414
Compact Models for Integrated Circuit Design
With reference to Figure 11.27, the base current in SGP BJT model can be
obtained from Equation 11.52 as
I
I
V
v
C I
V
n v
B
SS
FM
BE
kT
SS
BE
E kT
=





 −





 +





 −

β
exp
e xp
1
1
2
 



 +





 −






+





I
V
v
C I
V
n v
SS
RM
BC
kT
SS
BC
C kT
β
exp
exp
1
4
  −






1
(11.116)
and the collector current is given by
I
I
q
V
v
V
v
I
V
C
SS
b
BE
kT
BC
kT
SS
RM
BC
=





 −











 +
exp
e xp
exp
β
v v
C I
V
n v
kT
SS
BC
C kT





 −






−





 −






1
1
4
exp
(11.117)
The corresponding model equations as implemented in SPICE are as follows:
I
IS
V
n v
ISE
V
n v
B
eff
F
BE
F kT
eff
BE
E kT
=





 −





 +





β
exp
e xp
1
  −






+





 −





 +
1
1
IS
V
n v
ISC
V
n
eff
R
BC
R kT
eff
BC
C
β
exp
e xp
v v kT





 −






1
(11.118)
and,
I
IS
q
V
n v
V
n v
IS
C
eff
b
BE
F kT
BC
R kT
eff
=





 −











 −
exp
e xp
β R R
BC
R kT
eff
BC
C kT
V
n v
ISC
V
n v
exp
exp





 −






−





 −





1
1  
(11.119)
Comparing derived Equations 11.116 and 11.117 with the SPICE implementation corresponding Equations 11.118 and 11.119, we find: I SS   =  IS eff ;
C 2 I SS  = ISE eff ; C 4 I SS  = ISC eff ; β FM = β F ; and β RM = β R . In addition, the parameters
n F and n R are included as the fitting parameters to improve the accuracy of
data fitting with the model.
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