Design and Fabrication of the Guided Wave Devices at North Maharashtra University, Jalgaon D. K. Gautam Department of Electronics, North Maharashtra University, Jalgaon – 425 001(MS) INDIA D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Present trends of Optoelectronics
In India Designing, modeling and analysis of lasers and other devices are being carried out
In abroad Standardization in design,analysis and fabrication Optoelectronics Integrated circuit
Optimization of Optic fibers Optoelectronic materials thin films Device fabrication is being carried out at few places
Micro-machineries, short wave length lasers, optical computing Applied opt-electronics equipment Guided wave remote controlled automatic equipments
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Optical Communication Networks are being installed in India
Inevitable need for the developing the
INDEGENEOUS technology for Fabricating the components required for the communication networks
Cost Effectiveness D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Various Components required for the networks
Passive Power Splitters / Combiners Modulators / switches Multi/Demultiplexers Isolators
Active Laser Diode Amplifier LED
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Next Generation Computers and Integrated Circuits Demand for
Further Miniaturization for Increased Speed Higher Capacity That Needs
Tighter Confinement of Light New class of Devices
Photonic Crystal Devices D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Research & Development strategy at N.M.U.
Department of Electronics
First Tire
Second Tire
Third Tire
Design & Development Laboratory
Sophisticated Clean Room
Mass Scale Production facilities
Indigenously Developed Software Tools
Indigenously Developed Fabrication Machines
Characterization tools
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Department of Electronics, North Maharashtra University Established 10 years ago One of the Pioneer Institutions to Initiate the work related to optical guided wave devices
Capable of Design
Fabrication
Some Fabrication Facilities have been developed already, Work is in progress to develop other facilities
Active / Passive Devices D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
CAD Tools CAD Tools Based on BPM and FDTD Applicable to the Passive Devices: Optical Waveguide Waveguide Transitions, Bends, Junctions Optical Multi/demultiplexer
Tools for Quantum Well Structures CAD Tools for the design of the Laser diode Blue Laser Diode GaN/AlGaN Heterostructure Laser Diode ZnO/MgZnO Heterostructure Laser Diode
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Fabrication Infrastructure Available Clean room Photolithography facilities Chemical Draft Indigenously Developed Machines Characterization Laboratory Communication Laboratory
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Design Group
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Rib Waveguide Design w t
GT
Upper clad layer dh Guide layer
SiO2 buffer layer Silicon Substrate
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
w d h
Effective Index Method Applied to the Rib Waveguide Structure
Non Guiding region
GT
Guiding region
Non Guiding region
STEP I Air
Air
Air
Upper Clad
Upper Clad
Upper Clad
Guiding Film
Guiding Film
Guiding Film Lower clad
Guide I
STEP II
Lower clad
Lower clad Guide II Clad
Guid e
Nef1
Guide III
Clad Nef1
Nef2 Guide IV
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Main Equations used to Implement the Beam Propagation Algorithm e( x, y , z 0 ) = ∑a n E n ( x, y ) n
an =
+∞
∫ ∫ e( x , y , z
0
) E n ( x, y )
Decomposition to the Fourier Components
−∞
e( x, y, z 0 + ∆z ) = ∑ a n E n ( x, y ) exp(− jk n ∆z ) n
Propagation in Fourier Domain
Inverse Fourier Transform − jk 2 E1 ( x, y, z 0 + ∆z ) = e( x, y, z 0 + ∆z ) exp ∆n 2n0
Correction for the perturbation in Refractive Index
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Our Tools Applied for the Design of the Directional Coupler Based Demultiplexer λ2
w s λ1,λ2
Guide I Guide II
W=waveguide width S=separation between the waveguides Advantage: Easy Fabrication Method
λ1
Bpm simulation results for the propagation of two wavelengths through the demux
λ1 = 1.3 μm λ2 = 1.304 μm Guide Separation = 2.5 μm Guide Thickness = 4.4 μm Rib Width = 9 μm Rib Height = 2 μm Clad Thickness = 2 μm Device Length = 7.3175 cm
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Hetero-structure Laser Design
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Physical Equations Electrical Equations
Optical Equations
Poisson’s Equation
Wave Equation
Continuity Equations for electrons and holes
Rate Equation for Photons
Current density Equation Output Characteristics D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Blue Laser Structure Used for the Analysis Y
x
p-contact
Upper clad Active layer
Lower clad n- Substrate n-contact
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Structural Parameters used for Analysis Layer
Thickness in nanometer
Doping Concentration in cm-3 .
