3.single stage amp i
TRANSCRIPT
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EE6326 Analog IC Design – Fall 2007
Topic 3. Single-stage Amplifiers
- CS
J. Liu
Associate Professor
UT Dallas
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Single Stage Amplifier
Common source (inverting) amplifiers
Source follower (common drain)
Common gate stage
Cascode stage*
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Characterization of Single Stage Amplifiers
Large signal transfer function
Large signal swing limitations Small signalGain
Input resistanceOutput resistanceFrequency response
OthersNoisePower dissipation
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Common Source Amplifiers
AKA
Inverters
Inverting Amplifiers
ConfigurationsResistive load
Diode connected load
Current source loadTriode load
Source degeneration
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Inverting Amplifier with Resistive Load
G
D
S
VDD
R D
VinVout
Vin iDiD
Voltage across R D
Vout
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Inverting Amplifier with Resistive Load- Large Signal Transfer Function
G
D
S
VDD
R D
VinVout
iD
Vin
VoutVDD
VT
If Vin <VT, M1 is in cutoff regioniD = 0, Vout=VDD
If Vin >VT, M1 is in either triode or
saturation region
M1
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Inverting Amplifier with Resistive Load- Large Signal Transfer Function
G
D
S
VDD
R D
VinVout
iD
VTM1
Criteria for Saturation of M1:VDS1>VGS1-VT
Vout>Vin- VT, area above line
Vout= Vin- VT
Vin
VoutVDD
VDD
Sat.
Triode
Cutoff
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Inverting Amplifier with Resistive Load- Large Signal Transfer Function
G
D
S
VDD
R D
Vin
Vout
iD
M1
In saturation region:
DT oxn
T oxn D
T GS oxn D
D D
RV Vin L
W
C VDDVout
V Vin L
W C i
V V L
W C i
Vout RiVDD
2
'
2
'
2
'
)(2
1
)(2
1
)(2
1
−−=
−=
−=
+=
µ
µ
µ
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Inverting Amplifier with Resistive Load- Large Signal Transfer Function
G
D
S
VDD
R D
Vin
Vout
iD
M1
T
DT oxn
V VinVout
RV Vin L
W
C VDDVout
−=
−−=
11
)1(2
1
1
2
'µ
Vin
VoutVDD
VDD
Sat.
Triode
Cutoff
Vin1
Vout1
When Vin >Vin1, M1 is in triode region
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Inverting Amplifier with Resistive Load- Large Signal Transfer Function
G
D
S
VDD
R D
VinVout
iD
M1
When Vin >Vin1, M1 is in triode region
DT oxn
T oxn D
DS DS T GS oxn D
D D
RVout Vout V Vin L
W C Vout VDD
Vout Vout V Vin L
W
C i
V V V V L
W C i
Vout RiVDD
]2
1)[(
]2
1
)[(
]2
1)[(
2
2
2
−−+=
−−=
−−=
+=
µ
µ
µ
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Inverting Amplifier with Resistive Load- Large Signal Transfer Function
G
D
S
VDD
R D
VinVout
iD
VTM1
Vin
VoutVDD
VDD
Sat.
Triode
Cutoff
Vout= Vin- VT
Input swing range:VT<Vin<Vin1 for saturation
Output swing range:
Vout1<Vout<VDD for sat.
Vin1
Vout1
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Inverting Amplifier with Resistive Load- Small Signal Characteristics
G
D
S
VDD
R D
VinVout
iD
M1
gmvgs gmbs
v bs
gds
G
S S
D
+
-
vgsR D
DC voltage supplies = gnd
DC current supplies = openvout
vin
D D
ds D
inmout
ds Dinmout
ds Dbsmbs gsmout
R g g g
v g
v
g Rv g v
g Rv g v g v
/1,
)/1||(
)/1||)((
=+
−
=
−=
+−=
v bs=0 vgs=vin
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Inverting Amplifier with Resistive Load- Gain
G
D
S
VDD
R D
Vin
Vout
iD
M1
gmvgs gmbsv bs
gds
G
S S
D
+
-
vgsR D
vout
vin
ds D
m
in
out
ds D
inm
out
g g
g
v
v
g g
v g v
+
−=
+
−=
Low frequency gain
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Inverting Amplifier with Resistive Load- Input Resistance
G
D
S
VDD
R D
Vin
Vout
iD
M1
gmvgs gmbsv bs
gds
G
S S
D
+
-
vgsR D
vout
vin
∞=inr Input resistance
v bs=0 vgs=vin
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Inverting Amplifier with Resistive Load- Output Resistance
G
D
S
VDD
R D
Vin
Vout
iD
M1
gmvgs gmbsv bs
gds
G
S S
D
+
-
vgsR D vtest
vin=0itest
vgs=0, vbs=0
D D
ds D
out
out
ds D
test
test out
R g
g g r
g
g R
i
vr
/1
1
)/1(||
=
+==
==
Output resistance
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Inverting Amplifier with Resistive Load- Small Signal Characteristics Summary
G
D
S
VDD
R D
Vin
Vout
iD
M1out mds Dm
in
out
ds Dout
in
r g g R g v
v g Rr
r
−=−=
=
∞=
)/1||(
)/1(||
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Inverting Amplifier with Diode-connectedLoad
G1
D1
S1
VDD
Vin
VoutiD
M1
S2
D2
M2
G2
When the gate and the drain of a
MOSFET (N or P) are connectedtogether (diode-connected), it is always
in saturation region.
