv).

7.3

613

The Kostant Cone

Theorem 1 [PK] K^X G is transitive on TiK). The proof of this theorem is the focus of this section. We begin by expressing X(A) as the solution space of a specific set of quadratic equations. Let be dual bases (relative to the invariant form of g, see Section 4.4) for g“ and g““, a e A, 1 < / < dim g“. We can clearly take if a ^ 0, and it is convenient to assume this. Set Q ^= 0 .^ and as is customary. Proposition 2 Let A c P_^, Then T{K) is the set of nonzero solutions in L(A) 0 L(A) of the equation

(A 1A)(í; ® u) =

(3)

Y. ae A i

Proof Let r = + T' be the Casimir-Kac operator of L(A) (Section 4.5). If y G L(A), then T (u

u)

r®(£; 0 ¿;) + P(i^

=

v).

Now F ( ¿ ; <S> V) = 2

Yi aeA+

® i

= r ( i ) ) ® i; + y ® r '( y ) + 2 Y a e A+

+2 Y

Y^X^aV ® yi'^V

a e A+

= r(u )

® i

I

V + V ® r(v) + 2

Y

® yi'^i’

a G A\{0} i

(using (4)

Thus r ( ü ® ü) = r ( y ) ® Ü + y ® r ( u ) + 2

+ r^ (i; 0 í;) — T ^ ( v ) W riting

u=

w h ere

e L (A )^ ,

Y Y^a^^ ® ya^^ a G A\{0} i

<S> V — u <S> T ^ ( v ) .

^ P, and using the fact that

614

Coivjugacy Theorems

acts on L(A)^ as scalar multiplication by (/jl + 2p\ fi), we have (5)

r ^ ( v (8> u ) ~ r ^ ( i ^ ) (8> u — u (8> r ^ ( i ^ )

=

( ( m + i' + 2 p I jll + i ' ) -

H

(

p

-h 2 p I p )

/1, i/eF - ( u + 2 p l v))v'^ ® d " =

2

^

(/i, 1

® u"

= 2 Y, fX.V^P

® yo \v'^ ® i

= 2Y,X q^ ® y o \ ^ ® ^)-\ Combining this with (4), we obtain (6)

r ( i ; <S> z;) = r ( z ; ) <8) f + í; 0 T( i; ) + 2 51

®

ae A /

Now z; G L(A), and therefore F(z;) = (A + 2p | A)z; [Proposition 4.5.3(i)]. Thus r(z; 0 z;) = 2( A H -2p|A )z;0z; + 2 52

®

ae A /

Thus (3) is equivalent to (7)

r ( v 0 z;) = (2(A | A) + 2(A + 2p | A))z; 0 z; = 4(A + p I A)i; 0

V.

Using (1) decompose v ® v = Yiv 0 z;)^, {v 0 v)^ e L(p,), p e (2A 4 Q+) n into components using (1). Then (7) holds if and only if for each p with {v 0 i;)^ ^ 0 we have ( p

+

2 p

1 p )

=

4( A

+

p I A )

[Proposition 4.5.30)]. However, for p = 2A - a, a e Q+U{0}, (2A —a + 2p |2A —a) = (2A + 2p|2A ) - ( q:|2A ) - (2A - a + 2p | a ) < 4( A + p | A) with equality if and only if a = 0 (since 2A,2A —a e P^). Thus (7), and hence (3), is equivalent to z; 0 z; e L(2A). □

7.3

The Kostant Cone

615

Let V e and write v = where e L(A)^ for all Recall that the support of u, supp(i;), is defined by supp(i;) = {)Lt e

I

e 1^*.

=?i=0} c A + 2-

The arguments that follow involve a detailed discussion of supp(z;). Let A be the /-dimensional real affine space A = R with translation group F = R = ©¿^jRa,. Identify A + F with A by identifying A + o' with a e A. This allows us to think of supp(¿;) as a finite subset of the real affine space A. Recall that a mapping / : A -> A is called an affine linear transformation if there is a linear mapping df :V ^ V such that f ( x - \ - u ) = f { x ) + df {v)

iox dX\

X

^ V.

If A" c A and / : A ^ A is an affine linear transformation of A, then ( f ( X ) ) = f i x ) , where < > stands for “convex hull of.” The Weyl group W acts on F in the standard way. Let w ^ W . We can view w as an affine linear transformation of A by writing H^(A + a ) = A + (wA - A) + w{a)

for all a e F.

(Note that the last two summands lie in F.) It is easy to verify that this gives a group action of W on A. Let V e y{A), and let S ( v ) c A be the convex hull of supp(i;). An element ¡i e S ( v ) is said to be a vertex of 5(i;) if VI

M ^ S(v),

V2 there exists an (affine) hyperplane H of A through fjL such that S ( v ) \ { f j i } lies entirely in one of the open half spaces separated by H, By an edge of S ( u ) we will understand a pair of distinct vertices {A, for which there exists an (affine) hyperplane H of A such that

of

S(v)

E l the closed line segment [A, joining A and /x lies in H, E2 S ( v ) \ [A, ] lies entirely in one of the open half spaces separated by H, ijl

In broad outline the proof of Theorem 1 runs as follows: Let be a highest height vector of L(A). Evidently + e V(A). Thus we have to prove that 1K®G • u += T(A). We take any element u of TiA) and show that the vertices of S(u) lie in WA. We then select the “lowest” vertex and proceed to strip edges off S{v) by repeatedly replacing v by elements g • z;, g e G for which Sig ' v) has less edges than S{v). Ultimately we arrive at an element u

616

Coivjugacy Theorems

for which 5(¿;) has no edges. Then v ^ defined in Section 6.1, and we are done.

where N is the subgroup of G

Lemma 3 Let g = ^ that L(A) =

^

grading o f g by (R, + ) satisfying Qq = suppose is an U-grading o f L(A) compatible with that of g: g^ • L{A)t c L{A)s+t

(i) (ii)

for alls, i e R.

If V ^ L(A)^ n V(A) for some r e R, then v e L {A Y ^ for some w ^W . Let V e T{A), and write v = e ^(A)^ for all 5 e R. // m = max{5 e R | =?t 0}, then e ViA).

Proof (i) We first show that if a e A, then g" c g^ for some 5 e R. It suffices to show this for a = ±a¿, i e J. Clearly s ¥= 0 if a ^ 0. Write e- = E jc^, jc^ e g^. Then for all /i e 1^, E [/i, Jcj = [h,e¡] = a¡{h)e¿ = £ a¡{h)x,. S&U S^U But [h, jrJ e g^, since = gg. Thus [h, x j = af h)x^, and we conclude that there is only one s with x^ 0, and this x^ lies in g"'. This shows that g“' c g^. The argument for g““' is similar. Suppose that u e L(A)^ c V(A). Then (Proposition 2) ( A | A ) ¿ ; 0 ¿ ; = Y, ae A i

The left-hand side of this lies in L(A)^ ® L(A)^, whereas x*¿^v ® y^'^v e L(A),+j ® L(A)^_^ for some s, and s 0 unless a = 0. Thus (A I A)u ® i! = E^o^^ ® Writing

V

=

with

e L(A)'^ for all

( Al A) i i ®i ; =

f i

e P(A), we have [see (5)]

iiJi\v)v>^ ® v ’', !X,vE.P

SO(A I A) = (/£ I v) whenever 0 that V = for some p e B^A.

=?^=0. By Proposition 6.2.9, we conclude

7.3

The Kostant Cone

617

(ii) The R-grading of the g-module L(A) induces a compatible grading in L(A) 0 L(A) by setting (L (A ) ® L (A )),=

L

L (A ),® L (A ),.

By restriction L(2A) inherits this grading, for the argument by which we showed that g"' c for some s can be used to show that the highest weight space L(A)^ of L(A) lies in L ( A \ for some s. Thus u + ^ u + ^ L(A 0 A) 255 and it follows that L(2A) is graded. Let V be as in (ii). Then since v ® u ^ L(2A) and v v = HS, / € U^S ® with deg(z;^ u^) = s t < 2m, we see that 0 is the homogeneous component of degree 2m of u u in L(2A). In particular e T(A). □

Lemma 4 Let A" be the usual n-dimensional real affine space. Let S c. be a finite set, and let (S ) be its convex hull. Let X (Z be a countable set. (0 Suppose that there exists Sq ^ S and an {affine) hyperplane H o f A" satisfying (ia) Sq ^ H n X , (ib) ( 5 >\ {5q}lies entirely in one o f the open half spaces separated by H. Then there exists an {affine) hyperplane H ' satisfying (ia) and (ib) and such that in addition (ic) (ii)

H'nX={s^}.

Let c Ei {S), and suppose that there exists an {affine) hyperplane H of A" such that < 5 )\{c} lies entirely in one of the open half spaces separated by H. Then c e S.

Proof, (i) Let R" be the real vector space of translations of A". For each V E R", <5> V is the convex hull of the set 5 + i;. If we now translate 5, X, and H by - 5 q, we see that we can suppose that Sq = 0. Choose a basis [u^, f 25 • • • 5 of such that {v2, . . . , is a basis for H and • / / = 0, where • is the usual inner product on R". Since 5 \ {sq} is finite and lies entirely in one of the open half spaces separated by H, we can suppose that there exists e > 0 such that

^\

{*^} ^R"I^ >e}0

618

Coi\iugacy Theorems

For each s ^ S \

set t/^ == {w e R" I 5 • M> e}.

Then

is open, and i;i € i/ :=

f l U,. s^S\{so)

For each a e A"\ {0}, //^ •= {w e R" | w • a = 0} is a hyperplane. By the Baire category theorem, we can choose a point w ^ U \ \J ae x\{0)^a' The hyperplane H' ■= {x ^ W \ x ' w = 0} satisfies (ia), (ib), and (ic). (ii) Suppose that c ^ S. Then by assumption 5 lies in one of the open half spaces, say, separated by H. Since is convex, <5> c a contradic­ tion. □ Lemma 5 Let V e y{K). Then the following two sets are equal: (i) The set of vertices o f S(u). (ii) supp(i;) n Wh., Proof Let /X be a vertex of S{v), By Lemma 4, /x e suppiu), and we can find an affine hyperplane of A through fx such that / / ^ n ( A + 0 ) = {m}, and S(v) \ {ju,} lies entirely in one of the open half spaces, say, separated hyH^. Let H be the unique hyperplane of V (translation group of A) satisfying = H ti. Choose p e V so that p, + p ^ Then V = H ® Rp. Define d:V^R by means of the projection of V onto Rp parallel to H: d{h + tp) = t

for all h g H, í g R.

If we consider the restriction oi d to Q c.V , it follows from our hypothesis that d{a) = 0 if and only if a = 0. By means of the group morphism d:Q ^ R

7.3

The Kostant Cone

619

we can define a grading of 9 by (IR, + ) by setting 9 , ==

E { 9 “ U ( a ) = t}, ol^Q

for all i e R. By construction Qq = i). Similarly we can give L(A) an (U, + ) grading by setting L(A ),== E { L ( A r " “ |d ( « ) = r} a^Q (with

defined as above). By our choice of p we see that V

e E M A ), i<0

and that L ( A ) '‘ = L ( A ) o .

Since the grading of L(A) is compatible with that of Q, we apply Lemma 3 to conclude that if i; = ^ ^(A), then Uq = ^ T(A) and p e H^A. Conversely, let p e w k n supp(¿;). Let w and « e N lie over w, i.e. n = [w\. Let u e cp e 1^*. Then nu = # 0, and clearly supp(«i;) = vv’CsuppCi;)) and S ( n u ) = w5(¿;). Thus to prove that /x is a vertex of S ( u ) , we may assume that p = A . But it is obvious that if A e S i u ) , then A is a vertex, since all other weights in supp(¿;) lie in A —(2+. □ Lemma 6 Let V e V(A), Then the edges o f S(u) are parallel to real roots o f g. Proof Let V = e L { A Y , and let [ \ , p ] be an edge of S(u). Then \ ¥= p, so (X \ p) ¥= ( A \ A). Look at the component for L i A Y L { A Y in (A I A )v

V

=

Y

,

®

namely (A

I

A)u^

=

Y

®

(or,
where F = {(a, (p,il/) \ a ^ A,

cp

a

= k,

if/

— a = p}. If for all (a,

cp,il/)

^ F

Coi\jugacy Theorems

620

we have a = 0, then

(A I A ) f ®

0 i

= (A I

0

which we just saw is impossible. Thus there is an a e A \ {0}, for which A - a and + a lie in supp(i;). By assumption S{v) \ [A, /x] is in one of the half open spaces defined by some hyperplane H containing If either A - a or + a does not belong to [A, ¡ \ then the midpoint ^(A + fji) of the line segment [X - a, + a] lies in contrary to |(A + /x) e [A, /x]. jl

jjl

jjL

a

It follows that A —a and fx a must lie on the line through A and /x. Thus a is parallel to [A, /x]. Writing X — fx = ka, k ^ U, and choosing w ^ W so that wX = A, we have A —wjx = kwa. Thus kwa e Reversing the roles of A and jjL, we find that —kw'a ^ Q+ for some other w' g W. Thus a is a nonzero root whose IT-orbit meets both 0 + and —Q+. By Proposition 4.1.5(iv) we have a e*^®A. □

Lemma 7 (i) For a

and X e WK, (A + Ua) n W X = {A,r^A}.

