Product Documentation
Spectre Circuit Simulator Components and Device Models Reference
Product Version 23.1, June 2023

Reference

Model Equations

Some important model equations are listed as following for your reference:

Basic Equations Solved in the HiSIM SOI Core Part

Though all following descriptions are written for the n-channel MOSFET, they are also valid for the p-channel case. The Poisson equation solved in HiSIM SOI together with the Gauss law and boundary conditions together with the approximation of the linearly decreasing carrier density to the depth direction are

where Q’s are charges induced within the SOI-MOSFET as depicted in 32-4 and Qh is the excess charge in the SOI layer due to the impact ionization, and

where VFBC is the flat-band voltage, TFOX is the physical gate-oxide thickness, and is the threshold voltage shift in comparison to the threshold voltage of a long-channel transistor [4]. is the permittivity of Si02. are the permittivity of vacuum and the dielectric constant of SiO2, respectively.

Eqs. (6)– (8) are solved simultaneously within HiSIM SOI. For the body-tied case, the potential node is connected to the external node potential and solved by the circuit simulator. The solution takes place at source side and drain side. Prior to the Newton iteration, an approximated, analytical initial value for each variable is estimated in the code.

Figure -4 Band structure of SOI-MOSFET and generated charges

All device characteristics are determined on the basis of the charge control by applied voltages. All charges induced within SOI-MOSFET are functions of surface potentials written as

Drain Current

Under the gradual-channel approximation with further approximations of an idealized gate structure and uniform channel doping, the drain current Ids is written as:

Threshold Voltage Shift

The surface-potential-based model requires no threshold voltage Vth in its core description of the model. However, HiSIM SOI has opted for modeling various submodels such as short-channel effects as a Vth shift from an otherwise ideal case.

The whole contribution to the Vth is summarised as

Vth = Vth, SC + Vth,R + Vth,P + Vth,SCR + Vth,W + Vth,sm - Spg

The modeled Vth is incorporated in the S iteration can be viewed as consisting of two main effects or components:

(I) the short-channel effect: Vth, SC

(II) the reverse-short-channel effect: Vth, R and Vth, P

The separation into these two components ( Vth = Vth, SC + Vth, R (or Vth, P)) is schematically shown in Figure 32-5.

Figure -5 Schematic plot of the separation of Vth into the contributions of the short-channel and the reverse short-channel effect.

Mobility Model

The low-field mobility is described with the following expressions and includes the three independent mechanisms of Coulomb, phonon and surface-roughness scattering:

Channel-Length Modulation

As the gradual-channel approximation is not valid for large Vds causing the pinch-off phenomenon in the channel. Without taking into account the pinch-off phenomenon, the calculated channel conductance gds enters abruptly into the saturation condition. To include the pinch-off phenomenon in HiSIM, we apply the conventional method of modeling the pinch-off region ( L) separately from the rest of the channel as depicted in Figure 32-6:

Figure -6 Schematic showing the correlation among physical quantities in the pinch-off region.

After taking into all effects, the final L is derived as:

Narrow-Channel Effects

The Vth reduction for reduced channel width (Wgate) is modeled under inclusion of the edge-fringing capacitances Cef at the edge of the trench as:

Temperature Dependences

The temperature dependence is included automatically in the surface potentials through , which is the inverse of the thermal voltage. Additionally the band gap, the intrinsic carrier concentration, the carrier mobility, and the carrier saturation velocity are also temperature dependent.

Drain-side resistance

Source-side resistance

Gate resistance

Capacitance

Intrinsic Capacitance

The intrinsic capacitances are derivatives of the node charges determined as

Overlap Capacitance

To consider the overlap capacitance, the flag COADOV must be selected to 1, which is the default. The overlap capacitance includes three options as summarized in 32-7, where the drain side and the source side are treated as identical. If Flag COOVLP=0, the overlap capacitances are treated to be constant. If CGSO and CGDO are defined, these values are taken. If they are not defined, the values are calculated with the overlap length LOVER and oxide capacitance CFOX.

Figure -7 Model options of the overlap capacitance at the drain side are summarized.