Saturation criteria:
vDS
>vGS
-VTWhen vD=vG, the above
criteria is always satisfied.
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Inverting Amplifier with Diode-connectedLoad
Vin
Vin iD
vSG2
vout=VDD-vSG2
G1
D1
S1
VDD
VoutiD
M1
S2
D2
M2
G2
2
22 |)|(2
1T SGox p D V v
L
W C i −= µ
For M2,
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Inverting Amplifier with Diode-connectedLoad - Large Signal Transfer Function
Vin
VoutVDD
VT
If Vin <VT, M1 is in cutoff regioniD = 0, M2 is in cutoff region
Vout=VDD-|VTP2|
If Vin >VT, M1 is on, iD is not zero,M2 turns on in sat.
G1
D1
S1
VDD
VoutiD
M1
S2
D2
M2
G2
VDD-|VTP2|M2 off
M1 of f
M2 satM1 sat
M1 triode
vin
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Inverting Amplifier with Diode-connectedLoad - Large Signal Transfer Function
G1
D1
S1
VDD
VoutiD
M1
S2
D2
M2
G2
21
2
22
22
2
222
2
'1
2
11'1
|)|(2
1
|)|(2
1
)(
2
1
)(21
D D
T ox p D
SDSG
T SGox p D
T oxn D
T GS oxn D
ii
V Vout VDD L
W C i
Vout VDDvv
V v L
W C i
V Vin
L
W C i
V v LW C i
=
−−=
−==
−=
−=
−=
µ
µ
µ
µ
When M1 and M2 are in Sat.
l f h D d d
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Inverting Amplifier with Diode-connectedLoad - Large Signal Transfer Function
G1
D1
S1
VDD
VoutiD
M1
S2
D2
M2
G2
T
D D
T ox p
T oxn
V vinvout
ii
V vout VDD LW C
V vin L
W C
−=
=
−−=
−
11
|)|1(21
)1(2
1
21
22
2
'
µ
µ
To find out the boundary between
the sat. and triode regions of M1,
Solve for vin1 and vout1.
I i A lifi i h Di d d
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Inverting Amplifier with Diode-connectedLoad - Large Signal Transfer Function
G1
D1
S1
VDD
VoutiD
M1
S2
D2
M2
G2
2
2
2
|)|(2
1
]
2
1)[(
T ox p
T oxn D
V vout VDD L
W C
vout vout V vin
L
W C i
−−=
−−=
µ
µ
When vin>vin1, M1 is in triode region
And M2 is still in sat. region.