(ii)

Every edge ofS(v), v e

is o f the form [A, r^X] for some real a.

7.3

The Kostant Cone

621

Proof, For A + A:a e WK = W \, (A I A) = (A + A:a I A + fca) = (A I A) + 2 k { \ \ a) + k'^{a \ a) k = 0 or

k = —

2(A I a) ( a Ia )

hence we have part (i). Now let [A, fjb] be an edge of S(v), v e By Lemma 6, n WK for some real root a, and hence, by part (i), ¡i = r^A.

e (A + Ra) □

Next we gather together a few definitions and simple results that are used in the process of “stripping off edges.” For A e P^, A e WK, define i/(A) =

Pi

wG_w~'^

w G i W , wA.

n

G^,

=A

which is clearly a subgroup of G and '®A+(A) = {a

1r„A > a).

Note that we use the usual convention that wG_w~'^ makes sense since H normalizes G_. (Remark 6.3.2). Lemma 8 Let A e

and let A e WK. Then

(i) is finite, (ii) a e*^®A+(A) <=> exp g“ c i/(A). Proof Let A = wA, a

Then r^A>A <=i> < 0 <=> < ^

w

A —1a '

,

< 0

622

Coiyugacy Theorems

and is finite by Proposition 5.2.3. This proves part (i). Now using Proposition 5.2.6,

9“ =

“w ' c wg_w ^

Thus a e*^^A+(A) => exp g“ c wG_w~^ Pi G+. We now prove Theorem 1, namely that

□ G • u^= V(A).

Proof of Theorem 1. It is clear that IK®* G • f +c T{k). As for the reverse inclusion, let V e T{A). Partially order Q by the height function, and transfer the order to A + Q- Let A be minimal in the set of vertices of S{v). If A has no edges from it, then S(u) = {\} [5(z;) is the convex hull of its vertices], and u e L(A)'^ = L(A)’^^ some w ^ W. Then u e K^nv+, where (n ) = w. Suppose then that S(u) has at least one edge, say, [A, r^A], a g A+. Write r^A = A + ka, and let Uj be the component of v in L(A)'^'^-'“, ; = 0 ,1 ,..., A: (k is positive by the minimality of A). Look at exp te^ • v and its component in tfc-iefc-i k\

-Vn +

( A :- ! ) !

+

If iei/j \)v^_j = ajv^, Oj e then this reads (i*a. + k-1 + *** -\-aQ)Uf^. In an algebraic closure (Kof IKwe can find i = io to make this 0. Then at least in ^ (A ), r^A ^ supp(exp t^e^u). Let / / be a hyperpl^e through [A, r^A] so that 5(i;) \ [A, r^A] (zH ^. Then supp(exp c and since r^A is not in the support, S(txp tQe^u)\{\} c / / ^ . In particular A + a ^ supp(exp tQe^u), so io^a^o + = 0. Thus e IK. We now replace u by expio^a^^) so S ( u ) \ { \ } If r^A,)3 e A+, is another edge then [A, r^A] points “into” Thus supp(exp se^v) \ {A} c //+; in other words, when we remove more vertices, we cannot add a back again. It remains only to recall that from Lemma 8(i), {a

I r^A > a}

is finite.

A finite number of repetitions of the process just described removes all the edges from 5(z;). □

7.4

7.4

Coiyugacy of Split Caitan Subalgebras

623

CONJUGACY OF SPLIT CARTAN SUBALGEBRAS

Proposition 1

Let I be a finitely generated Lie algebra with center 5. Let t be a subalgebra of I, hoistable in I. Then (i) adji is finite dimensional and solvable, (ii) t is solvable. It is also finite dimensional z/ t n 5 is finite dimensional, (iii) if Í is an ideal o f some Lie algebra g then t is hoistable in g. Proof Let {x^,. . . , be a set of generators of I. For each 1 < j < m, let be an ad(t)-stable flag containing Xj. Consider the following se­ quence X of subspaces of I: m —\

m

■■■ j=i

j=i m —1

m —\

E

E

;=i

y=i

K ^P ^

••••

By removing redundant terms in X, we obtain an ad {(testable flag, also denoted by X, which contains x^ , . . . , x^. Thus adi(t)|;^^ c End(A") is finite dimensional and solvable. Since X generates I the map adjt ^ (adjt)l;^^ is faithful, and hence adit is solvable. Finally, t is solvable, since t / t n a - a d i(t). If t n 3 is finite dimensional, then clearly t is also finite dimensional. This proves parts (i) and (ii). Let i; G g \ I. Then [t, i;] is a finite-dimensional subspace of I (by part i). As above, we can see that [t, i;] lies inside an ad t-stable flag • d Fq 3 Vq is an ad t-stable flag of I. If we set = Kv ® V^, then Vn +\ ^ in g that contains v. □ Let M be a g-module. Recall that Af * has a g-module structure via X ' f ( v ) = —f { x • v)

for alt jc e g, / e M*, v ^ M.

We let T \ M ) and S \ M ) be the space of degree 2 elements of the tensor and symmetric algebras of M, respectively. These we view as g-modules

624

Coi\jugacy Theorems

(Section 1.6). The canonical surjection v : T ^ { M ) ^ 5^(M ) induces an injection of the dual spaces ^ T^{Mf via *^7(2) = / ( v ( z ) )

f o r a ll/G

z € r^ M ).

One verifies easily that the g-module structure of S \ M Y is that induced from T \ M ) * by restriction to v‘( S \ M) * ) . More precisely, if / g SHM)*, a: G g, and z g T \ M ) , then {x - f ) { v { z ) ) = {x ■ v ' / ) ( z ) . Let Q(M) be the space of quadratic forms on M. By definition F e Q(M) means that F : M K satisfies Q1 = a^F(u) for all i; e M for all Q2 the map B : M <S>M K defined by

e IK,

B{u, w) = j [ F{ v + w) - F{u) —F()v)}

for all v, w E: M,

is bilinear. Now B defined in this way is symmetric and hence defines a unique element B^ e S K M T by B^(uw) '= B( v , w)

for all v, w ^ M.

Conversely, each element B^ ^ S \ M ) * determines a symmetric bilinear form B and then a quadratic form F by F( v) = B ( v , v ) = This bijection of Q(M) and SKM)* determines, by transport of structure, a g-module structure on Q(M). Namely for y g M, (1)

x-F {v):=x-B ,iv^)=

- B^i xv ^)

= - 2 S * ( ( a: • v)v) =

+ x ■v f ) + B ^ ( v ^ ) -h

= —F{v + X ■v) + F( v ) + F ( x • v).

• u)^)

7.4

Conjugacy of Split Cartan Subalgebras

625

Define a g-module map M* ®M*

S^{M)*

by f® g^fg with fg(vw) ■■=

+ /(w ')^ (^ )}

for all

e Ai.

Evidently fg = gf. Let {y,}, ei be a basis of M, and let c M* be the corresponding set of dual elements. Then all i, j e I, v* vf satisfies U 1 vO

if i = ; = * = /, otherwise.

If we fix a total ordering < in I, we have S^(M)* = n iK u f y /. i< j

A typical element of S \ M Y may be thus written as a formal sum = Li<jbijU*uf, or more conveniently as a formal sum 5* = L ^ u v r ^ r , i j

where \bij ^ij Then satisfies

^ji

, i>ii

if i < j. if i = J-

defines a quadratic form F whose associated bilinear form B B(Vi,Vj) =B^(viVj) =a^j.

In the sequel we will write quadratic forms in the notation F = ' LaijVfvf, ‘J thus identifying F with its associated element in

In this notation the

626

Coi\|ugacy Theorems

g-module structure of Q(M) is given by (2)

x - Z a,jv* v * = Z a,X( x ■vr)v* + v H x ■v*)). 1<J

1<J

Lemma 2 Let cr, T e Endo^CM), and write = LbfkVj, j

JlbJkVj. Let V =

e M, Then in T \ M ) we have au ® TV = Y .F lp’''\v)V j ® Vp, j,P

where k,q

Proof. av <S)rV=i ' Zb^k^kv] ® ( E ^j,k ' ^P,q

= E (E

J,P^k,q

'

®V p .

On the other hand, we have Y. bf kb; , {vt , v){v*, v) k, q

^ ^jk^pq^k^q' k,q

Corollary In T^{M) one has for all f e M, v ® v = Zvfv^^{v){v^^v^). j,p

7.4

Coiúugacy of Split Caitan Subalgebras

627



Proof. Set O' = T = id in the last lemma.

Henceforth we assume that g is a finitely displayed invariant Kac-Moody algebra, that P is a weight lattice, and that M is an integrable g-module. Then S \ M ) is integrable, and by Proposition 6.1.16 we see that == Q(M) is a G-module satisfying g-F{v) =g-B^{v^) =

= F ( g - 'y )

f o r a l l g e G , f e Q ( M ) ,ü G M .

In terms of a fixed basis we have g • Y.ai jvf vf = i;a ,.y (g - v f ) { g - v f ) . Our next objective is to interpret the defining equations of the Kostant cone y = c L(A), A e in terms of quadratic forms. We maintain all the notation of Section 7.3 concerning y. The representation of g on L(A) is denoted by For each a e A_^ we write

and

J

We have, for v = ® y^J'^V = Y,Flp’' \ v) Vj ® Vp, J, P

where

k,q

Furthermore by the last corollary (A| A)i> ® Ü = ( Á \ Á ) ' Z v ^ v * ( v ) { v j ® Up).

628

Coi^jugacy Theorems

Hence by Proposition 7.3.2, the equations defining the Kostant cone become ((A I \ ) v*v * - E

(3)

i V

p

}’P ^

In short, the Kostant cone is defined by a set of quadratic equations. Let /r ( A ) = = { /^ Q ( M A ) ) l/( y ) = 0 f o r a lli) e r ( A ) } . Lemma 3 Let A e P T h e n (i) (ii)

= {y e L(A) I f(,v) = 0 for all f e is (^-stable.

Proof, (i) Since

contains all quadratic forms of type

it is clear that TiX) is the zero set of Iy(^xy (ii) The G-invariance of TiX) and the identification of 2(L(A)) with 5^(L(A))* imply by Proposition 7.2.7 that is g-invariant. □ Fix A ^ P+, and let t be a 7T;^-hoistable subalgebra of g. Consider the finite-dimensional t-module F = U(t)i;+, where is a highest weight vector of L(A). V affords a representation tt of t by restriction of to V. We have a natural homomorphism < p:G L (V)

^

G L {S \V )* )

=GL

of algebraic groups defined as follows. The map g e G LiV) extends uniquely to GL(5(F)) and by restriction to an element g* of GL(5^(K)). Now (p(g) is the inverse transpose of g*. Thus for g SKV)*, (4)


for all

e F.

Since ^ is a polynomial map we can consider its differential [Bor, Ch3]

7.4

Coivjugacy of Split Cartan Subalgebras

629

In what follows we fix once and for all a 7r(t)‘Stable flag F = F „ d K „_, d ••• :d I/o = (0) of V. Having done this, we define the corresponding Borel group By ■■= { g ^ G L { V ) \ g V k ^ V ^ , k = 0 , . . . , n ) and its Lie algebra hy-.= { X ^ q l { V ) \ X V ^ < z V ^ , k = 0, . . . , n } . Observe that by definition (5)

^(t)
By restriction we obtain a map of will denote by f >-*f. We set

to functions on F c L(A), which we

/== The elements of / are quadratic forms on V and can therefore be thought of as elements of S \V )* . There are two natural t-module structures on /. Since F is a t-module, the space Q (F) of quadratic forms on F admits a t-module structure whose action is given by (1). Let / e / c Q ( F ) , and let ;c e t. Since is g-invariant, it follows from (1) that ( 6)

X - f = x •f

and hence that / is a submodule of the t-module Q(F). On the other hand, t can be made to act on / c 5^(F)* via

(V)

X ■f = [d(pTr(x))f

for all a: e t .

Let us see that these two actions of t are the same. Let e S^(F)* be the linear map defining / , and let “ : T^(F) -» S^(F) be the canonical map (called v above). For all e F and g e GL(V) we have from (4)
®

® M'))-

Coi^ugacy Theorems

(>30

Thus for all X e t, d(p7r{x)B^{vw ) =

—7t ( jc) (g) id — id <8> 7t (

x

) ) ( i; ®

= - B ^ { tt{ x ) { v) w) - B^{ vtt{ x ){ w)).