Gate-Fringing Capacitance

The outer fringing capacitance is modeled as

Leakage Currents

Substrate Current

The substrate current is derived as

where

and Xj is the junction depth.

Gate Current

All possible gate leakage currents are schematically shown in Fig. 32.8

Between Gate and Channel, Igate

Between Gate and Bulk, Igb

The Igb current under the accumulation condition is modeled as

Between Gate and Source/Drain, Igs/Igd

GIDL (Gate-Induced Drain Leakage)

Floating-Body Effect Model

Model selector COFBE as well as COISUB must be set to 1 to activate FBE model. In HiSIM SOI, Qh is modeled as follows:

History Effect Model

Time constant for the history effect is modeled as:

where HIST1 and HIST2 are history effect model parameters.

Self-Heating Effect Model

The self-heating effect is modeled as a C-R thermal network with a heat resistance parameter RTH0 and capacitance parameter CTH0. The flag COSELFHEAT must be equal to 1 and RTH0 must not be equal to zero to activate this model. The SHE should be switched on/off only with the model flag COSELFHEAT.

Figure -8 Thermal Network applied for the self-heating effect

Source/Body and Drain/Body Diode Models

Diode Current

Between drain and body

The forward and backward currents between drain and body are calculated as:

The drain-body current equations are derived as follows:

Between source and body

Body-Tie Models

HiSIM SOI considers both the floating-body and the body-tie structures.

Body-Contact Capacitances

ABTN = LBT ·WBTN

ABTP = LBT ·WBTP

Overlap capacitance of body-tie area

The capacitance between the body-tied gate (hammer head) and the body-tied well is treated as MOS capacitance.

Cgb,bt = CbtN · ABTN + CbtP · ABTP

Overlap capacitance of body-tie periphery

Instance parameters PSBCP and PDBCP are introduced to take into account the overlap capacitance of the periphery of the body-tie contact. These lengths are added to the Weffc as:

Weffc,source = Weffc + PSBCP

Weffc,drain = Weffc + PDBCP

where

Weffc = Wgate - NBT · XWDBT- (2 - NBT) · XWDC

Diode current of body-tie periphery

The diode current also flows at the body-tie periphery. Therefore the lengths determined by the instance parameters PSBCP and PDBCP are added the width as

Weff,source = Weff + PSBCP

Weff,drain = Weff + PDBCP

where

Weff = Wgate - NBT · XWDBT- (2 - NBT) · XWD

Gate-Fringing Capacitance

For body-tied devices, an additional gate-fringing capacitance is considered between gate and body:

Noise Models

1/f Noise Models

The 1/f noise is caused by both the carrier fluctuation and the mobility fluctuation. The final description for the drift-diffusion model is

where the parameters NFALP and NFTRP represent the contribution of the mobility fluctuation and the ratio of trap density to attenuation coefficient, respectively.

Thermal Noise Model

Van der Ziel derived the equation for the spectral density of the thermal drain-noise current at temperature T by integrating the trans-conductance along the channel direction y based on the Nyquist theorem

where s, d and av are mobilities at the source side, the drain side, and averaged, respectively.

Induced Gate Noise Model

Coupling Noise Model

Non-Quasi-Static (NQS) Model

Formation of carrier

Carriers in the channel take time to build-up as opposed to the Quasi-Static (QS) approximation. To consider this phenomenon in HiSIM, the carrier formation is modeled as

where q(ti) and Q(ti) represent the non-quasi-static and the quasi-static carrier density at time ti, respectively, and t = ti – ti-1 is valid. Above equation implies that the formation of carriers under the NQS approximation is always delayed in comparison to the QS approximation, which is the basic origin of the NQS effect.