I i A lifi i h Di d d
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Inverting Amplifier with Diode-connectedLoad - Large Signal Transfer Function
Vin
VoutVDD
VTG1
D1
S1
VDD
VoutiD
M1
S2
D2
M2
G2VDD-|VTP2|
M2 off
M1 of f
M2 satM1 sat
M1 triode
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Plot transfer functions
Label X- and Y-axis
Label the operational regions of each device
Label the important transition points betweendifferent operational regions on both X- and Y-axis
Write the equation for each portion of the curve
S ll Si l E i l t f Di d C t d
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Small Signal Equivalent of a Diode ConnectedMOSFET
GD
S
gm gds
v1
v1
VDD
gm is approximately 100 times go (gds) gm
gmvgs gds
v1
vgs
I ti A lifi ith PMOS Di d
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Inverting Amplifier with PMOS Diode-Connected Load – Gain
2
1
2
1
2
1
221
1
1
1
m
m
in
out
in
m
m
m
inmout
dsmds
gsmout
g g
vv
v g
g
g v g v
g g g v g v
−≈
−=−≈
++
−=
G1
D1
S1
VDD
VoutiD
M1
S2
D2
M2
G2
vin
gm1vgs1 gmbs1v bs1
gds1
G
S S
D
+
-
vgs1 gm2+gds2
v bs1=v bs2=0v
gs1
=vinvgs2=vout
I ti A lifi ith PMOS Di d
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Inverting Amplifier with PMOS Diode-Connected Load – Rin, Rout, and Gain
out m
dsmds
m
in
out
mdsmds
out
in
r g
g g g
g
v
v
g g g g r
r
1
221
1
2221
11
−=
++
−=
≈++
=
∞=
G1
D1
S1
VDD
VoutiD
M1
S2
D2
M2
G2
vin
gm1vgs1 gmbs1v bs1
gds1
G
S S
D
+
-
vgsgm2+gds2
S ll Si l E i l t f Di d C t d
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Small Signal Equivalent of a Diode ConnectedMOSFET with Bulk Effect
G D
gm go
gmbs
S
gmVgs
Vgs=0-vx Vbs=0-vx
I ti A lifi ith NMOS Di d
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Inverting Amplifier with NMOS Diode-Connected Load – Gain
η
η
+
−≈
+
−=
+
−≈
+++
−=
11
1
11
1
2
1
2
1
22
1
2221
1
m
m
in
out
in
m
m
mbsm
inmout
dsmbsmds
gsmout
g g
vv
v g
g
g g v g v
g g g g v g v
gm1vgs1 gmbs1v bs1
gds1
G
S S
D
+
-
vgsgm2+gmbs2+gds2
In tin Amplifi ith NMOS Di d
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Inverting Amplifier with NMOS Diode-Connected Load – Rin, Rout, and Gain
out m
dsmbsmds
m
in
out
mdsmbsmds
out
in
r g
g g g g
g
v
v
g g g g g r
r
1
2221
1
22221 1
111
−=
+++
−=
+≈
+++=
∞≈
η
gm1vgs1 gmbs1v bs1
gds1
G
SS
D
+
-
vgsgm2+gmbs2+gds2
Inverting Amplifier with Current Source
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Inverting Amplifier with Current SourceLoad - Large Signal Transfer Function
Vin
Vout
VDD
VT
M2 triode
M
1 of f
M2 sat
M1 triode
G1
D1
S1
VDD
VoutiD
M1
S2
D2
M2
G2
vin
VB
M2 Sat.: VDD-Vout >VDD-VB-|VTP2|
Vout < VB+|VTP2|
Assume M2 is on, VDD-VB>|VTP2|
VB+|VTP2|
Vout>Vin-VTN1
M1 sat
Inverting Amplifier with Current Source
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Inverting Amplifier with Current SourceLoad
G1
D1
S1
VDD
VoutiD
M1
S2
D2
M2
G2
vin
VB
Consider the small signal characteristics of
M2:
gm2vgs2
gds2
G2=0
S2S2
D2
+
-
Vgs=0
Equivalent to gds2
Inverting Amplifier with Current Source
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Inverting Amplifier with Current SourceLoad - Gain
G1
D1
S1
VDD
VoutiD
M1
S2
D2
M2
G2
vin
VB
gm1vgs1 gmbs1v bs1
gds1
G
S S
D
+
-
vgsgds2
21
1
21
1
1
dsds
m
in
out
dsds
inmout
g g
g
v
v g g
v g v
+
−≈
+
−=
Inverting Amplifier with Current Source
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Inverting Amplifier with Current SourceLoad – Rin, Rout, and Gain
G1
D1
S1
VDD
VoutiD
M1
S2
D2
M2
G2
vin
VB
gm1vgs1 gmbs1v bs1
gds1
G
S S
D
+
-
vgsgds2
out m
dsds
m
in
out
dsds
out
in
r g
g g
g
v
v
g g r
r
1
21
1
21
1
−=
+
−=
+=
∞≈
Inverting Amplifier with Current Source
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Inverting Amplifier with Current SourceLoad vs. Triode Load
G1
D1
S1
VDD
VoutiD
M1
S2
D2
M2
G2
vin
VB
If M2 operates in the saturation region,
M2 is a current source.
Calculate gds2 in saturation region.
If VB is very low, (Large VSG2), M2
is mostly likely work in the triode region.
Calculate gds2 in triode region.