In particular d
{g^GL( V) \
The Lie algebra of this closed subgroup of GL(V) is [Ch3, ch. 2, §14, Theorem 12]. 1 = {2fG gI(F)|rf
CIn

Proof, We know that 7r(t)
Lemma 5

There exists v e T{ \ ) n U(i)i;+ such that 7rfit)v c IKi;. Proof Let P ■= (L n By)Q (connected component of the identity of L n By). Then P is a connected solvable K-split algebraic group. We show that P acts on the set T ( \ ) n V. Indeed, if g ^ P and v e V(X) n F, then g • v

7.4

Coixiugacy of Split Cartan Subalgebras

631

since g G By. Now by Lemma 3(i), g • i; e T ( \ ) <=>f { g ’ u) = 0

for all / e

But f { g • v) = f ( g • u) = {(p{g) ~V) ( v) . Since g “ ^ G L we see that (p(g)~^f g /, and hence that ((p(gy ^ f ) ( v ) = 0» It follows that P acts (morphically) on the projective variety ^(A ) n K of lines of V(X) n V. Since projective varieties are complete, and v +^ ^(A) Pi V ^ 0, we may use the Borel fixed point theorem to conclude that there exists Kv Ei y { \ ) r \ V such that P • Kv = Ki; [Bor, Thm. 15.2]. The Lie algebra of P is [Ch3, ch. 2, §14, Thm. 11] P = I n b^.D7T;^(t). Thus '7T;^(t)z; c pz; c Ki;. Recall that b+=



0 g+ and b_=

n g_= o-(b^).

Proposition 6 [PK] Let t be a subalgebra o f an invariant finitely displayed Kac-Moody Lie algebra g. The following are equivalent: (0 t is a hoistable subalgebra o f g. GO t is TT^ and Trf-hoistable for all A ^ P+. Gii) Ad(g)(t) c b + Pi wb_ for some g 0 G and w

W.

Proof (i) => (ii) We know that t is finite dimensional and solvable (Proposi­ tion 1) and hence that t is and irf locally finite (Proposition 7.2.5). Let K be th^algebraic closure of K. We use “ to denote the corr^ponding objects over K obtained by extension of the base field from IK to K. Since ! c g is solvable, we apply Lie’s theorem (Exercise 1.22) to conclude that each V g L(A) ot L ( x y lies inside an ad f-stable flag. _ The following argument shows that the extension to IK is superfluous. We work with (the case of irf being analogous). We fix x g t, and let g= the decomposition of g into generalized eigenspaces for ad X (Proposition 7.1.23). Let v be an element of the generalized eigenspace L(A)^ for 1 0 7t/ x). It is clear that for a g g^. TT),(a)v e L (A ) CO+fX

Coivjugacy Theorems

632

and hence that E L ( ^ ) fJL+ÜÍ •

'^(11(9))^’


Since L(A) is irreducible, it follows that L(A) = £ L(A)^+<,. 0>GlK

Now given y e L(A), we can find a finite-dimensional 7T;^(t)-stable subspa^ Y so that y e y. If 17/x) has eigenvalues /i, + Wi,. . . , /t + o)„ on Y, < t ) j , e IK, then wju. + (wi + ■• • +
IKy+.

Indeed let

Z := { : e g_ I a

+

Since g““' n Z = (0) for all a¿ e n (since A e P++), we conclude that Z is (ad b_^)-invariant. It follows that ad(U(g_))Z c g_ is an ideal of g, and hence is (0) since g is radical free. Thus Z = (0). Now, if : e g satisfies 7r^(x)u^
2

2

2

Ad g (t) = A d(g+V i)t c b+, Ad g ( t) = Ad(«g_g2)t c A d (n )b _ c wb_. Thus Ad g (t) c b ^n wb_. (iii) =* (i) It will suffice to show that b^.n wb. is a hoistable subalgebra of g. Now b+n w b_c b ® Ece A+nwA_9“- Since A+n h'A_ c ^*A+ is finite (Pro­ position 5.2.3), we can write b+n wb_= b ® n, where n c ®„e^=A^.9“ finite dimensional and nilpotent. We show first that b + ti is ad-locally finite. Let n e be an arbitrary root vector. Let {ati, be a basis of n consisting of root vectors, say, Xi e g'»'- with y¡ e'®A+. Each ad a:, is locally

7.4

Conjugacy of Split Cartan Subalgebras

633

finite, and we have a sequence of finite-dimensional spaces Fo == K d c Ki := (ad U(K a:i ))F o c

■■= (adU(lKA:2))Fi c ••• c F„ := (adU(0<x„)F„_,). By the PBW theorem Vn =

U(n)Ko = U(n)U(^)Fo = U(^ + n)Ko

so is ad(l^ + n)-invariant. Finally, + n is finite dimensional and solv­ able, and the argument of (i) => (ii) shows that admtits an ad(l^ + n)-stable flag. □ Lemma 7 Let Q be a Kac-Moody Lie algebra. For w ^ +^

set © 9“* ae A+nvFA_

Then (0 (ii)

§,, = f| ® n,„, n,, = is its own normalizer in g.

and n,, = D§„,.

Proof, (i) It is clear that ^® and that c n^. The reverse inclusion follows from = g" for all a Finally, H^A_n (ii) Let n be the normalizer of in g. Then c n, and hence n = ®aeA^“ with n “ = n n g“ (Proposition 2.1.2). Clearly [f),n“] c and therefore n “ c Thus n c The reverse inclusion is obvious. □ Proposition 8 Let g be an invariant Kac-Moody Lie algebra, and l e t w ^ W . I f x ^ n ^ , then acts locally nilpotently in every integrable representation ( i t , F ) o f g, and there exists exp jc e G [independent o f ( tt, V)\ such that tt exp x = exp tt( jc).

X

Proof. Let {jCj,. . . , be a basis of consisting of root vectors x^ e g^% Pi The Xi act locally nilpotently on ( tt, V) (Proposition 6.1.3). Using PBW with the above basis, we see that every v ^ V lies inside a finite­ dimensional 7r(n^)-subspace of V and hence that 7r(n^) c End(F) is strictly triangularizable [Proposition 7.1.25 (ii)]. In particular exp7r(x) is a welldefined automorphism of F for all a: e n^.

Coiijugacy Theorems

634

Let M be the free monoid on the symbols X and Y. In the ring have

we

exp A^expy = exp(A^ + y + [AT,y] + • • • ) = exp/i(AT, y ) . Let be a nilpotent associative algebra of transformations of a finite­ dimensional vector space U. There exists a unique monoid morphism End(t/> satisfying

for any two given jc, y ^ N. Since any word of large enough length vanishes under ht )32 > • • • > ht We claim that if x = E flia,x, e n„, then (8)

expTr(x) = exp'7r(bjX,) exp ir ( 62^2) ■■■ ®xp Tr(hjvXyv),

where {¿j,. . . , bj^} c IK depends only on {a,,. . . , a/^} and n^, but not on ( t7, V). It will suffice to establish (8) on every finite-dimensional 7r(n^)-stable subspace U of V. Since ir(n^)lu is strictly triangularizable it generates a

7.4

Coiyugacy of Split Cartan Subalgebras

635

nilpotent (associative) subalgebra N of EndQJ). We use the above discussion and induction on r, where x = 0. If r = 1, then exp irix) = exp iriaiX^X as desired. Assume the result holds for r — 1 > 1 and that jc = jc' + a^x^, where x' •= # 0. Then on U, exp 7t( jc) = exp 7t( x ' + a^x^) = expir(ji' + f { x , a , x,))eTop'jr{a,x,). Now f i x , a,.xf) e 0 [r/K jr, because all roots involved in commutators of x and a^jc^ are of height greater than ht /3^. Thus exp 7r(jc' + / ( jc , a^x^)) has the desired form, and this completes the induction step. Let exp JC — exp(fciJCi) • • • exp(feyy^Xf,) e G. By (8) this element satisfies TTexp JC = exp 'Tr(jc) for all integrable representations ( tt, F ) of g.



Let I be a Lie algebra over K. A subalgebra i of I is called a Cartan subalgebra of I if CSl: f acts ad locally nilpotently on itself, CS2: f is its own normalizer in I. If in addition SCS: f is hoistable in I. We then say that f is a split Cartan subalgebra of 1. Example If g = (g + ,^ ,!2 + ? ^ )isa Lie algebra with triangular decomposi­ tion, then ij is a split Cartan subalgebra of g. Remark 1 Let f be a Cartan subalgebra of a Lie algebra I. If f if finite dimensional then f is nilpotent by CSl and Engel’s theorem. Most of the time we shall restrict ourselves to this case in what follows. The above definition comes from a general theory of Cartan subalgebras and their relations to regular elements. For more details see [BPl]. Remark 2 Cartan subalgebras need not exist for a given Lie algebra I. Theorem 9 (Chevalley, Peterson-Kac [PK]) Let g be a finitely displayed invariant Kac-Moody Lie algebra, and let G be its derived Lie group. Then Ad G acts transitively on the set o f split Cartan subalgebras of g.

636

Coiyugacy Theorems

Proof. Let f be a split Cartan subalgebra of g. By Proposition 6 we may assume that f c e n^. Thus f is a Cartan subalgebra of ^ in the classical sense, and by a classical conjugacy result (Exercise 7.6) there exists jc e such that expad x ( t ) = ij. Finally, by the last proposition we have exp ad jc = Ad g for some g ^ G. □ Proposition 10 Let I be a finitely generated ideal o f a finitely displayed invariant Kac-Moody algebra g. For a subalgebra a o f I the following are equivalent : (i) a is simultaneously diá-diagonalizable on I. (ii) There exists g ^ G such that Ad g(a) c n I. In either case a is abelian and finite dimensional. Proof (i) => (ii) If a d a c g l ( I ) consists of simultaneously diagonalizable transformations then it is clear that a is hoistable in I and hence also in g (Proposition 1). By Proposition 6 we may assume that a c for some w E:W. We now follow [Bo4]. Let c be the centralizer of a in and let f be a Cartan subalgebra of c. Since a lies inside the center 3 of c, we have a c 5 c f. Let n be the normalizer of f in and let b be an ad a-stable space so that n = Í + b. We have [a,b] c [ a , n ] n b c [ f , n ] n b c f n b = (0). It follows that b c c and hence that n is the normalizer of f in c. Thus ! = n so that f is a Cartan subalgebra of Up to conjugation we may assume that a (zi) and hence that a c n I. (ii) => (i) Clear. □ Corollary If a c Dg is ad-diagonalizable on Dg, then a can be conjugated by Ad(G) into i). Proposition 11 (Jordan-Chevalley decomposition) Let q be a finitely displayed invariant Kac-Moody algebra^ and let x ^ ^ be an ad-locally finite element. Then there exist unique elements x^ and m g such that (i) X=X5+X;^, (ii) [X5, x^] = 0, (iii) X5 {resp. Xff) acts semisimply (resp. locally nilpotently) on every integrable representation o f g.

7.4

Conjugacy of Split Cartan Subalgebras

637

Proof. Assume first that IK is algebraically closed. Since x is ad-locally finite, t := IKx is hoistable in g, and hence by Proposition 6, x can be conjugated into for some w ^ W. This allows us to assume at the outset that x e Let jc = JC5 + be the decomposition of x guaranteed by Proposition 7.2.6. Since [jc, c Proposition 7.2.6 shows that [x^, c and Write Xf^ = h -\c and hence by Lemma 7(h) that x^, x^^ n, where h n ^ n^. Then for any 7 e A and any a e we have (ad

a = (ad(/t + «)) a = {y,h)^a +

A: = 1 ,2 ,...,

where ¿ a: ^ ^ht5>htyS^- The local nilpotence of adxj^ then shows that <7, h) = 0 and, this being true for all 7 e A, that h lies in the center a of g. We write X = (x^ + /1) + n and observe that [(xs + h), n] = 0, n ^ acts locally nilpotently on every integrable representation (Pro­ position 8), JC5 + /z acts semisimply on every integrable representation (for this we let a ■= Kx^ + Kh and use Proposition 10). This proves the existence part of Proposition 11 when IK is algebraically closed. As for uniqueness, suppose that X=X^+Xjs¡ = x'^ + x',^ ''N are two decompositions of x satisfying the properties (i)-(iii). Then x'^ - x^ = Xn - x'j^. Also [x's, X5] = 0, since e g^ = g^^ p, c (see Proposi­ tion 7.2.6). Similarly [x^, = 0. Thus (jCy^ - x^) acts locally nilpotently, and x's - Xs acts semisimply on every integrable representation of g. This forces x's = Xs and x'^^ = x¡^. □ To prove the nonalgebraically closed case, we need the following: Lemma 12 Assume that {Ay}y ^ P+ span 1^*. For each i let be the kernel o f the action of g on L(Ay). Then X — fl = (0). {See Exercise l.A for the existence of {Ay}.)