Delay Mechanisms

Weak inversion

Strong inversion

These two delay mechanisms (diffusion and conduction) are combined using the Matthiessen rule:

Applying the same approach for the formation of bulk carriers, leads to the approximation of the bulk carrier delay as an RC delay in the form

Component Statements

Instance Parameters

Refer to the following table for Instance Parameter details:

1
l=5.0E-6 m
Gate length (Lgate).
2
w=5.0E-6 m
Gate width (Wgate).
3
ad=0.0 m^2
Area of drain junction.
4
as=0.0 m^2
Area of source junction.
5
pd=0.0 m
Perimeter of drain junction.
6
ps=0.0 m
Perimeter of source junction.
7
ngcon=1.0 -
Number of gate contacts.
8
xgw=0E0 m
Distance from gate contact to channel edge.
9
xgl=0E0 m
Offset of gate length.
10
m=1.0
multiplicity factor.
11
nf=1.0 -
Number of gate fingers.
12
sa=0 m
Length of diffusion between gate and STI.
13
sb=0 m
Length of diffusion between gate and STI.
14
sd=0 m
Length of diffusion between gate and gate.
15
pdbcp=0.0 m
Parasitic perimeter length for body contact at drain.
16
psbcp=0.0 m
Parasitic perimeter length for body contact at source.
17
lod=10.0E-6 m
diffusion length between gate and STI edge.
18
temp=0.0 C
Device temperature.
19
dtemp=0 C
Device temperature change.
20
trise=0 C
Device temperature change.
21
nbt=1.0
Number of body contact.
22
lbt=0.0 m
Length of gate over body-contact well.
23
wbtp=0.0 m
Distance of gate protrusion over body-contact well.
24
wbtn=0.0 m
Distance of gate protrusion over body-contact well.
25
abtn=0.0 m^2
Area of N^+ poly area of body contact.
26
abtp=0.0 m^2
Area of P^+ poly area of body contact.
27
nrs=1.0
Number of squares in source .
28
nrd=1.0
Number of squares in drain .
29
ldrift=1.0E-6 m
Parameter for drift region length (drain) .
30
ldrifts=1.0E-6 m
Parameter for drift region length (source) .
31
rbdb=50.0 Ohm
Substrate resistance network.
32
rbsb=50.0 Ohm
Substrate resistance network.

Model Definition

model modelName hisimsoi parameter=value ...

Model Parameters

Refer to the following table for Model Parameter details:

1
l=5.0E-6 m
Gate length (Lgate).
2
w=5.0E-6 m
Gate width (Wgate).
3
wmax=1.0
Maximum width for the model.
4
wmin=0.0
Minimum width for the model.
5
lmax=1.0
Maximum length for the model.
6
lmin=0.0
Minimum length for the model.
7
copprv=0
Previous phi_s flag.
8
coadov=1
Lateral field induced and overlap capacitances are added to intrinsic.
9
coisub=0
Substrate current flag.
10
cofbe=0
Floating-Body Effect flag.
11
coiigs=0
Gate current flag.
12
cogidl=0
GIDL current flag.
13
coovlp=0
Overlap capacitance model selector.
14
coign=0
Induced gate and cross correlation noise flag.
15
coflick=0
1/f noise flag.
16
cothrml=0
Thermal noise flag.
17
coisti=0
STI leakage current flag.
18
conqs=0
Non-quasi-static model flag.
19
corg=0
Gate-contact resistance flag.
20
coievb=0
Valence-band-electron-tunneling-current model flag.
21
cohist=0
History Effect flag.
22
coselfheat=0
Self-Heating flag.
23
covbsbiz=0
Symmetry treatment flag.
24
colgleff=0
Lgate to Leff flag.
25
coqovsm=1
Qover capacitance model selector.
26
coqbdsm=1
Gate/body contact well MOS-capacitance model selector.
27
cobcnode=0
Body contact node flag.
28
cosubscale=0
Switch scaling for Isub.
29
coisubfb=0
Switch Isub in FB mode: 0 with analytical Ids; 1 with iterative Ids.
28
info=0
print information selector.
31
qhsmax=1e-3
Upper limit Qhs .
32
dvgpsub=0
Delta VGPSUB (in addition to VFBSUB).
33
dvbssub=0
Delta VBSSUB for Qh effect.
34
type=1 -
1 for nMOS and -1 for pMOS.
Possible values are p and n.
35
version=1.40 -
Model parameter version accepts only real number values, like 1.30 for version=1.3.0. The available versions are 1.30 and 1.40. Default version is 1.40.
36
vmax=7.00E+6 cm s^-1
Saturation velocity.
37
bgtmp1=90.25E-6 eV K^-1
Temperature dependence of bandgap.
38
bgtmp2=100.0E-9 eV K-2
Temperature dependence of bandgap.
39
eg0=1.1785 eV
Bandgap.
40
xld=0.0 m
Gate overlap length.
41
xldc=0.0 m
XLD for capacitance.
42
vfbover=0.0 V
Flat-band voltage in overlap region.
43
nover=1E19 cm-3
Impurity concentration in overlap region.
44
xwd=0.0 m
Gate overlap width.
45
xwdc=0.0 m
XWD for cap.
46
saref=1E-6 m
Reference distance from STI edge to Gate edge.
47
sbref=1E-6 m
Reference distance from STI edge to Gate edge.
48
xqy=0.0 m
Distance from junction to max field point.
49
xqy1=0.0 F μm^XQY2-1
Vbs-dependence of Qy.
50
xqy2=2.0 -
Lgate-dependence of Qy.
51
rshg=0.0 Ω/square
Gate sheet resistance.
52
vfbc=(-1.0) V
Flat-band voltage.
53
vbi=1.1 V
Built-in potential.
54
nsubpl=0.001 m^-1
Modification of pocket-impurity concentration.
55
nsubpfac=1 -
Modification of pocket-impurity concentration.
56
parl1=10.0E-9 cm
SOI SCE parameter.
57
parl2=10.0E-9 m
Depletion width of channel/contact junction.
58
lp=0.0 m
Pocket penetration length.
59
nsubp=1.0E+17 cm-3
Max pocket concentration.
60
nsubp0=0.0 -
Modification of pocket concentration for narrow W.
61
nsubwp=1.0 -
Modification of pocket concentration for narrow W.
62
wl1=0.0 m
Small-size effect parameter for STI leakage.
63
wl1p=1.0 -
Small-size effect parameter for STI leakage.
64
wl2=0.0 -
Threshold voltage shift due to small-size effect.
65
wl2p=1.0 -
Threshold voltage shift due to small-size effect.
66
scp1=0.0 -
Magnitude of short-channel effect due to pocket.
67
scp2=0.0 V^-1
Vds-dependence of SCE due to pocket.
68
scp3=0.0 m V^-1
Vds-dependence of SCE due to pocket.
69
sc1=0.0 -
magnitude of short-channel effect.
70
sc2=0.0 V^-1
Vds-dependence of short-channel effect.
71
sc3=0.0 m V^-1
Vbs dependence of short-channel effect.
72
scr1=0.0 -
Parameter for SCE via BOX.
73
scr2=0.0 -
Parameter for SCE via BOX.
74
scr3=0.23 -
Parameter for SCE via BOX.
75
pgd1=0.0 V
Strength of poly-depletion effect.
76