Refractive Index
Substrate
1180
3 * 1018
3.6
767
7 * 1017
2.5878
13 %
17 %
50
1.7 * 1016
2.78
0 %
3 %
138
7 * 1016
2.5878
13 %
17 %
GaAs
Lower clad
% of Magnesium
−
% of Sulphur
−
ZnMgSSe
Active layer ZnSSe
Upper clad ZnMgSSe
Device width: 60 micron Channel width: 5 micron Channel depth: 0.5 micron
Physical Parameters Used for the Analysis Physical parameter Electron mobility Hole mobility Electron affinity Electron life time Hole life time Concentration in active layer Energy band gap Cavity length Reflectivity of each facet Thermodynamic temperature
value 600 cm2/volt-second 30 cm2/volt-second 3.9 electron volt 5 nanosecond 5 nanosecond 1.7 * 1016 cm-3 . 2.7 electron volt 700 microns 0.237 3000K
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Plot of Intensity(relative) verses Wavelength 1 0.9
Intensity (relative)
0.8 0.7 0.6 0.5 0.4 0.3 0.2 0.1 0 503
505
507
509
511
513
Wavelength (nanom eter)
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Current verses Voltage Characteristics 350
Current (m illiam pere)
300 250 200 150 100 50 0 3.55
3.6
3.65
3.7
3.75
3.8
Voltage (volt)
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Plot of Output Power verses current 19.75
Pow er (m illiw att)
15.8
11.85
7.9
3.95
0 0
50
100
150
200
250
300
350
Current (milliampere)
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Field Intensity Distribution in X-direction 1 0.9
Intensity
0.8 0.7 0.6 0.5 0.4 0.3 5
15
25
35
45
55
Distance X (micrometer)
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Field intensity distribution in Y-direction Active layer
1
Substrate
0.9 0.8
Upper clad
Lower clad
Intensity
0.7 0.6 0.5 0.4 0.3 0.2 0.1 0 700
1000
1300
1600
1900
2200
2500
Distance Y(nanometer)
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Analysis of optical field confinement
Upper Clad
ncu
Y Active Layer nf Lower Clad
Y
Nl
Nm
Nr
ncn
X X
Waveguide structure used for the light confinement in the vertical direction.
Waveguide structure used for the light confinement in the horizontal direction
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Full width of half maximum of field spreading as a function of channel width at 507 nanometer
Full w idth at half m axim um
35 30 25 20 15 10 5 0 0
5
10
15
20
25
30
35
Channel width (micron)
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Effective refractive index variation with the channel width 2.60527 2.605265
Effective index
2.60526 2.605255 2.60525 2.605245 2.60524 2.605235 0
5
10
15
20
25
30
35
Channel width (micron)
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Photonic Crystal Device Design
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
WHAT IS PHOTONIC CRYSTAL?
Photonic Crystal - Photonic crystals are microstructured materials in which the dielectric constant is periodically modulated on a length scale comparable to the desired
wavelength
of
operation
and
in
which
electromagnetic waves of desired frequencies are forbidden.
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Why Photonic Crystal ? Most Important Points for today's VLSI/ULSI and Communication Technology : Speed – Photonic crystals uses photons hence speed is greater than electro-optical devices. Information carrying capacity – Photonic crystals uses photons hence information carrying capacity is greater. Size – Photonic crystals has the dimensions of nano-sizes hence very compact size devices are possible. All-optical IC’s – All-optical IC’s can be developed because using photonic crystals various devises can be fabricated such as lasers, filters fibers, multiplexer/demultiplexer,
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Semiconductor Semiconductor crystal crystal Periodic Potential Due to Periodic Atomic Lattice Bragglike diffractio n from atom Forbidden Gap for electrons
Photonic Photonic crystal crystal Periodic Potential Due to Lattice of macroscopic dielectric media Braggscattering at the dielectric interfaces Forbidden band gap (Photonic band gap) for photons
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
One dimensional photonic crystals
z
y x
Periodic in one direction
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Two dimensional photonic crystals z
A)
y x
B) Periodic in two direction
A) Dialectic rod PC with triangular lattice - lattice constant 700 nm, rod diameter 500 nm, rod height 3.9 µ m. B)
Air column PC with triangular lattice - lattice constant 580 nm, column radius 430 nm, column height 4.2 µ m.
(Obtained by Reactive ion etching of Si)
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Three dimensional photonic crystals
z
y x
Periodic in three direction
d w Logpile type PC –
Facets of a Si
d = 4.2 µ m,
inverted opal.
w = 1.2 µ m PBG is in infrared range
PBG Range
88% infiltration- 1.40 - 1.48 µ m 100% infiltration- 1.46 - 1.55 µ m
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Defects in Photonic Crystals
Point Defect
Line Defect
Resonant Cavity
Waveguide
(Traps Light)
(Transports Light)
Planer Defect
Perfect Dielectric mirror (Reflects Light)
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Fabrication Group D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
High growth rate techniques FHD
Sol-gel
PECVD
1. High growth rate 2. Porous Films 3. Poor uniformity 4. High temperature process 5. Annealing needed
1. High growth rate 1. High growth rate 2. Porous film 2. Dense film 3. Poor uniformity 3. Good uniformity 4. Low temperature 4. Low temperature process process 5. Annealing needed 5. Annealing not required 6. Useful for 6. Cannot be used in microelectronics microelectronics
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Chemical Vapor Deposition PECVD Sr. Properties APCVD LPCVD Techniques No. 300-500
500-900
100-350
Materials
SiO2
Poly-Si, SiO2, Si3N4, SiOxNy
Si3N4 , SiO2, SiOxNy
03.