638

Coqjugacy Theorems

Proof. Let r be the skeletal graph of the Cartan matrix ^ of g, and let be its connected components. These define submatrices of A and subroot systems consisting of those roots whose supports lie in j = 1 , r. Let be the subalgebra of g spanned by the root spaces g“, a e A^^\ and ij. Then by Proposition 4.3.9, g = Ey=ig^-'^ By Proposition 4.3.10, any ideal of g^-'^ is either inside i) or contains Dg^^\ In particular K n g^^^ (zi) oi K Dg^^\ The latter is impossible: If e A-' n II, then there must be an / e / for which
We now finish the proof of PropositionJ.1. Consider K arbitrary. Let IKbe an algebraic closure of IK, and let g — IK<8 rel="nofollow">|,^g, x •= 1 ® x. For each r e Gal(IK/[K) we have a IK-linear automorphism of g defined by (a (S>y Y = a'^ <8>y, and g = 1 <8> g is the set of points of g fixed by all these automor­ phisms. Let P+= {A G P |< A ,a /> ^ Z > q for all i e J} be as usual. For each A e ]^* we have the irreducible representation of g on L(A). It is clear that L(A):= IK0|,^L(A) is_the irreducible module of g under — 1_0 whose highest weight is A == 1 0 A e 1K0 1^* = ^*. Clearly r e Gal(IK/lK) defines a IK-linear isomorphism (as a vector space) of L(A) : a u a"’ 0 y. It is an elementary exercise to show that for y g g, D e L(A), (y • í;)^ = y'" • u'". Now consider x. By the above x = for some g g that satisfy parts (i)-(iii) of Proposition 11. In particular x^ acts diagonally, and Xyv acts locally nilpotently on L(A). If x^ • d = fiv, then x j • = (x^ • vY = /I'v"', and xj acts diagonally on L(A); similarly Xn acts locally nilpotently. Also [xj, xj^] = [x^, Xj^Y = 0. Thus x = x"* = xj -I- x^, and for each A g ^ /x ) = is a Jordan-Chevalley decomposition. But this is unique, and hence ^ / x ¡ ) = tt/ x ]^) = Since {A | A g P_^j span ]^*, we conclude from Lemma 12 that x j = x^, x]^ = Xj^ for all r g Gal(lK/[K) and hence that x^, Xj^ g g. .M is inteIf M is any integrable representation of g, then M •= grable for g, and so x^ and x^ act semisimply and locally nilpotently on M, as well as on M (see Proposition 7.1.16(i)). This concludes the existence part of the proposition. Uniqueness is as before. □

The decomposition of the locally finite element x g g in Proposition 11 is the Jordan-Chevalley decomposition of x. The following proposition is easy

Exercises

639

to prove (see also Proposition 7.2.6): Proposition 13 Let Q be a finitely displayed invariant Kac-Moody algebra^ and let x be an 2id-locally finite element o f g. Let x=x^-\ -Xj ^ be its Jordan-Cheualley decom­ position in g. Then (i)

for any subspace K o f any integrable ^-module M , x - K c z K ^ X s ' K c i K and Xj^ • K ;c = 1 0 X5 + 1 <8) is the Jordan-Chevalley decomposition o f 1 x in K EXERCISES 7.1 Let t be a Lie algebra over IK and ( tt, K) a representation of t. Let L be the set of functions from t into IK. For each A e L define = (y e K 1i; g V^^yix) for all x g t}, F ^ (t) = {y

G

K Iy

G

for all X G t}.

(a) Show that the sums and are direct. (Use Proposition 7.1.21). (b) Let ( tt^, FO, i = 1,2,3 be representations of t. Let B ® -> be a bilinear map satisfying TT^(x)B(vi, ^ 2^ = B(v^(xXvi),V2) + B(Vi,TT2(x)v2), for all X G t. Show that the induced linear map ^ :V^ 0 ^ is a t-module homomor­ phism. Use Proposition 7.1.22 to conclude that for all Aj, À2 e L. (c) Show that if a:, y g t are such that (ad 'n-(j:))''(ir(y)) = 0 for some n G N, then Tr(y) stabilizes V^ix) for all k ^ K. [Use (b) applied to End(F) ® V.] 7.2 Let t be a finite-dimensional solvable Lie algebra (Exercise 1.22). Let V (0) be a finite-dimensional t-module. Assume that for all x in t the eigenvalues of ir(x) in V all belong to K. In this Exercise we establish Lie’s theorem. The first step is to prove (by induction on dim t) that (*)

th ere exists A

g

t* such that F ' ' ( t )

¥= ( 0 ) .

640

Coiijugacy Theorems

(a) Let Í} be an ideal of t of codimension 1 (Exercise 1.22). By induction ^ (0) for some A e 1^*. Show that t stabilizes VKijX [Show that A[a:, y] = 0 for all x e t, y g )^. For this, fix VG \ {0}, and choose N maximal so that u, tt{x ) • V , . . . , Tr(x)^ • V are linearly independent. Let W¿ = 0 J “¿IK7r(jc)^(i;). Show that stabilizes and that, if z g 1^, then trp^^(7r(z)) = NX(z). Apply this to z = [x, y].] (b) Write t = ]^ © IKjc. Find an eigenvector of v i x ) on Extend A to t* and establish.(*) (c) (Lie’s theorem) Show that if IK is algebraically closed every irre­ ducible representation of t is one dimensional. Using a composi­ tion series, conclude that V admits a 7r(t)-stable flag. (d) Show that there exists a sequence of ideals 0 = t o C t i C ••• c = t such that dim t • = i for all 1 < i < n. (e) Show that for a finite-dimensional Lie algebra g to be solvable, it is necessary and sufficient that be nilpotent. 7.3 Let t be a finite-dimensional nilpotent Lie algebra and ( tt, F ) a finite-dimensional t-module. We maintain all the notation of Exercise 7.1. (a) For all A G L show that F /t) is a submodule of F. (b) Show that if 7t( jc) g End(F) is triangularizable for all jc g t, then F = © ;^^^F/t) (Proposition 7.1.23). ( c ) If F;^(t) # (0), show that A g t* and that moreover Alot = 0. [Assume that F = and show that A(x) = (dim V)~^ tiy 7t( jc).] (d) Let f :V ^ M be a suijective t-module homomorphism. Show that /( F /t) ) = M /t) for all A g L. 7.4 Let g be a finite-dimensional Lie algebra and t nilpotent subalgebra of g. View g as a t module via the adjoint representation. We maintain the notation of Exercises 7.1 and 7.3. (a) For all A, /x g L show that [g;^(t), g^(t)] c g;^+^(t). Conclude that go(t) is a subalgebra of g that stabilizes g /t) . (b) Show that A/g(go(t)) = go(t), that is, that go(t) is its own normalizer. 7.5 Let g be a finite-dimensional Lie algebra. A subalgebra t of g is called a Cartan subalgebra if CSl: t is nilpotent, CS2: A/g(t) = t (t is its own normalizer). We maintain all of the notation of Exercises 7.1, 7.3 and 7.4.

Exercises

641

(a) Let t be a nilpotent subalgebra of g. Show that the following are equivalent: (i) A/g(t) = t (and hence t is a Cartan subalgebra). (ii) [If ^ consider the t-module ^ind use Engel’s theorem.] Conclude that Cartan subalgebras are maximal nilpotent subalgebras. (b) Let f : g be a surjective Lie algebra homomorphism and t a Cartan subalgebra of g. Show that /( t ) is a Cartan subalgebra of f). [Use (a) and Exercise 7.3(d).] (c) Let 5 be the centre of g and t a subspace of g. Show that the following are equivalent: (i) t is a Cartan subalgebra of g. (ii) g e t and t/3 is a Cartan subalgebra of g/a. [For (i) => (ii) use (b). The converse is straightforward.] 7.6 Let g be a finite-dimensional solvable Lie algebra. Recall the ideal -^ (g ) (Exercise 1.23). The purpose of this exercise is to prove the following central result of classical Lie theory. Theorem (conjugacy of Cartan subalgebras: solvable case) If t and t' are two Cartan subalgebras o f g, then there exists x e ^ ( g ) such that t' = exp(ad x)t. We reason by induction on dim,,^ g. (a) Let n # (0) be a minimal abelian ideal of g. Let ~ : g g /n be the canonical map. Use Exercises 1.22 and 1.23 and the induction hypothesis to show that V = exp(ad jc)î for some x e T^~(g). Conclude that, without loss of generality, we may assume that Î = Î' and hence that t + n = t ' -h n : = i .

(b) Show that t and t' are Cartan subalgebras of Î and conclude that

we may assume, without loss of generality, that t + n = t' + n = g There are two cases: Case 1. [g, n] = (0), Case 2. [g,n] = n.

642

Coiijugacy Theorems

In Case 1 show that t = t'. [Use Exercise 7.5(c).] Assume therefore that [g,n] = n. (c) Show that n c (d) Show that n is an irreducible t-module under the adjoint action. Use this to reduce to the case when t n n = (0). (e) Assume henceforth that t © n = g = t ' 0 n . Given a e t, let ¿z' e n be the unique element satisfying a - a' e t'. Show that for a, h e t, [ a , b j = [a,b' ] - [b,a' ].

Conclude that there exists jc e n such that a' = [jc, a] for all a ^ t. [Make M — n 0 K into a t-module via a • (x, k) = (a • x — ka',0). Consider the canonical module homomorphism M ^ K, and use Exercise 7.3(d).] Show that exp(ad jc)t = t'. 7.7 Let g be a minimally realized invariant Kac-Moody algebra. In this exercise we provide a description for the group Aut(g) of automor­ phisms of g. (a) Let f be a supplement for in so that g = f 0 0 a\{0}9“ and g/D g = f. Show that each / e Hom^Cg/Dg, Zg) determines an automorphism = k'> for all i e J.] This leads to a subgroup D c Aut(g) consisting of auto­ morphisms that (i) permute the root vectors e,, i e J, and the root vectors /„ i e J, (ii) stabilize f|, and (iii) satisfy 0 ^ HomK(g/Dg)

D ^ A u t(r) ^ 0.

(d) Using the conjugacy theorems for Cartan subalgebras and for root bases show that every element r e Aut(g) can be expressed as a product ( - a - Y x • 5 • A d (g), where g ^ G, 8 ^ D, x ^ Hom((2, K®), e e (0,1} [Here a is the anti-involution that is part of the definition of (g, ^ } . ] In particu­ lar Aut G = < - o->Hom((2, IK®)£> Ad(G).

Exercises

643

7.8 In this exercise we establish a result of Kac and Peterson [KP2] on bounded subgroups (even bounded semigroups) of the group G associ­ ated with a complex Kac-Moody Lie algebra (g, ^ ) . The original results of this type (for a different class of groups) are due to F. Bruhat and J. Tits [Groupes reductifs sur un corp local, IHES, no. 41, 1972]. The proof of Kac and Peterson is unusual because of its use of techniques (due to Kempf) involving the theory of convex functions. In fact most of the results we need from this theory are easy to prove as they are included here as part of the exercises. One may consult A. W. Roberts and D. E. Varberg, Convex Functions (New York: Academic Press, 1973). Fix once and for all A = a Cartan matrix where J is finite, and (J) = /. Let R = (l^j^, II, II ^) be a minimal realization of A over U, Let C ^,C , 3£^,3£, be the fundamental chambers and Tits cones relative to 11^ and II in and respectively. Form the Kac-Moody algebra = g(^4, R) over IR, and let g = C <8>p5g be its complexification with diagonal subalgebra = C We are interested in the associated group G of g. Let be the full subcategory of (the integrable weight modules of g) whose objects are those integrable g-weight modules V satisfying V is U(g+)-locally finite [i.e., dim(U(g+) • u) < oo for every v P(V) c Int(3E).

VI

Let y be a set. A set ^ of subsets of y is a system of bounded subsets for y if M, M ' c ^ => M U M ' e M ' c M, M G ^

M' e

If y is a group, then the system ^ is compatible with the group law on y iff

(a) Prove that if (G, B, N, S) is Si Tits system with associated group W and we define ^ to be all subsets of G that lie in finitely many R-double cosets, then ^ is a system of bounded subsets. In the sequel this is the system that we will always have in mind. (b) Let [/ be a nonempty convex subset of W . A function f : U ^ U i s convex on U if for all x, y ^ U and for all t g [ 0 , 1 ] , fitx + ( l - t ) y ) < t f ( x ) + ( l - t ) f ( y ) . We say that / is strictly convex if the inequality is strict whenever X ¥=y and t G (0,1).

644

Coi\jugacy Theorems

(c) Show that jc is strictly convex on R and z \e^\ is convex on C. (d) Let t/ c IR'* be a nonempty convex set, and suppose that {/^} is a sequence of convex functions f ^ : U R such that L/^. converges pointwise to a function on U, Show that / is convex and / is strictly convex if at least one is strictly convex. (e) Let / be a convex function defined on an open convex set U c R", and suppose that / is differentiable at Xq e U. Let a g R" \ {0}, and let be the partial derivative in the direction a. Show that / ( ^ 0 + 5« )

-f(X o ) >s(dJ)(Xo)

for all 5 > 0 for which Xq sa ^ U and furthermore the inequal­ ity is strict if / is strictly convex. (f) Show that there exists a function /:Int(3E) ^ R^ satisfying / is H^-invariant, / is strictly convex. Set A^o = maxiCardCW^^) IK c J, K is a subset of finite type}. Fix a basis c Int(C ^) of Show that for all A e Int(3£) and for each k. ,-r(mi+ ••• +m/)

where r (which depends on A) is some positive constant. Show that / : A gives us the desired function.] In what follows, / refers to the function / that we have just constructed. (g) By extending the definition of / in the obvious way to a function / on Int(3£) 0 show that / is the restriction of a complex analytic function and that hence it is real analytic. (This requires some minor analysis about uniform convergence of convex functions.) (h) Show that for any IF-invariant subset D of Int(3£) that lies in the union of finitely many (2+-fans, ¡jl i Q ^ , / ( |( A + j/)) A e D , i/e D n C

converges.