pgd2=1.0 V
Threshold voltage of poly-depletion effect.
77
pgd4=0.0 -
Lgate-dependence of poly-depletion effect.
78
ndep=1.0 -
Depletion charge contribution to Eeff.
79
ninv=0.5 -
inversion charge contribution to Eeff.
80
ninvd=0.0 V^-1
inversion charge parameter.
81
muecb0=300.0 cm2V^-1s^-1
Coulomb scattering.
82
muecb1=30.0 cm2V^-1s^-1
Coulomb scattering.
83
mueph0=300.0E-3 -
Phonon scattering.
84
muephw=0.0 -
Phonon-related mobility reduction.
85
muepwp=1.0 -
Phonon-related mobility reduction.
86
muephl=0.0 -
L-dependence of phonon mobility reduction.
87
mueplp=1.0 -
L-dependence of phonon mobility reduction.
88
muephs=0.0 -
Mobility change due to small size.
89
muepsp=1.0 -
Mobility change due to small size.
90
vtmp=0.0 cm s^-1
Temperature-dependence of saturation velocity.
91
wvth0=0.0 Vμm
Threshold voltage shift.
92
muesr1=2.0E15 cm2V^-1s^-1
Surface-roughness scattering.
93
muesr0=2.0 -
Surface-roughness scattering.
94
muesrl=0.0 −
L-dependence of surface roughness on mobility.
95
muesrw=0.0 −
Surface roughness-related mobility change.
96
mueswp=1.0 -
Surface roughness-related mobility change.
97
mueslp=1.0 -
L-dependence of surface roughness on mobility.
98
muetmp=1.5 −
Temperature-dependence of phonon scattering.
99
bb=2.0 -
High-field-mobility degradation.
100
ddltmax=10.0 -
Smoothing coefficient for Vds.
101
ddltslp=10.0 μm^-1
Lgate-dependence of smoothing coefficient.
102
ddltict=0.0 -
Lgate-dependence of smoothing coefficient.
103
sub1=0.01 V^-1
Substrate current coefficient of magnitude.
104
sub2=20.0 V
Substrate current coefficient of exponential term.
105
sub1l=2.5E-3 m
Lgate-dependence of SUB1.
106
sub1lp=1.0 -
Lgate-dependence SUB1.
107
sub2l=2.0E-6 m
Lgate-dependence of SUB2.
108
svds=3.0 -
Substrate current dependence on Vds.
109
slg=3.0E-8 m
Substrate current dependence on Lgate.
110
svbs=0.5 -
Substrate current dependence on Vbs.
111
svbsl=0.0 -
Lgate-dependence of SVBS.
112
svbslp=1.0 -
Lgate-dependence of SVBS.
113
svgs=0.8 -
Substrate current dependence on Vgs.
114
svgsl=0.0 -
Lgate-dependence of SVGS.
115
svgslp=1.0 -
Lgate-dependence of SVGS.
116
svgsw=0.0 -
Wgate-dependence of SVGS.
117
svgswp=1.0 -
Wgate-dependence of SVGS.
118
slgl=0.0
Substrate current dependence on Lgate.
119
slglp=1.0
Substrate current dependence on Lgate .
120
vfbsub=(-1.0) V
Flatband voltage for Isub calculation.
121
vfbsubl=0.0 −
Lgate-dependence of VFBSUB.
122
vfbsublp=1.0 -
Lgate-dependence of VFBSUB.
123
subdlt=2.0E-3 -
Smoothing parameter (hisimsoi_fb only).
124
hist1=10E-9 V
History-effect parameter.
125
hist2=1E-20 A
History-effect parameter.
126
qhe1=1.5 -
FBE parameter.
127
qhe2=0.35 V
FBE parameter.
128
evb1=0.0 V-2s^-1
Electron tunneling from valence band.
129
evb2=0.0 V m^-1
Electron tunneling from valence band.
130
evb3=0.0 -
Electron tunneling from valence band.
131
fvbs=0.0 -
Vbs dependence of Fowler-Nordheim current.
132
ibpc1=0.0 Ω
impact-ionization-induced bulk potential change.
133
ibpc2=0.0 V^-1
impact-ionization-induced bulk potential change.
134
nsti=5.0E17 cm-3
Substrate impurity concentration at STI edge.
135
wsti=0.0 m
Width of high-field region at STI edge.
136
wstil=0.0 −
Channel-length dependence of WSTI.
137
wstilp=1.0 -
Channel-length dependence of WSTI.
138
wstiw=0.0 −
Channel-width dependence of WSTI.
139
wstiwp=1.0 -
Channel-width dependence of WSTI.
140
scsti1=0.0 -
The same effect as SC1 but at STI edge.
141
scsti2=0.0 V^-1
The same effect as SC2 but at STI edge.
142
vthsti=0.0 V
Threshold voltage shift due to STI.
143
vdsti=0.0 -
Vds dependence of STI subthreshold.
144
muesti1=0.0 m
Mobility change due to diffusion length.
145
muesti2=0.0 -
Mobility change due to diffusion length.
146