Particles
Many
Few
Many
04.
Film Properties
Good
Excellent
Excellent
05.
Advantages
Simple reactor, Fast Deposition,
Excellent purity and uniformity
Low temp, Fast deposition
06.
Disadvantages
Low deposition rate
Chemical and Particulate contamination
07.
Applications
Poor step coverage & particle contamination Passivation, Insulation
Gate metal, Passivation, Insulation
Final Passivation, Insulation
01.
Temperature (oC)
02.
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Conventional CVD Technique Use of Silane
Dichloro - Silane • Toxic • Explosive • Pyrophoric • Corrosive
Solution is
Dangerous in handling
TEOS Extra Safety Measures required More Deposition Cost
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
TEOS-CVD Deposited films Show
Advantages
TEOS is non Excellent toxic uniformity Non Conformal step Pyrophoric coverage Stable, inert Good film liquid properties used in bubbler Reaction Handling is [Si(OC2H5)4] + O2 =easy SiO2 + by products D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Why SiO2 Films for Optical Devices? Matured Process Technology Refractive Index matches with the Optical Fiber Minimizes the coupling losses Polarization independent operation Easy Fabrication High integration capacity Low manufacturing cost
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Why Si3N4 and SiOxNy Films? Superior material properties like: High density, High electrical resistivity, Resistance to sodium ion, Moisture permeation, High thermal stability Adjustable refractive index Adjustable film stress D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Optimization of process parameters Flow rate Chamber pressure Substrate temperature TEOS temperature Reactor geometry Material of electrode Inter electrode spacing Electrode type
Growth rate
RF Power Residence time
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Processing Parameters Sr. No.
Process parameter
Physical value
1
Chamber Pressure
1 Torr
2
TEOS flow rate
3
O2 flow rate
4
TEOS Bubbler temp.
450 C
5
RF power
40 W
6
RF frequency
7
Substrate temperature
3 SCCS 15 SCCS
13.56 MHz 300 0 C
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Thickness Profile of SiO2 Films by PECVD
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Refractive Index Profile of SiO2 Films by PECVD
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
FTIR Transmittance spectrum of SiO2 Films by PECVD
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Transmittance Spectra of SiO2 films by PECVD S.N.
Si-O-Si stretching (cm-1 )
Si-O-Si bending (cm-1 )
Si-O-Si rocking (cm-1 )
FWHM
Authors
01
1070
810
450
88
L. Zajickova et al
02
1074
820
---
92.8
Ying-Chia CHEN et al
03
1080
800
---
---
Kunio Okimura et al
04
1069
---
---
---
K. Ramkumar et al
05
1072
820
447
---
Nur Selamoglu et al
06
1080
---
---
140
William J. Patric et al
07
1070
---
---
67.7
K. Ishii et al
08
1076.2
814.3
447.5
85.68
Present study
EDX of the deposited SiO2 films by PECVD
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Surface Morphology
Microphotograph of granular SiO2 film
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Surface Morphology
Microphotograph of uniform SiO2 film
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
EDAX of Deposited Silicon Nitride Films Element App Conc. NK 5.17 Si K 51.30 Cl K 1.27 Totals
Intensity Corrn. 0.1488 1.0817 0.6157
Weight% Weight% Sigma 34.78 1.70 47.42 0.82 2.06 0.30 84.26
Atomic% 58.70 39.92 1.37
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
FTIR Absorption Spectra of Deposited Si3N4 Films Si-H Stretch Si-N-Si Stretch Si-N Vibration 493.3 cm-1
N-H 1579.8 cm-1
Absorption
N-H Stretch 3378.8 cm-1
N-H bending 1179.9 cm-1
Wavenumber (cm-1 )
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
Total Hydrogen Concentration Vs. Substrate Temperature 7
H Concentration (X10
23
cm -3)
6
Si-H N-H H total
5 4 3 2 1 0 740
780
820
860
Deposition tem perature ( oC)
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
SEM of Deposited Silicon Nitride Films
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
CONCLUSIONS The Department of Electronics has developed the capabilities to design various guided wave active and passives devices including laser diodes, optical power splitters, multi / demultiplexers etc The infrastructure for the fabrication of the devices has been partly established and rest of the facilities would be established in near future
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA
D. K. Gautam, Department of Electronics, North Maharashtra University, Jalgaon-425 001 (MS) INDIA