645

Exercises

(i) For each subset T c ]^* let denote its convex hull. Show that if T is finite, then / assumes a minimum value on ( T ) at some unique point of . (j) Let D be a PF-invariant subset of Int(3E) lying in the union of finitely many <2+-fans. Show that for each M e there are, up to H^-equivalence, only finitely many finite subsets T oi D for which > M. (k) Let V e Obj(5^). For v = V, supp(i;) — {A I eP(K)^ 0} c Int(3£). For any nonzero finite-dimensional vector subspace U of K, define supp(i/) := U supp(i;) c Int(3£). v^U Show that supp(i/) is finite thus enabling us to define r = 7 t/:G

Int(3E),

y ( g ) = M<supp(g • i/)>,

where • is the integrated action to G of g on F. Let B, G+, N, H, be the standard subgroups of G (Section 6.2). Prove that for all n e N and w = nH e W, y(ng) = wy ( g) (1)

for all g e G.

Let U # (0) be a finite-dimensional subspace of K e OhjiS^), and let y = yu be defined as in (k). Let g ^ G, and suppose that y(g) e C. Show that for all a e f)g such that y(g) + a e. <supp(g • i/)> we have (d^fXyig)) > 0. Use the IL-invariance of / to show that for all I e J we have /(y (g )) > 0. Given b e B, conclude that any element A of <supp{bg • U)) can be written as ^

where a e

=y(g)

+a +P

is such that y(g) -f- a

<supp(g • t/)> and /3 e

(m) Prove that for g e G with y(g) C and b ^ B, /(y(bg)) > fiyigJ). (n) Let U # (0) be a finite-dimensional vector subspace of F e O b j(^ ). Show that there exists a finite subset {A,} c C so that m ( g ) - G ) c uA,ie^. (o) Let y = yj; be as in (k). Prove that the function g /(y (g )) on G assumes a maximum at some point gg e G for which yCgg) e C

646

Coi\jugacy Theorems

(p) Let V, U, y, gQ, be as in (o): Show that for g ^ G, y{g)

= y(go)

^g^PKgo^

where K = {/ e J 1(ji g^X « /> = 0} and is the parabolic sub­ group BWj^B of G. (Consider the element ggo^, and use the Bruhat decomposition.) (q) (Kac-Peterson) Let M be a subsemigroup of G. Prove the follow­ ing are equivalent: Bl: M is contained in a parabolic subgroup where K c J is of finite type. (Parabolic subgroups of this type are some­ times called Iwahori subgroups.) B2: M is bounded. B3: M acts locally finitely on every V e Obj(5^). B4: M leaves invariant a nonzero finite-dimensional subspace of some V e Obj(<9^).

A*l*-An Extended Example APPENDIX TO CHAPTER 1 Let K[t,t~^] denote the ring of Laurent polynomials with coefficients in K: K[t , t

— I X) I

^

^

j = tn

where addition and multiplication are defined in the usual way { L a j t ’) + {j:bjt^) = E i a j + bj )t \ + {T,bjt^) = e ( e « A -;)^ * k ^ j



Let L§l2(IK) = §I2(1K[L i ” M), the set of 2 X 2 matrices with coefficients in K[t,t~^] and trace 0. This is a Lie algebra, called the loop algebra of ^I2(IK), under the usual bracket and contains ^l2(IK) as the subalgebra of matrices all of whose entries are constant polynomials. We can think of g as an algebra over the ring K[i, i “ ^], in which case it is of rank 3 as a module. However, over K it is infinite dimensional and reveals an entirely different structure. Consider the standard basis of ^l2(K):

‘ =(2

i).

A

/=(;

II

Then the matrices t^e = Z, form a basis for L^l2(IK) over K. An alternate description of L^l2(lK) is as lK[i, 0ij^^l2(W, the isomorphism being obvious: t^x ® x for all X

G ^ l2 (tK ).

647

648

Extended Example

There are infinitely many integer gradings that can be placed on L§l2(IK) (a fact that becomes obvious later on). For now, however, we settle on one, called the principal grading, by defining deg r*e = 2k + \, d e g r* /= 2k - 1, deg t'^h = 2k.

A: e Z.

The grading is schematically shown below. Notice that dim or 2 according to whether k is even or odd.

= 1

degree 3 2 1 0 -1

t

-2 -3

t-^h

e h f

te th tf

Treating L§l2(IK) as a module for §I2(IK) (under the adjoint action) we can see from this schematic picture how decomposes into a direct sum of infinitely many §l2(IK)-submodules each isomorphic to itself (as an §l2(K)-module). Let K be the Killing form on §I2(IK). (See Example 1.20). Define a bilinear form ( I •) on L§l2(IK) by setting (A.1) (i*ali'b) =

QK{a,b)

for all A:, / e Z , a , b e [ e , h , f )

(5 = Kronecker delta). The invariance of this form is an immediate conse­ quence of invariance of the Killing form [but (-| • ) is not the Killing form of §l2(IK[r, r " '])]• Evidently Lêl2(IK)* J. L il2 (IK )' if A: -Il Q. On the other hand, L§l2(IK)* and L§l2(IK)“* are nondegenerately paired, namely x e L§l2(IK)** and (x|L§l2(IK)^*) = 0 => x = 0. It follows that (-| • ) is nondegenerate, symmetric, and invariant. Since §I2(1K) is perfect (i.e., is equal to its own derived algebra) so is L§l2(K). Thus by the theory of Section 1.9, Lil2(K) has a universal covering

Appendix to Chapter 1

649

algebra. In fact we can explicitly construct a covering algebra, and later we will show that this algebra is the universal cover. We let §I2 (K) :=

(A.2)

e IKC

be a one-dimensional vector space extension of § l2(IK[i, t ']) and define multiplication on it by bilinear extension of 1 [ra ,t'Z )] = t'‘*‘[a,b] + k8^+, Q-K{a,b)
(A.3)

[t*a,e] = [e,r*a] = [«:,c] = 0

for all

k ,l ^ Z,a,b ^ {e,h ,f).

The bilinear mapping e; L§l2(IK) XL§Í2(IK) defined by

(A.4)

e { r a , t ‘b) = k8k+i^Q-K{a,b)

is a 2-cocycle in the sense of Ch 3.8(3), and hence § I2(IK) with [•, • ] is a Lie algebra and a eentral extension of L § l2(IK). Since [th,t~^h] = \K{h,h)
if yfc e 2Z \{0 }, (IK/i -I- IKc

if A: e Z \ 2Z, if A: = 0.

^^0

Extended Example

a p p e n d ix t o c h a p t e r

2

Using the principal grading set

^>0 k<0 5 := Kh + K0,SO

^i2(K) = §i2(iK)_0 § e We consider this as a potential triangular decomposition of ^ l2(IK). Define an anti-involution a on §I2(IK) as follows: §I2((K) has a natural anti-involution, transposition of matrices. Extend it to an anti-involution a of L § l2(IK) by t^a t~^cr(aXk G Z, Observe that this is not transposition on § l2(lK[i, Lift a to §I2(IK) by setting cr(c) = C. Then or([i*a, t'b]) = o-(r*+'[afe] + k8^+, o\K(a,b)c) = t~^‘‘'^‘\
8

Q^K^ab, (To)(t

= [a-(i'i)),
= 0, i 2i*a = < 0

according as

Thus, defining a ; : 5 ^ IK by « j : e 0 and ^ decomposes into three eigenspaces relative to

I e, a = I h, \f2, we see that § I2(IK)^.

§I2(K)+ = g l2 (K )7 ' ® §l2(»<)+ ® ^i2(i<) +

Appendix to Chapter 2

651

and §i2(»<)+=

fc> 0

The problem is that ad § does not create enough different eigenstates. We remedy this by enlarging We let d: gljilK) ^ § l2(IK) be the linear map defined by d\.— = scalar ^I2(IK) multiplication by k. Since d e Der(§l2(IK)) we can form the Lie algebra §I2(IK) = Kd © i l 2(IK) using the construction of Section 1.5: [d,d] = 0 [d, x] = d ( x )

for all x e §I2(IK),

in which § I2(IK) appears as an ideal of codimension 1. Set (A.4)

S==IK d® §,

and extend
§ Q k )_ ,


where we define § I2(IK)^= § l2v-v+Define «o>

^ ft* by ao(d) = 1,

a^iit) = 0,

ao(^) = “ 2, " i(^ ) = 2,

and let 8

=

Q!g -|- C f].

Then = {2k -h l)t*e] [e,i*e] = 0 [/i, i*e] =

—— —— — Qri+Ac5 ——o;n+(^+ 1)5 c §I 2(IK) = §I 2(IK)

652

Extended Example

Similarly t'^f ^

= gÍ2(IK)“'>'"^*“ *^, i*/j e §I2(IK)**. Thus

(A.7) kd -a^+kd © §l2(K )''"e © §I2(K)

§Í2(í<) += © §Í2(K) ^>0

A:>0

k>0

and all of these root spaces are one dimensional. With (^•8)

Q +'= {^«0 + ma^\k, m > 0} \ {0},

we have §Í2([K)_,=

© §Í2(IK) «^í2+

(note that §Í2(D<)^ao+mai = (0) unless \k — m\ < 1). Together (A.5), (A.6), (A.7), (A.8) show that § 12( 11^) has a regular triangu­ lar decomposition. The Lie algebra ^ Í2(IK) is called the affine Lie algebra of type The root lattice is g = Za^ + Zctj, and the set A of roots is given as (A.9)

A = [ka^ + ma^\k,m e Z,|fe — m\ < l}.

^ : = (§I2(K)

Q+, (t ) is a regular triangular decomposition. We set n := [ao,a{\

and n -= = { a o ^ < } . We introduce further notation that will be convenient later on. Set Cj := e, « 1^:= h, / j ■=f , and define i Í 2(IKy^^ = Ke^ + Kai'^+ K/j. Define (A.10)

eo '=tf,

ao - = t - h ,

f o - = t ^e,

(0)

:= K cq + IK«(^+ IK/q = §I2(IK), for example and observe that [^o»/ol = W> t~^e] = - h + jKif, eH =
e§l2(0<)

d-, h ^ % ,

i = 0 ,l-

Let us see that the subalgebra <eo, gj) generated by Cq and

is precisely

653

Appendix to Chapter 2

Evidently

c

However,

(ad Cj ad eo)*ad Cj(eo) = [i*^, e j = 2i*e, [i*;i,eo] = -2i*=^*/,

A :>0,

from which the reverse inclusion follows. Similarly § l 2W

- =

-

Thus ^ I

2( I K )

=

< /o ,/i>

e

i| 0

< eo,C i> .

Next we consider as a module for (defined above) under the adjoint representation. This action is integrable (see Section 2.4). In fact (ad c) annihilates d,0,t^e (ad e)^ annihilates t^h (ad e)^ annihilates t ^ f for all k e Z, so (ad eY = 0. In the same way (ad f Y = 0. Thus by Proposi­ tion 2.4.4, § 12( 11^) is completely reducible into irreducible modules for §I2(IK)^^\ Two of these are the one-dimensional modules and Wd — The others are the three-dimensional submodules that we already saw in Lél2ÍKX The situation here is somewhat unusual because ad e and ad / are actually nilpotent, not simply locally nilpotent. This reflects itself in the bounded dimensions of the irreducible ^ 12-modules that we just obtained. More typical of integrable representations is the discussion below of the basic representation of §Í2( 0^) ¡n which e and / no longer act as nilpotent operators. For the same reasons as above, (ad e^Y = 0 = (ad / qY, s o the representa­ tion of on §12( 1^ ) determined by the adjoint representation is integrable and hence completely reducible. Using the above description of the roots ^l2(K) = © (§I2(K) k^Z ^

—cíQ +

kS

~kS

0 ^I2(1K)

0 ^12'

aQ+kd

)■

654

Extended Example

For ^ 0 we are looking at irreducible § l2(IKy®^-submodules each isomor­ phic to the adjoint representation. For A: = 0, - - ocq §Í2(IK) 0 §I2(1K) + §Í2 =

lK ( d

-I----- 0

IK c 0

^ I2 (1K )

which consists of two trivial representations and the adjoint representation again. The two ways that we have just described for decomposing § 12(11^) into ^ l2(IK) submodules is made schematically evident by looking at the root system A.

-Uq — 25

-a 0 ^ -2 5

- “0 -8 — —8

«1 0 -« 1

+ 5 8

28 Uq + 8

an + 25

«0

The vertical (resp. horizontal) sections correspond to ^I2(1K)^^^ [resp. §I2(IK)^®^] submodules. Since each root has several descriptions (« q? ^ linearly dependent) the naming of the roots as shown here is best understood by starting at 0 (corresponding to §) and successively applying operators ad Cq and ad Cl to move right up and ad / q and ad / j and to move left and down). Let us return to our integrable representation of §I2(IK)^^^ on §Í2(1K). According to Proposition 2.4.4, there is a compatible action Ad [in the sense of condition Ch 2.4(8)] of SL2(K) on ^I2(1K)‘ for all nilpotent X e ^ Í 2(KY^\ exp ad¡^)A^ = Ad(exp X ) . Since ad^----- X is a nilpotent derivation, Ad(exp AT) is an elementary autoéÍ2(IK) morphism (Proposition 1.5.3) of ^I2(1K). Since SL2QÍ) is generated by {exp X \ X nilpotent} (see Proposition 2.4.8), we see that we have a subgroup 5L2(IK)^^^ - PSL2ÍK) in Autg(él2(lK)) determined by g l2(IKy^\ In the same (0) Together these way we obtain SL2(KY^^ c A u t/^ l2(IK)) from ^ I2(IK) generate most of A ut(^l2(IK)) (see below). Remark 1 Since § l2(ll^) decomposes into a sum of only odd dimensional irreducible modules for §Í2(IK)^^^ under the adjoint representation, the corresponding group SL2(KY^^ of autmorphisms is isomorphic to PSL2ÍK).