muesti3=1.0 -
Mobility change due to diffusion length.
147
nsubpsti1=0.0 m
Pocket concentration modifier.
148
nsubpsti2=0.0 -
Pocket concentration modifier.
149
nsubpsti3=1.0 -
Pocket concentration modifier.
150
nsubcsti1=0.0 m
Channel concentration modifier.
151
nsubcsti2=0.0 -
Channel concentration modifier.
152
nsubcsti3=1.0 -
Channel concentration modifier.
153
tpoly=0.0 m
Height of poly-Si gate for fringing cap.
154
cgbo=0.0 F m^-1
Gate-to-B overlap cap.
155
cgdo=0.0 F m^-1
Gate-to-drain overlap cap.
156
cgso=0.0 F m^-1
Gate-to-source overlap cap.
157
ovslp=2.1E-7 mV^-1
Coefficient for overlap capacitance.
158
ovmag=0.6E0 V
Coefficient for overlap capacitance.
159
js0=1.0E-4 A m-2
Saturation current density.
160
nj=1.0 -
Emission coefficient.
161
xti=2.0 -
Temp coefficient for forward current densities.
162
xti2=0.0 -
Temp coefficient for reverse current densities.
163
vdiffj=1.6E-3 V
Diode threshold voltage at junction.
164
divx=0.0 V^-1
Reverse current coefficient.
165
cj=5.0E-04 F m-2
Bottom junc cap/unit area at zero bias.
166
cjsw=5.0E-10 F m^-1
Sidewall junc cap grading coefficient.
167
cjswg=5.0E-10 F m^-1
Sidewall junc cap per unit length at zero bias.
168
mj=0.33 -
Bottom junc cap grading coefficient.
169
mjsw=0.33 -
Sidewall junc cap grading coefficient.
170
mjswg=0.33 -
Gate sidewall junc cap grading coefficient.
171
pb=1.0 V
Bottom junc built-in potential.
172
pbsw=1.0 V
Sidewall junc built-in potential.
173
pbswg=1.0 V
Gate sidewall junc built-in potential.
174
lover=30E-9 m
Overlap length.
175
clm1=700.0E-3 -
Hardness coefficient of channel/contact junction.
176
clm2=2.0 -
Coefficient for QB contribution.
177
clm3=1.0 -
Coefficient for QI contribution.
178
clm5=1.0 -
CLM parameter.
179
clm6=0.0 −
CLM parameter.
180
vover=10.0E-3 -
Velocity overshoot effect parameter.
181
voverp=100.0E-3 -
Leff-dependence of velocity overshoot.
181
vovers=0.0 -
Modification of max velocity due to small size.
183
voversp=1.0 -
Modification of max velocity due to small size.
184
wfc=0.0 F cm-2 m^-1
Threshold voltage change due to cap change.
185
nsubcw=0.0 −
Substrate concentration modifier.
186
nsubcwp=1.0 -
Substrate concentration modifier.
187
nsubcmax=5E18 cm-3
Upper limit of substrate concentration.
188
nsubcl=0.0 -
Lgate-dependence of substrate concentration .
189
nsubclp=1.0 -
Lgate-dependence of substrate concentration .
190
qme1=0.0 mV
Vgs-dependence of quantum mechanical effect.
191
qme2=0.0 V
Vgs-dependence of quantum mechanical effect.
192
qme3=0.0 m
Minimum Tox modification.
193
gidl1=5.0E-6 A V-3/2C^-1m
Magnitude of GIDL.
194
gidl2=1.0E6 V-2m^-1F-3/2
field-dependence of GIDL.
195
gidl3=300.0E-3 -
Vds-dependence of GIDL.
196
gidl4=0.0 V
Threshold for Vds dependence.
197
gidl5=0.2E0 -
High-field correction.
198
gidlvb=0.5 V3
Vb-dependence of GIDL.
199
gleak1=10.0E3 V-3/2 s^-1
Gate-to-channel current coefficient.
200
gleak2=20.0E6 V^-1/2 m^-1
Gate-to-channel current coefficient.
201
gleak3=300.0E-3 -
Gate-to-channel current coefficient.
202
gleak4=4E0 m^-1
Gate-to-channel current coefficient.
203
gleak5=7.5E3 V m^-1
G-t-C short channel correction.
204
gleak6=250E-3 V
G-t-C Vds-dependence correction.
205
gleak7=1E-6 m2
G-t-C L and W dependence correction.
206
glksd1=1.0E-15 A m V-2
G-t-S/D current coefficient.
207
glksd2=5E6 V^-1 m^-1
G-t-S/D current coefficient.
208
glksd3=(-5E6) m^-1
G-t-S/D current coefficient.
209
glkb1=5E-16 A V-2
G-t-S/D current coefficient.
210
glkb2=1E0 m V^-1
G-t-S/D current coefficient.
211
glkb3=0E0 V
G-t-S/D current coefficient.
212
vzadd0=10.0E-3 V
Symmetry conservation coefficient.
213
pzadd0=5.0E-3 V
Symmetry conservation coefficient.
214
nftrp=10E9 V^-1
