Chapter 3 Four-port RF MOSFET Modeling for Simulation with DBB ( UN65 CMOS
3.3 Four-port RF MOSFET Small Signal Equivalent Circuit Development and
3.3.2 Small Signal Equivalent Circuit in Linear Region
In this section, small signal equivalent circuit will be derived for 4-port RF MOSFET in linear region. Note that the bias condition for linear region has to follow the criterion of |Vgs| >
|VT| and |Vds|<< |Vgs -VT| to ensure strong inversion of the channel and linear velocity vs. field under sufficiently low Vds. In this study for UN65 nMOS with Vdd=1.0V, the bias condition is specified as Vgs=Vdd =1.0V and Vds=0 for linear region. Considering the channel conduction driven by inversion carriers, the channel resistance between source and drain is represented by Rch in the device cross section and equivalent circuit as shown in Fig. 3.42 and Fig. 3.43, respectively. Then Rch appears as one additional model parameter compared with those required for off state shown in Fig. 3.27and Fig. 3.28. According to a simple equivalent circuit analysis on Fig. 3.43, Rch can be extracted from 1/Re(Y32) at very low frequency when all of the capacitors become open circuit, given by (3.47)~(3.48).
At very low frequency,
2 2
2
32 1
( )
1
Re( ) | ( )
s d
ch d s
ch d s
L L
R R R
Y R R R
(3.47)
2(Ls Ld)2 1
32 1 32 1
1 1
( )
Re( ) | Rch Rd Rs Rch Re( ) | Rd Rs
Y Y
(3.48)
The body network model previously derived for 4-port RF MOSFET at off state can be applied to linear region with an appropriate modification on Cgb2, due to formation of inversion channel.
Besides necessary change to Cgb2, Fig. 3.44 reveals significant increase of Cgs and Cgd caused by the raising Vgs to well above VT (Vgs =1.0V >>VT ) as compared to those at off state (Vgs=0) shown in Fig. 3.29.
Table 3.5 summarizes the small signal equivalent circuit model parameters for 4-port RF MOSFET in linear region. It appears that the increase of Vgs to strong inversion region leads to increase of Cgs and Cgd whereas decrease of Cgb2, due to shielding effect from inversion carriers.
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Cgs is larger than Cgd by around 5.7% and it can be explained by the difference of finger numbers for source and drain contact in the multi-finger MOSFET with even finger number (NF=evern : NF/2+1 for source contacts and NF/2 for drain contacts). The channel resistance Rch
is determined by (3.48) to be around 7.3 .
Source Gate Drain Body
Cgs
Rbb
STI STI
DNW
P-well
Deep N-Well Cdnw1
P-substrate
STI
P-sub
Cgd
P-sub DNW
Cjs Cjd
Rdnw
Cdnw2
Rbb2
Rbb3
Cgb2 Rgb
Rch
Fig. 3.42 4-port MOSFET device cross section and the representation of RC elements for the small signal equivalent circuit in linear region, Vgs=1.0V, Vds=Vbs =0
S (2)
D (3)
Rbb Body
(4)
Cjs Cgb2 Cgd
Cgs
G
(1) Lg Rg
Ls Rs Rd Ld
Cjd
Rgb
Cgb1
Cdnw1 Cg
Rdnw Rbb2 Cdnw2
Rbb3
P-sub
Cds
Rch
Fig. 3.43 Small signal equivalent circuit with new body network model for 4-port RF MOSFET in linear region, Vgs=1.0V, Vds= Vbs=0. Rch represents channel resistance of the inversion channel.