Appendix to Chapter 2

655

Let us turn to the internal ideal structure of §I2(IK). Taking account of Propositions 2.7.5 and 2.7.2, we have rad(§l2(lK)) = for any triangular decomposition T of ^I2(1K) (in particular for the one we have constructed) and n(§l2(IK)) n $ = Z(§I; These become fairly trivial-looking statements in this case, since we can prove that Z{§Í2(K)) = Ki, the ideal lattice of §Í2( ^ ) is

__ §I2(1K) I __

§ I2 (K ) = d (§Í2(IK))

{0}. Indeed let a be a nonzero ideal of ^ I2(IK). Then a is an l^-module and hence decomposes into root spaces: a = a “ ^ (0) for some a # 0, then t^e, or t ^ f is in a for some k. Then one easily finds that a D §I2(IK). If a" = 0 for all a # 0, then a c $ and from [t^e, a] = 0 = [t^f, a] V/& obtain a c Kc. Thus ^7^= (0), r a d ( i r ; w ) = (0), n(§l2(lK)) = K0. The ideals of are precisely all the subspaces of the form a • §I2(IK), where a is some ideal of IK[i, i “ ^]. In fact the correspondence a a • §I2(1K) is an isomorphism of the lattice of ideals of K[t, t ~^] and L^I2(1K). Every nonzero ideal of has a unique preimage in §I2(1K), and this accounts for all ideals of ^12(11^) except (0) and K0. However, with the exception of ^ l2(IK), Kc, and (0), none of these other ideals is
656

/ lí‘*-An Extended Example

We can clarify this by an example. Consider the ideal of lK[i, The corresponding ideal of L § i 2(K) is (t - l>Lgf^([K) = (fUXt - l)x |/(i) e IK[i, r“ *], Ai e g l2(lK)}. The preimage of this in §I2(IK) is an ideal of that contains c. As a vector space it is KC + L§I2(1K). However, this is not ¿-invariant; If x e § I2(IK)“ \ {0} then ct e §I {0} and > 2

\ \

d{t - l) x = (« (¿ ) -I- 2)x - a { d ) x = 2x ^ (t - 1>L§I2(IK). In fact the smallest ideal of §I2(IK) containing x is S T J k ).

A PPE N D IX TO CH APTER 4

Our triangular decomposition (§ l2(IK)+,h,Q+,or) satisfies CT1-CT3, and hence §I2(1K) is contragredient. Since ade, and a d /,, i = 0 ,1, are nilpotent, and a fortiori locally nilpotent, §Í2(IK) is integrable; in other words, it is a Kac-Moody algebra. The Cartan matrix A is determined from 'afh) = 2 aj(C - /i) = - 2 a^{h) = - 2 -h) =2

if i = j = 1, ifi = 1 ,; = 0, •fi = 0 ,; = 1, i f i = 0 ,/ = 0.

Thus

2

A =

(A.11)

-2

-2 2

with Coxeter-Dynkin diagram O O of type The Lie algebra § I2(IK) is often referred to as A^i\ The Weyl group is given by W = ( tq, Tj ). Direct computation using the structure matrix gives rQ-.ao^ - a o , rj : «0

a , -> 2ao + ttj = «Q-I-8, “i +

“i

-« 1

(here, as before, 5 == « q -I- « 1). Then r, 5 = 8 ,

''o'*!: «0

“ 0 + 25,

i = 0,l,

«1

a - 25,

Appendix to Chapter 4

657

Thus IV has infinite order and has = (Z, + ) as a subgroup of index two. A presentation for W is <''o.''ll''o =

= 1>-

This is in accordance with Theorem 5.3.1. W = [I, ro,

rj,

r^r^, r j r o ,

roz-irg,. . . } .

The roots are, as we have already seen, (A .12)

= W{aQ, a^} = [ka^ + m a j \k — m\ = 1} = Z5.

The triple i? := {§, II, II is a realization of A (the natural realization). One notes that it conforms exactly with Example 1 of Section 4.2. From Proposition 4.2.4,

u(^, /?) = u_e ij ©u+, where is freely generated by two generators eg, and u_ is freely generated by two generators, /g, /i- According to Proposition 4.2.10 there are surjective homomorphisms
ii^i,

d r - ( a d / ,) V y ,

i* i,

and q(A, R) = u(A, f?)/rad u(A, R)). But we have already seen that rad(§l2(IK)) = (0), and hence (see Proposition 4.2.8) §l2(K) = 9 ( ^ ,i? ) .
658

Extended Example

i = 0,1, and the relations (A .14)

[A o,A i ] = 0,

[¿ ,A ,] = 0,

[A„e,] [hi, fj\ = - A j i f i

/ = 0,1

[d,ej\= ej / , / = 0,1,

[d,fj\ = - f j

[^<>/;] ~ ^ij^i (ad e^fcj = 0 = (ad f i f Cj,

i Фj

(see Section 4.2, Remark 2), and furthermore D ( i l ^ ) = [§I^0<),§I^(IK)] = D iTI(i<j“ + IKAo + IKAi is defined by the generators h^, e^, f-, / = 0,1 and the same relations (A.14) less those involving the generator d (Proposition 4.3.4). One would suspect that in the relatively simple case here there would be an elementary way to see that g^(^, R) = д(Л, R) without recourse to the Gabber-Kac theorem. It is a worthwhile exercise to look at this and convince oneself of how difficult it is. According to Proposition 4.1.14, 9^(Л, R) and ^ I2(IK) = д(Л, R) have the same root systems and in both cases the real root spaces are one dimensional. It follows that ker

9^(A,/?)*«.ThuS [e„rad(g4A,/?))] c r a d ( g 4 ^ , / ? ) ) n

E

= (0),

fcsZ\{0}

and similarly [/¿,rad(g'^(yl,/?))] = (0). It follows that rad(g^(^, Л) central­ izes D(g^(^, Ю) (which is generated by e„ /), / = 0,1), and hence D ( g t( ^ ,/? ) ) - ! ^ ii^ ^ 0 is a central extension. In fact one can show that §I2(IK) is centrally closed [Ks], so this sequence splits. It follows at once that Dg^(^, i?) = ^ §I2(1K). The Cartan matrix (A.11), ~ | 2 2 ) ’ ** symmetric and hence symmetrized by ( sq, Cj) = (1,1). The map of Ch 4.4.(8) is then (A.15) In particular 5° =

Х Л.1 a-

,

/ = 0,1.

= <г. According to the prescription of Ch 4.4, we

Appendix to Chapter 5

659

define a symmetric bilinear form (*| • ) on ^ by using the matrix (A.16) relative to the basis a / , d). Here * = (d\d) is arbitrary. This extends uniquely to all of i Í 2(IK)= g ( /l ,/?) by the use of Ch 4.4(10a), (10b), and (10c) [t"e, r " f ] = ( i'’e |i - 7 ) ( a , + n S f = ( t " e \ r ' ’f ) { a ¡ ' + n in Section 4.7 gives us = (í"e|í7-í"e) = -(e\f) = h (r hU^ h) = ( t^ h lr ^ h ) = (h\h) = 2, from which < • | • > is clearly positive definite if K is a totally ordered field. This is deceptively simple. In general Kac-Moody algebras root spaces are not one dimensional, and there is no easy way, here, to make the computa­ tion of < • I • >. APPENDIX TO CHAPTER 5 We have $ = lKao''+

Kd,

where (a¡, d) = 1, i = 0,1, and ]^* = K ckq + [Ko!^ + H.d*. We define (d*,an= S,^o, ( d * ,d ) = *

arbitrary in IK.

^i^^-An Extended Example

The matrix of ( • , • ) on $ x 1^ relative to these bases is 2 -2 1

-2 2 0

11 0 *J

[compare with (A.16)] and »

where n - { a o ,a ,} , is a set of root data. The reflections /*q,

n ''= = { a o " ,< }

defined above extend to

by

rod* =d* - ( d * , a ^ ) a o = d* - a o , rid* = d* - { d * , a ^ ) a i = d*. The group that they generate restricts faithfully to + Z aj according to Corollary 2 to Proposition 5.2.3. But this is in any case obvious from the presentation of W given above. Likewise we define reflections r^ , r / on $ by = h - (ai,h}ay,

i = 0,1.

These generate a group with presentation ( r ^ , r^^lr^'^ = = D . which is isomorphic to W (Lemma 5.1.2). The Bruhat ordering on W is, by Proposi­ tion 5.4.2,

(A.17)

ro^iro

'• i v l

rcJ O'l

r^r, I'O

The Tits cone and fundamental chamber in 5.3 and 5.4.

are illustrated in Figures

661

Appendix to Chapter 6

For w ^ IV, 5^ := {a e A + k “ ’a e A_} and (SJ^=

L «

(Section 5.2).

With p := 2d* - jao, we see that p is a minimal regular in weight: = 1,

/ = 0,1.

Note that for all /: e [K, p + A:5 is also a minimal regular in weight. We have (Proposition 5.2.5) <5^> = p - w p . It is easy to see by induction on k that (A.18)

(''o''i) P ^ P ^ 2ka^ — k{2k + 1)5,

r^ijQ r^) p = p — {2k + l)ai — k{2k + 1)5

for all k

Thus = - l k a , + k { 2 k + \ )8, (A.19)

= (2* + 1)«! + k(2k + 1)5, , , i m ( m — 1) {<5,,>k e IF} = m a, + ---- -8\m g Z

Notice that (A.19) establishes a 1-1 correspondence between W and Z under which l(w) s m (mod 2). For further reference we also note (A.20)

(ro/'j)"d* = d* + noiy — n^8

for all

n

APPENDIX TO CHAPTER 6 We define a restricted weight system P ■= Zd* + Z (aj/2 ) + Z5 with set of fundamental weights il = {wg, w j, where Wq = d* and o)^ = d* +

<562

Extended Example

We next examine what the denominator formula of Corollary 1 to Theorem 6.4.1 has to tell us in the case of §I2(IK). Using (A. 18), the fact that dim §l2(IK) = 1 for all a e A^., and the explicit description of A^. as seen in (A.9), we can write the denominator formula as E

c(p + Ika^ - k{2k + 1)5)

k = —OO

~

H ^(p — (2A: + I)«! —k(2k + 1)6) k = -00 00

= e (p )n (l-e (-a o -A :5 )) k= 0

X(1 - e ( - « j - it5))(l - e { - { k + 1)5)). We cancel off e(p) from both sides, and set x = e(-a^), q = ei —8) [so e (-a o ) = obtaining E k^Z

j.-2k^k{2k-^\)

=

^ ^(2k +D^k(2k +\) k^Z ‘9*-"‘) ( l- x ( ? * ) ( l - «*■"')

k= 0

or, finally, combining the two sums, (A.21)

E (-l)"xV^"- D /2

k =0

This is a nontrivial fact called the Jacobi triple product identity. One may consult [HW, An] for applications of this to number theory. Let us remark on two of its specializations: replacing q by and x by q,

E (-i)V3"-'^/^= ñ íi- í" ) , which is Euler’s pentagonal number theorem. Since n ” =i(l —^") expands as ~ where p^ {k) [resp. p^ik)] is the number of distinct partitions of k into an even number (resp. an odd number) of parts, we obtain p^{ k) = Po(k), except when A: is a pentagonal number, namely of the form ^nOn - 1) (See [HW] for an explanation of the terminology). The right-hand side is usually denoted by (p(q):

n= i

663

Appendix to Chapter 6

It has already appeared in Section 2.5, Example 3. Euler used his pentagonal number theorem to compute the partition function. Since l.y ( ,) - V ( 9 ) -

ip (k ),4 ^=0

z meZ

we obtain, by looking at the coefficient of 0=

E

(-ir« " » » — « ) , /

n > 0,

(-irP (A :),

where I(n) •= {(A:, m)\k + |m(3m — 1) = n}. Thus (A.22)

E

- iw (3m - 1)) = So „

meZ

[p(j) == 0 if j < 0], which gives a very effective recursive determination of pin). If we replace q h y and x by q, then the Jacobi triple product identity gives the Gauss identity

E (-i)V = «eZ

n ( "=1

< pW

1

( 1 - «^")



Next we consider in detail the integrable highest weight module L(fi*) of §I2([K) with highest weight d*. According to Theorem 6.4.2 there is, up to isomorphism, only one such module (hence the use of the word “the” above), and it is irreducible. The weight system P{L{d^)) lies in the set d* - (Na^ + Na^X Let II G P(L(6i*)). We claim that also ¡jl - 8 ^ P(L(d*X). Since W8 = 8 and WjjL n P^¥^ 0 (see Proposition 6.1.11), it is enough to prove the claim for jji ^ P ^ n P(L(d*)X By Proposition 6.2.5(i), ¡x is connected through d*. This means that if we write jx = d* - a ^ d* i Q+, then either fx = d* or (d*, a / > # 0 for some i e supp(a). In our case this means that jx = d* or «0 ^ supp(a). In any case i e supp(a) => i e supp(a + 8 \ and since /X —5 e P^r\(d* i Q^X we may use Proposition 6.2.5(ii) to conclude that fx — 8 ^ P(L(d*X), (This argument works quite generally for affine Lie algebras.) If /X e and we write ¡x = d* - maQ — na^, m, n e N, then from (fx, a ^ } = 1 —2m

2n ^ N,

( f x , a ^ ) = 2m — 2n ^ N,

664

Extended Example

we obtain 0 < 2(m — n) < \ from which m = n. Thus ¡jl = d* - m8. Putting this together with the remark above, we see that P (L (d * )) = Wd* - N5. Since r^d* = d* and W = (A.23)

P(L{d*))

=

[d* +

u (ro ri)ri, we obtain from (A.20) na^

-

{ n^

+

k)8\n

e Z, A: G N) .