Ratio of trap density to attenuation coefficient.
215
nfalp=1.0E-19 cm s
Contribution of mobility fluctuation.
216
cit=0.0 F cm-2
Cap caused by the interface trapped carriers.
217
falph=1.0 sm3
Power of f describing deviation of 1/f.
218
tnom=27.0 C
Temperature selected as a nominal value.
219
dly1=100.0E-12 s
Coefficient for delay due to diffusion of carriers.
220
dly2=0.7E0 -
Coefficient for delay due to conduction of carriers.
221
dly3=0.8E-6 Ω
Coefficient for RC delay of bulk carriers.
222
tfox=3.5E-9 m
Front oxide thickness.
223
tsoi=5.0E-8 m
Silicon film thickness.
224
xj=5.0E-8 m
Impurity doping depth.
225
tbox=1.1E-7 m
Buried oxide thickness.
226
nsubs=3.0E+17 cm-3
SOI layer impurity concentration.
227
nsubb=4.0E+14 cm-3
Substrate impurity concentration.
228
rth0=0.1 Kcm/W
Thermal resistance.
229
cth0=1.0E-7 Ws/(Kcm)
Thermal capacitance.
230
sc4=0.0 -
SCE parameter.
231
ptl=0.0 V^(1-PTP)
Punchthrough parameter.
232
ptp=3.5 -
Punchthrough parameter.
233
pt2=0.0 V^-1
Punchthrough parameter.
234
ptlp=1.0 -
Punchthrough parameter.
235
gdl=0.0 -
Strength of high-field effect.
236
gdlp=0.0 -
Modification of channel conductance.
237
gdld=0.0 m
Modification of channel conductance.
238
pt4=0.0 V^-1
Punchthrough parameter.
239
pt4p=1.0 -
Punchthrough parameter.
240
vgsmin=(-5.0) V
Surface potential limiter.
241
rmin=1E-3 ohm
Minimum resistance.
242
mueph1=25.0E3 cm2V^-1s^-1
Phonon scattering.
243
ldrift=1.0E-6 m
Parameter for drift region length (drain) .
244
ldrifts=1.0E-6 m
Parameter for drift region length (source) .
245
cors=0 -
Source side resistance OFF(0)/ON(1).
246
cord=0 -
Drain side resistance OFF(0)/ON(1).
247
corbulk=0 -
Bulk resistance OFF(0)/ON(1).
248
corbnet=0 -
Activate body resistance net (1) or not (0).
249
rsh=0.0 ohm
Drain diffusion sheet resistance .
250
novers=1E19 cm-3
impurity concentration in overlap region.
251
rdrmued=1.0E3
Mobility in drift region (drain).
252
rdrmues=1.0E3
Mobility in drift region (source).
253
rdrvmaxd=3.0E7
Saturation velocity in drift region (drain).
254
rdrvmax=3.0E7 cm/s
Saturation velocity in drift region (drain).
255
rdrvmaxs=3.0E7
Saturation velocity in drift region (source).
256
rdrmuetmp=0.0 -i
Temperature dependence of resistance.
257
rdrvtmp=0.0 -
Temperature dependence of resistance.
258
rdrdjunc=1.0E-6
Junction depth at channel/drift region.
259
rdrbbd=1
Degradation of the mobility in drift region (drain).
260
rdrbbs=1 -
degradation of the mobility in drift region (source).
261
rdrbbtmp=0 -
Temperature coefficient of RDRBB.
262
rdrvmaxw=0.0 -
Wgate dependence of the saturation velocity in drift region.
263
rdrvmaxwp=1.0 -
Wgate dependence of the saturation velocity in drift region.
264
rdrvmaxl=0.0 -
Lgate dependence of the saturation velocity in drift region.
265
rdrvmaxlp=1.0 -
Lgate dependence of the saturation velocity in drift region.
266
rdrmuel=0.0 -
Lgate dependence of the mobility in drift region.
267
rdrmuelp=1.0 -i
Lgate dependence of the mobility in drift region.
268
rbdb=50.0 Ω
Substrate resistance network.
269
rbsb=50.0 Ω
Substrate resistance network.
270
copt=0 -
flag punchthrough.
271
copspt=0 -
flag Ps0 method for deep punchthrough.
272
xjpt=5.0E-8 m
Junction depth for deep punchthrough.
273
njunc=1e20 cm-3
Junction doping conc; deep punchthrough.
274
mupt=0.0 m2/V/s
Mobility for deep punchthrough.
275
vfbpt=0.0 V
dVfb for deep punchthrough.
276
pslimpt=0.0 V
Ps0 limit for deep punchthrough.
277
rbulk0=0.0 Ω
Offset of bulk resistance.
278
rbulkw=0.0 Ω/m
Bulk resistance per width.
279
vfbbtp=0.12 V
Flatband voltage for overlapped MOSFET part.
280
cbtbn=0.0 F/m2
N^+ poly capacitance.
281
cbtbp=0.0 F/m2
P^+ poly capacitance.
282
xwdbt=0.0 m
BT overlap width.

