BSIM1 WHY? Industry switched to BSIM models � Berkeley Short channel Igfet Model � About 10 years ago industry quit using MOS level 1 � Was a big impact on students at first job(conversion form one level to another) To make hand calculation easy extract some parameter. 1
How? All parameters have Length and width modifiers Using equation,
Where P’ is BSIM electrical parameter. L-DL is effective channel length W-DW is effective channel width LP is length modifier WP is width modifier all above are electrical parameter assoi with P’ 2
BSIM DC equation
Threshold voltage The drain current The subthresod current
3
The Thresold voltage
Remember that this equation is calculated using,
4
Much worse than the old threshold Equation Not constant for a given device size Not easily worked by hand Simplified equation,
By neglecting the effect of device and lower drain induced barrier resulting from non zero VDS
5
BSIM DC equation
Threshold voltage
The drain current The subthresod current
6
Drain current Cut off : VGS < VTHN (ID = 0, neglecting STC) Linear : VDS < VGS-VTHN > 0
7
8
9
U0Z’ and U1z’ accounts for mobility degradation effect X2UO, X2U1 X3U1
sens. of trans. field mobility degrad. eff. subs. bias sens. of velocity saturation effect to substrate bias sens. of vel. sat. eff. on drain bias at Vds=VddL
LX2UO, WX2UO LX2U1, WX2U1 LX3U1, WX3U1 10
Saturated Current model
11
This equation does not depend on VDS
(are we wrong?)
12
channel length modulation
13
MUO , neglecting length and width dependence by using linear interpolation between the mobility at VDS=0(MUZ) and VDS=VDD(MUS)
Output resistance of MOS is given by,
14
Parameter λm is called mobility modulation parameter. Thus change in ro MUS( VDS=VDD) < MUZ(VDS=0) 15
For short channel length λc For long channel length λm In digital application we assume both to be zero
16
BSIM DC equation
Threshold voltage The drain current
The subthresod current
17
Subthresold current VGS< VTHN The transistor doesn’t turn off suddenly As Vgs nears Vth, it turns on gradually Two current components Weak Inversion The current we have ignored Strong Inversion The part we said was 0 before This current is due to diffusion between drain and source 18
Iweak
19
20
21
Small currents, used in low power operation Sensitive to Vgs, exponentially
�Sensitive to Temperature Gradual change
22
If Iexp << Ilimit Intersection of slopes of current curves VA (Early Voltage…)
23
The output resistance of a MOSFET, subthresold and SI region ,
24
25
26
Increases by 10X every 60-100mV change in VGS-VTHN Increase VGS or lower VTHN !!!! S = n(kT/q)ln(10) depends on n and T
27
Thanks
28