This is illustrated in Figure A.1 (see [FL]). The dotted curves represent PT-orbits. Multiplicities are constant on orbits. It is a consequence of Proposi­ tion 6.2.8 that the multiplicities increase (not necessarily strictly) as we pass

Figure A.1. The weight system of L ( d * ) for §I2(1K). If IK = [R the shaded region represents that part of d * + IKao + IKaj that lies inside the fundamental chamber F. The dotted curves represent PT-orbits.

665

Appendix to Chapter 6

to successively lower orbits. In fact we will soon describe the multiplicities exactly. From our description (A.23) of the weight system of L(d*), we have ch(L (d*)) = E E j^Z k^ N

- kd)

Since the weight multiplicities of L(d*) are IF-invariant, the inner sum can be written as b f, ■■=

E d im L (d * )‘'’ ~**e(-A:S) k^N

and (A.24)

ch L ( d * ) = b r . - L e { ( r o r , y d * ) .

The expression b^* is called a string function or branching function. (Of course, as it stands, it is not a function at all. However, see below.) The notation b^* anticipates the more general notation of branching functions. Write bj* = E p ( k ) e ( - k d ) = E k=0

k=0

where q •= e ( - 8 ) as usual. We plan to prove that p(k) really is the partition function. For this purpose we apply the Weyl-Kac character formula (Theo­ rem 6.4.1). Here we use (A.24) and replace the denominator in Theorem 6.4.1 by the skew-invariant sum of the denominator formula (corollary to Theorem 6.4.1). (A.25) ^\k=0 =

l ^ j^ Z

'

E ( - l ) ''" 'e ( w ( d * + p ) ) .

Now observe that on the right-hand side the only term of the form e{d* +

666

Extended Example

p - nS), fi >0, occurring is e(d* + p), since d* + p - nd ^ P^, but by Proposition 6.1.11, W(d* + p) n P^= {d* + p}. Let us compute the coeffi­ cients of all the terms e(d* + p — nS) on the left-hand side, namely (A.26)

£

L

( - l ) « “'V(A:))c(d*-t-p-nS), /

n = 0 \ (w, kJ)^B(n)

where Bin) ■■=[iw,k,j)\wp ~ k8 + ir^r^Vd* = d* + p - nS}. Using (A. 19) and (A.20), we see that wp - k 8 + (rotiYd* =d* + p - n8 <=> —mai —

m (m — 1)

8 - k8 + ja^ —j^8 = —n8

[where w ^ m in (A.19), and we have used p — wp =

(A.27)

(m - j = 0, - m ( m — 1)

- k

= -n,

f m - y = 0, <=> ( m I k + — {3m — 1) = «. Since each m e Z and n we have from (A.26),

I determines a unique

A: e N satisfying (A.27),

(A.28) — \m{3m — l))e(
. -1 bf.=cpiqy

Thus we have the remarkable fact that (A.30)

dim L ( d * ) ‘‘

= p(k).

667

Appendix to Chapter 6

We can now rewrite the character formula (A.24) as

ch neZ

1

Y, e{d* + na^ - n^8)
E x-^q"" n

where x == e( —a^). Specializing x to 1, we obtain

^(^*) -^(^*)I

©((?)

specialized with e(-ai)= 1

where ©(^) — = 1 H- 2^ + 2q^ + • • • . This is the theta function of the lattice Z. All of these things have suitable generalizations, which have been the subject of considerable investigation (see [KPl] for more on this). Suffice it to say we have arrived at the point where modular forms enter into the theory. The transition into functions is made hy q where r ranges over the upper half plane in C (i.e., {z e C|Im z > 0}, and the modularity refers to the transformation properties of these functions ia h \ ar-h b under the action of SLSX) on defined by j\ = ------- 7\c a } CT d The way in which the weight system of L(rf*) decomposes into strings - k8, k = 0,1,2,... seems to suggest that L(d*) itself decom­ poses with respect to some suitable representation of a Lie algebra. This is in fact the case. To see how this comes about we assume that K = C. Consider the Lie algebra

a = Cc + E ^I2(C)

We have

= Cc + E

Extended Example

Define a(.n) = t " h / y/l n ^ Z \ {o}. xhen ®

I I Ca{n) + Ci,

[a(m ),e] = 0. Note that by our choice of d, above [^>a(m )] =2ma {m ). The Lie algebra a is a Heisenberg algebra. It can be identified with the Heisenberg algebra of Section 2.2., Example 2, by

Now we want to apply Proposition 2.8.4. We have L(d*) is unitarizable (Theorem 6.4.3), [d,a] c a, cr(a) = a [ 0 for all a e fl = {«(,, a j . Thus Lid*) is completely reducible as an a-module. Note that with á ~ a + Cd, a decomposition of Lid*) into irreducible S-modules is also a decompo­ sition of Lid*) into irreducible a-modules (see the proof of Proposition 2.8.4). Now consider the space - k S

*-0 formed from the weight string {ir^r^yd* It is evidently an fi-module. Now & has the triangular decomposition á = d_-f-(Ce -l- Cd) -I- fi+. Let Vj G Lid*y'°'''^‘‘^* \ {0}. This spans L(á*)^''»''i^‘'* and is evidently a highest weight vector for S (in the displayed triangular decomposition). Since ^v¡ ^ 0, this vector generates a Verma module MUr^r^Vd*) c Vj [here ir^r^yd* is considered as a linear functional on (Cc -t- Cd)], and by Section 2.13 it is an

669

Appendix to Chapter 6

irreducible a-module. By the remark above, it is an irreducible a-module. It follows that its character is chM ((ro r,)V * - k8) = e{(r^r,yd* - k8) O = dim a “ In this case Q+= Z+5 and

(1 - e ( - a ) y " ' \

(see Proposition 2.19). = 1 for all

e Z+. Thus

chM ((ror,)'d* - k8) = e((rori)'d* - A:5) O (1 “ e { - k 8 ) y = «{(roriYd* - k8) n (1 - 9*) k= l

= e{ir^r,yd* - k8) E p(k)q>^. k= 0

But we also have chVj = e((rori)''d* - *8)chFo = e^iror^yd* - k8)bf., since dim (A.31)

is constant on the orbit Wk, Thus by (A.30), ch

= ch Vj.

But now there is a nice trick that shows that — k8) = Vj. We already know that M d r ^ r ^ d * — k8) ^ Vj. Hence for all weights a, dim M d r ^ r y d ^ Y < dim Vf. But (A.31) then gives equality. Thus we have proved that Vj is an irreducible a-module, L(d*) = ®j^jVj a direct sum decomposition of L(d*) into irreducible a-modules. We can now give a structural interpretation to (A.24). Each weight space jg dimensional and is spanned by a vector that is annihilated by a^_. These highest weight vector or “vacuum vectors” span the entire space annihilated by a+. Equation (A.24) expresses a factorization of L(d*) as an irreducible a-module times the space of vacuum vectors. This was one of the insights that led to the Frenkel-Kac vertex operator construc­ tion of affine representations ([F-K, KMPS, MoPi]). It is interesting to look at the meaning of Proposition 6.7.7. Corresponding to the Bruhat ordering (A. 17), we have the following inclusions amongst

Extended Example

Verma modules for M(A), A e p^: / Ai(A) \

and furthermore there are no other submodules. Since tv >v • A is an injective map and tv • A c A J. (3^, it is clear that for any e {w\ii e (w • A)i Q+} is finite and hence ■A) = (0). We now consider the character of the irreducible module L(A) = M(A)/(M(rQ • A) + M(fi • A)). As a first estimate we have ch M(A) - {ch M(ro • A) + ch M{r^ • A)}. But A/(fo • A) + M(ri • A) is not a direct sum; indeed all the submodules M(w • A), Z(tv) ^ 2 lie inside the intersection of these two modules. Thus we have removed ch Mir^r^ • A) + ch Mir^r^ ■A) twice, and as our second esti­ mate we have ch M(A) - ch M{r^ • A) - ch M (rj • A) -1- ch M{rQV^ • A) -I-

ch M{r^rQ ■ A).

Of course the third level has now to be corrected because we have added too much, and so by the principal of exclusion and inclusion we obtain c h L (A )=

£ (-l)'^ '^ ^ c h M (w A ). w^W

Since ch M(w • A) = • A)/n^^eA+d ~ ^-a)dimg“ Proposition 2.5.3), we obtain in this way a simple explanation of the character formula (6.29). For more on this type of approach to the character formula in general, see [GLl] and [GL2].) APPENDIX TO CHAPTER 7 Next we consider the Lie groups G and G of Section 6.1 that are attached to §I2(IK). We can derive a considerable amount of information by constructing a special integrable representation of ^ I2( 1K).

Appendix to Chapter 7

Let ( it, V), where V = §I,(IK):

671

be the natural 2-dimensional representation of

\c

d)[v )

(A.32)

[cu + dv ) ’

and set L F ~ IK[r**] ® F. Then we have a representation of L § l2(IK) on L F by (A.32), where now a , b , c , d , u , v e By letting (5 act trivially, we can lift this to a representation ^ g l( L F ) . Define a Z-grading on L V (as a vector space over K) by deg| deg

I = 2k, =2 k-l.

and observe that this is compatible with the Z-grading of i l 2(IK), namely for X e §i^([K)*, y G L F '”, X • y G LF*+'”. For example, deg t ^ f = 2p - 1, deg| Q j = 2q, deg(i^/ ‘10 1) = deg|

^ = 2{p + q) - 1. Now we extend

our representation to a representation tt of ^12( 1^ ) on L V by defining d ' X = kx on the elements x e LK^, /: e Z. Since the real root spaces of ^I2(1K) are spanned by the elements t^e and t ^ f , k ^ Z, it follows that ( , LV) is integrable. Thus affords a representa­ tion TT of G and G = G(P) on LV. Now we observe that t t

t t

K exp5i*e)|“ j =

1 0

K ex p si* /)(“ ] =

1 St*/

1 jU i’

:i(;i

Thus ir(G) c S L 2(IK[r±‘]). The study of SL2(R) for commutative rings is a whole world in its own right. If f? is a euclidean ring, then 5L 2O?) is generated by the elementary matrices ( j

(j

5L2(lK[r±*])(see [HoM]).

J ) . a G R. In particular we see that ir(G) =

672

^i^^-An Extended Example

Now we invoke the result of Exercise 6.30. Since ker tt = ker TT c Z(G) and G —>5L2(lK[i -^]) is central. According to Theorem 6.3.14

c ]^, we have

Given an integrable representation (i//,M), 9fr(h^Jis)h^f±s)) acts on as ^(+5)Yhich in general is not trivial.Vhus we see that Z(G) = [K^ X {±1}. For LV, aQ ai ^ c acts as 0, so . Since | ¿ j ^

is a weight vector with

weight A where = 1, we see that — does not act trivially, namely ^ ker tt. [For the adjoint representation, however, the weight satisfy = and furthermore e 2Z. Thus hc^s)h^(,±s) acts trivially for all s, as we would expect.] We conclude that we have the central extension {1} ^

G

5L2(IK[i±']) -> {1}.

According to Exercise 6.30 the mapping Ad induces an epimorphism 5L2(K [i±i]) and Ad(G) - SL2(K[t - ^])/Z(SL2(K[t ± IP

A d(G ), It is not hard to see the centre is

^ j , and hence Ad(G) -P5L2(lK[i=^^]) == 5L 2(K [i± ^])/{± l}

(projective special linear group). We have already defined

/>= Zd* + Zh ( tr ) + Now we wish to consider the larger group G = G(P) = GX, where X • Hom(P,K^).

Appendix to Chapter 7

673

Consider an element e H. As an element of X it corre­ sponds to the homomorphism of P into K” satisfying d* ^

= to, f^cc,/2,a^'y^(a,/2.c:n = S ^ 1.