Output Parameters

Refer to the following table for Output Parameter details:

1

meff

Effective multiplicity factor (m-factor).

Operating-Point Parameters

Refer to the following table for Operating-Point Parameter details:

1
rdd (Ω)
Drift Resistance on Drain side.
2
rsd (Ω)
Drift Resistance on Source side.
3
rbulk (Ω)
Body Contact Resistance.
4
idse (A)
Drain-Source current.
5
isuba (A)
Substrate current.
6
igidle (A)
Gate-Induced Drain Leakage current.
7
igisle (A)
Gate-Induced Source Leakage current.
8
igde (A)
Gate-Drain current.
9
igse (A)
Gate-Source current.
10
igbe (A)
Gate-Substrate current.
11
ggm (S)
Transconductance.
12
ggds (S)
Channel conductance.
13
ggmbs (S)
Body effect (Back gate) transconductance.
14
ggmt (S)
Temperature transconductance.
15
deltemp (S)
Temperature.
16
vone (V)
Threshold voltage.
17
vdsate (V)
Saturation voltage.
18
qge (C)
Gate charge.
19
qde (C)
Drain charge.
20
qse (C)
Bulk charge.
21
cggbd (F)
g-g MOSFET capacitance.
22
cgdbd (F)
g-d MOSFET capacitance.
23
cgsbd (F)
g-s MOSFET capacitance.
24
cbgbd (F)
b-g MOSFET capacitance.
25
cbsbd (F)
b-s MOSFET capacitance.
26
cbdbd (F)
b-d MOSFET capacitance.
27
cdgbd (F)
d-g MOSFET capacitance.
28
cddbd (F)
d-d MOSFET capacitance.
29
cdsbd (F)
d-s MOSFET capacitance.
30
ibdb (A)
b-d Diode current.
31
ibsb (A)
b-s Diode current.
32
gbd (S)
b-d Diode conductance.
33
gbs (S)
b-s Diode conductance.
34
capbdb (F)
b-d Diode capacitance.
35
capbsb (F)
b-s Diode capacitance.


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