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0 5 10 15 20 25 30 35 40 20
40 60 80 100 120
-Im(Y12)/ Im(Y11)/ Im(Y
11)/=C
gg
-Im(Y
12)/=C
gs
-Im(Y13)/=C
gd
Im(Y 11)/, -Im(Y 12)/, -Im(Y 13)/(fF)
-Im(Y13)/ Freq (GHz)
Vgs=1V, Vds=Vbs=0
Fig. 3.44 Im(Y11)/, -Im(Y12)/, and -Im(Y13)/ vs. frequency measured from 4-port RF MOSFET under the biases in linear region Vgs=1.0V, Vds=Vbs=0. Cgg, Cgs, and Cgd determined from Im(Y11)/, -Im(Y12)/, and -Im(Y13)/ at very low frequency
Table 3.5 Small signal equivalent circuit model parameters of 4-port MOSFET in linear region (Vgs=1.0V, Vds= Vbs=0)
According to the model parameters shown in table 3.5 for 4-port MOSFETs in linear region, S- and Y-parameters are simulated. Fig. 3.45 ~ Fig. 3.52 present the 4-port S-parameters from measurement and simulation for this 4-port MOSFET (W2N32) in linear region under Vgs=1.0V and Vds=Vbs=0. Note that the simulation by using the small signal equivalent circuit shown in Fig. 3.43 and model parameters in Table 3.5 was compared with
4-port MOSFET model parameters in linear region
Capacitances (fF) Resistances Ω Inductances pH
Cgs 31.18 Rg 7.2 Ls 70
Cgd 29.44 Rd 1 Ld 70
Cgb1 2 Rs 1 Lg 70
Cgb2 1.4 Rb 1 Lb 70
Cg 2.1 Rbb 958
Cds 3 Rbb2 664
Cjs 18.91 Rbb3 5484
Cjd 17.12 Rdnw 476
Cdnw1 18.91 Rgb 518500
Cdnw2 18.91 Rch 7.3
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those calculated by BSIM-4 default model. The results indicate that the small signal equivalent circuit can predict 4-port S-parameters with promisingly good accuracy whereas the simulation uding BSIM-4 default model reveals large deviation from the measurement, particularly for the components related to the body, i.e. port-4, e.g. Mag(S44), Mag(S41), Mag(S42), and Mag(S43) as shown in Fig. 3.45 and phase(S44), phase(S41), phase(S42), and phase(S43) as shown in Fig. 3.49. Besides S-parameters, Re(Y42), Re(Y43), and Re(Y33) are three more important parameters to verify the body network model. Fig. 3.49 indicates that the small signal equivalent circuit with new body network can improve simulation accuracy for Re(Y42) and Re(Y43) compared with those simulated by using default body network model.
Fig. 3.54 presents similar effect from body network model when applied to BSIM-4 for Re(Y42) and Re(Y43) simulation. Similar with the condition for off state, the impact from body network model on Re(Y33), i.e. the key parameter responsible for output resistance, is relatively smaller, as shown in Fig. 3.55. Again, the new body network model can be applied to both small signal equivalent circuit and BSIM-4 for an accurate simulation in linear region.
The verification by extensive data suggests that body network model is the key to determine simulation accuracy for 4-port RF MOSFETs and proves that the new body network proposed for linear region (Fig. 3.43) can fix the problem with BSIM-4 for 4-port MOSFET simulation.
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0.10 Small signal eq. ckt Cds=3fF
measured : circuit with new body network model. Dash lines : BSIM-4 with default body network model.
0 5 10 15 20 25 30 35 40 Small signal eq. ckt Cds=3fF
measured :
BSIM-4 default model (c) (d)
(b)
Fig. 3.46 The measured and simulated Mag(S) of 4-port MOSFET in linear region Vgs=1.0V, Vds=Vbs=0 (a) Mag(S11) (b) Mag(S12) (c) Mag(S13) (d) Mag(S14). Solid lines : small signal equivalent circuit with new body network model. Dash lines : BSIM-4 with default body network model
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Small signal eq. ckt Cds=3fF measured :
BSIM-4 default model (c) (d)
(a) (b) circuit with new body network model. Dash lines : BSIM-4 with default body network model
0 5 10 15 20 25 30 35 40 0.00
0.05 0.10 0.15
0.20 measured : Small signal eq. ckt Cds=3fF
simulation
Fig. 3.48 The measured and simulated Mag(S) of 4-port MOSFET in linear region Vgs=1.0V, Vds=Vbs=0 (a) Mag(S33) (b) Mag(S31) (c) Mag(S32) (d) Mag(S34). Solid lines : small signal equivalent circuit with new body network model. Dash lines : BSIM-4 with default body network model
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Small signal eq. ckt Cds=3fF
measured : Small signal eq. ckt Cds=3fF
measured :
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Small signal eq. ckt Cds=3fF
measured :
71 Default body network
Re(Y 42)(10-3 ) default body network
(b)
Freq (GHz)
Fig. 3.53 Measured and simulated Re(Y42) and Re(Y43) for 4-port MOSFET in linear region Vgs=1.0V, Vds=Vbs=0 (a) Re(Y42) (b) Re(Y43). Simulation by small signal equivalent circuit model. Solid lines : new body network model. Dash lines : default body network model
0 5 10 15 20 25 30 35 40 Default body network
Re(Y42)(10-3 ) default body network
(b)
Freq (GHz)
Fig. 3.54 Measured and simulated Re(Y42) and Re(Y43) for 4-port MOSFET in linear region Vgs=1.0V, Vds=Vbs=0 (a) Re(Y42) (b) Re(Y43). Simulation by BSIM-4, solid lines : with new body network model. Dash lines : with default body network model
0 5 10 15 20 25 30 35 40 default body network UN65 nMOS W2N32 default body network UN65 nMOS W2N32 VGS=1V, VDS=VBS=0
(b)
Freq (GHz)
Fig. 3.55 Measured and simulated Re(Y33) for 4-port MOSFET in linear region Vgs=1.0V, Vds=Vbs=0 (a) simulation by small signal equivalent circuit (b) simulation by BSIM-4. Solid
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lines : with new body network model. Dash lines : with default body network model