Clearly X = H X X q, where jifo =

e H o m (P ,K O k (d * ) = < p (y ) = 1

= Hom(Z5,IK^) = Hom(Z,[K=") == K^. Also by the corollary to Proposition 6.3.12, G n X = H, G n X o = l , G = G ■X q. Finally, recalling X q ~ {;t' e X\x(Q) = 1} (see Theorem 6.3.14), Z (G ) = X q = H om (P/!2,IK'') = Hom(Z X (Z/2Z),IK ^) / Z = Hom(Z,lK^) X Horn — ,IK^ = K"^x{±l} = Z ( G ) . In fact f o i h ^ H and e X q, hxoiQ) = 1 => ;^o = 1> hence Z(G) = Z(G). Thus G = G X IK^, Z(G) = Z(G) = IK^ x ( + l}. Finally, we consider the group ¿¡/~ Aut(§l2(IK)). Though Ad we have .QfD Ad G = G /Z G = G • Xo/ZiG) = P5L2(IK[t ±‘]) • X^. We already know that P5L2(IK[i **]) embeds in as the group of inner automorphisms generated by the elements |expad se„|s e K-*, a e " A ,

e„ ^

or equally well by the elements {exp ad sc,, exp ad s/,|s e K^, i = 0,1} (Corollary to Proposition 6.1.9). If x ^ is defined by x(8) = a e K^, Xid*) = x(<Xi/2) = 1 then a: acts on i l 2(IK)'"“»^”“' as o'". Let 0 e S3/, then Of) is some split Cartan subalgebra and by Thm. 7.4.9 there is an element


674

Extended Example

Let n ^ isfies fjL2^ =

G satisfy l^J = w. Then 1x 2 == (Ad n) ^Ad
sat-

= ^I2(K)" for all a. Case 1. /Lt*«/ = oiiy i = Q? 1- In this case 112^^2 But then In particular /jl2[^12{^)^\ = M2' a / ) = Then M2^z ~ ^/] = 2/i,2^z leads at once to 112^ 1^~ and fi2fi = i = 0,1. Let x ^ HomCQ, K^) be chosen so that A'(<^/) = ^ = 0? 1; Af induces an automorphism, also denoted by X, of g by A la" = multiplication by ;^(g). Then x ~^t^2 [e^, a / , /¿\i = 0,1}, and so fjL;^ — at” V 2 as 1 on §I2(IK). Now it is a straightforward exercise to show that ¡x^id) = d + ac for some a e K. Conversely if « e K, then there is an automorphism cp of id,
^g C, geG, ATeHom(i2,K^).

Case 2. At*n^o = In this case we introduce the automor­ phism y of the Coxeter-Dynkin diagram T of A : y : Vq (see Section 3.4). This determines an automorphism y of ^12( 11^) by Corollary 4.4 which effects Cq <-> «o ^ /0 ^ f v nnd y ’* : «n ^ «1 This automorphism can be lifted (not uniquely, but up to a coset of C) to an automorphism y of ^ I2( 1K). Then replacing fi2 by y^t2? back in Case (1). Case 3. /x*!! = - I I . In this case we use the automorphism -cr of g. We have ((-o-)jLL2)*n = II, and hence we are in Case (1) or (2). In summary every element of Aut(^l2(IK)) is expressible in the form A d(g)Arly(-o-)% where g g G, x ^ Hom((2, K“^), ^ ^ C, y ^ Aut(F), e ^ {0,1}. Heaven and earth grow together with me, and the ten thousand things and I are one. We are already one—what else is there to say? Yet I have just said that we are one, so my words exist also. The one and what I said about the one make two, and two and one make three. Thus it goes on and on. Even a skilled mathematician cannot reach the end, much less an ordinary man... Enough. Let us stop! —Chuang tsu

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Index

Absolutely irreducible representation, 35 Ad-nilpotent: element of a Lie algebra, 28 locally, 28 Adjoint group, 320 Adjoint representation, 30 Algebra, 1 associative, 2 commutative, 2 identity element, 2 proper ideal, 3 right, left, two-sided ideal, 3 structure constants, 3 Associative algebra, 2 commutative, 13 free, 13 modules and representations, 34 Base of a root system, 240, 472 Base ring, 9 BGG duality, 198 Bilinear form: alternating, 291 invariant, 35 locally invariant, 355 Birkhoff decomposition, 523 Borel group, 518, 629 Branching function, 665 Bruhat decomposition, 126, 523 Bruhat ordering, 426 Campbell-Baker-Hausdorff formula, 70 Cartan matrix, 258 affine, 258 decomposable and indecomposable, 251 finite type, 276 hyperbolic, 485, 482 indefinite type, 276 realization, 330 symmetrizable, 251

Cartan matrix of an associative algebra, 185 Cartan or generalized Cartan matrix, 250 Cartan subalgebra: of a finite dimensional Lie algebra, 640 of a Kac-Moody algebra, 635 Casimir-Kac operator, 372 Casimir operator, 119 Category 142 Central extension, 50 Central extension of abelian groups, 289 Centralizer, 84 Character, 130 Character map, 152 Characteristic set, 204 Cocycle, 290 Combinatorically symmetric matrix, 247, 353 Completely reducible representation, 34 Composition series, 149 equivalent, 149 local, 149 proper and extraneous factors, 149 Connected through (weights), 513 Connecting homomorphism, 78 Contragredient: bilinear form, 169 hermitian module, 169 hermitian unity module, 169 Contragredient Lie algebra, 310 adjoin group, 320 Cartan matrix, 324 display, 311 integrable, 323 invariant, 359 minimally realized, 350 radical free of a pair 340 rational form, 352 real and imaginary ro
682

Coroot, 321 Covering, 50 morphism, 50 universal, 51 Coxeter-Dynkin diagram, 250 Coxeter group, 419 Coxeter matrix, 418 Coxeter number, 477 Coxeter transformation, 477 Crystallographic, 425 Demazure-Tits group, 302 Denominator formula, 533 Depth function, 140, 510 Derivation, 23 inner of a Lie algebra, 27 inner of an associative algebra, 24 Derived Lie group of a Kac-Moody Lie algebra, 488 Display, 311 Edge (of a support), 615 Eigenspace, 599 Elementary automorphism, 28 Endomorphism: diagonalizable, 588 Jordan-Chevalley decomposition, 594, 597 locally finite, 591 minimal polynomial, 587 primary decomposition, 588 semisimple, 588 strictly triangularizable, 602 triangularizable, 602 Exchange condition, 424 Ext, 72 Extension of modules, 71 Exterior algebra, 14 Fan, 104, 130 source of, 130 Finite root system, 232 ambient space, 232 base, 240 Cartan matrix, 246 coroot of a root, 303 decomposable and indecomposable, 239 dual, 303 fundamental weights, 303 highest root, 303 highest short root, 303 isomorphism of, 233 natural bilinear form, 256 positive system of roots, 242 reduced and nonreduced, 237

Index

root and coroot lattice, 303 simple root, 240 weight and coweight lattice, 303 Weyl group of, 232 Flag, 603 Forest, 249 Formal exponential, 130 Friedrichs’ theorem, 68 Fundamental chamber, 438 Fundamental region, 444 Generalized contragredient Lie algebra, 376 Generalized eigenspace, 600 Generating function, 130 Geometric lattice, 217 automorphism, 217 definite and indefinite, 218 determinant, 218 dual, 219 even and odd, 218 index of duality, 220 isomorphism, 217 of type A , 223 of type D , 222 of type E , 226 orthogonal sum of, 221 rationalization, 217 realization, 217 signature, 218 sublattice and full sublattice, 218 type I and II, 218 unimodular, 220 Graded: homomorphism, 17 ideal, 18 module, 15 subspace, 18 Gradings, 15 Graph, 248 incidence matrix, 248 Group algebra, 130 Heisenberg algebra, 23 Highest root, 270 Highest weight, 103 module and representation, 103 series, 150 weight vector, 103 Hoistable representation of a Lie algebra, 604 Homogeneous element (of a Kac-Moody group), 528 Homomorphism: graded, 17 homogeneous, 16 Hyperbolic plane, 224

Index

Ideal, 3 residually nilpotent, 165 Imaginary root, 317 Imaginary roots, of a set of root data, 464 Indecomposable blocks of a matrix, 352 Index of connection, 271 Inferior matrix, 278 Integrable ^ 12-module, 124 Integrable module, 482 Integrable representation, 482 Invariant bilinear form: proper, 359 standard, 365 Isotypical component, 122 Iwahori subgroup, 646 Jordan-Chevalley decomposition, 594 Kac-Moody Lie algebra, 324 finite, affine, and indefinite type, 324 Killing form, 37 radical of, 36 Kostant cone, 612 Kostant partition function, 139 Lattice, see Geometric lattice Laurent polynomial, 647 Lie algebra, 2 abelian, 2 algebraic, 630 antiautomorphism, 3 bracket, 2 central simple, 83 centralizer, 3 centrally closed, 56 centre, 3 centroid, 83 derived, 4 free on a set, 61 free product of, 64 given by generators, 64 holomorph of, 82 of an associative algebra, 5 perfect, 51 presentation, 64 quotient, 4 semisimple, 5 simple, 4 solvable, 89 special orthogonal, 81 special unitary, 82 subalgebra, 3 symplectic, 82 Lie group of a Kac-Moody Lie algebra, 502 Lie ring, 280

683

Locally invariant bilinear form, 355 Locally nilpotent endomorphism, 26 exponential of, 26 Lowest weight module, 106 Minimal regular weight, 367 Module, see also Representation of a Lie algebra character of, 132 Multiplicity of a module, 150 Normalizer, 84 Null root, 258 Ore domain, 85 Partition, 135 Pentagonal number, 662 Perron-Frobenius eigenvalue, 272 Poincare series, 128 Primitive matrbc, 272 Primitive vector, 119 Principal grading, 648 Principal subalgebra, 574 Quadratic form associated with a geometric lattice, 217 Quadratic form over field of two elements, 290 Quasi-roots, 549 Quaternions, 7 Racah formula, 541 Radical of a Lie algebra with triangular decomposition, 162 Rational form or structure of a vector space, 245 Real root, 317 Realization, 330 dimension of, 330 dual, 333 natural, 339, 343 universal algebra, 334 Realization of a root system, 457 Reflection, 230 orthogonal, 232 Representation of a Lie algebra, 28 action, 29 annihilator, 29 as a module, 29 character, 132 exterior representation, 32 faithful, 29 simple or irreducible, 29 tensor product, 31 tensor representation, 31 trivial, nontrivial, 29

684

Index

Representation ring, 152 Restricted dual, 17 Restricted dual in category 158 Restricted weight lattice, 491 Root: imaginary, 317 indivisible, 496 long, short, 270 real, 317 strictly imaginary, 481 support, 464 Root data, see also Finite root system, 396 base, 472 chambers, 440 coroots, 397 diagram automorphism, 474 dual, 397 faces, 441 facettes, 440 fundamental chamber, 438 height, 404 imaginary roots, 464 morphisms, isomorphisms, and automorphisms, 431 natural expression and height of roots, 404 obtained by extension of the base field, 434 relative chambers, 457 roots, 397 standard of a realization, 397 subroot system, 435 Tits cone, 440 universal covering, 400 walls, 441 Weyl group, 408 Root string, 327, 464 Saturated set, 514 Schur’s lemma, 33 Semiprimitive matrix, 272 Semisimple representation, 34 Separating group of characters, 499 Serre’s theorem, 375 Shapovalov form, 169 Skeletal graph, 352 Skew invariant, 532 Special linear group, 122 Split simple and semisimple finite dimensional Lie algebras, 354 Standard invariant bilinear form, 365 Strange formula, 575 String function, 665 Strong exchange condition, 424 Supplement of a module, 34 Symmetric algebra, 13 Symmetrizable matrix, 360

Tensor algebra, 13 Theorem: B ernstein-G erfand-G erfand (BGG), 556 Chevalley, Peterson-Kac conjugacy of Cartan subalgebras, 635 conjugacy of bases of a finite root system, 244 conjugacy of bases for a root data, 473 Gabber-Kac, 377 Jordan-Chevalley, 605, 636 Kac imaginary root, 468 Kac-Peterson complete reducibility, 543 Poincare-Birkhoff-W itt, 41 Shapovalov determinant formula, 545 Weyl-Kac character formula, 532 Weyl-Macdonald denominator formula, 533 Theta function, 667 Tits system, 521 Tree, 249 Triangular decomposition, 95 diagonal subalgebra of, 96 extension of base ring, 99 hermitian, 100 opposite, 96 regular, 95 root lattice of, 96 root system of, 96 Triangular pair, 161 Triangularizable representation of a Lie algebra, 603 Twisted group algebra, 296 Unimodal sequence, 509 Unitarizable (highest weight module), 534 Universal algebra of a realization, 334 Universal enveloping algebra, 38 graded algebra of, 49 grading inherited from g, 48 Vacuum vector, 103 Verma composition series, 155 Verma module, 107 Vertex (of a support), 615 Virasoro algebra, 20 Weight, 92, 367, 491 dominant, 367, 491 fundamental, 491 integral, 367, 491 minimal regular, 367 Weight lattice, 491 Weight space, 92 Weight space decomposition, 92 Weight string, 508 Weight vector, 91

Index

Weyl group, of a finite root system, 232 Weyl group, of a set of root data, 408 length of a word, 408 parabolic subgroups, 415 reduced words, 408 words, 408

WIP, 401 Witt algebra, 20 WUP, 401

Z-lemma, 428

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