3.single stage amp i

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EE6326 Ana log IC Design Fal l 2007 Topic 3. Single-stage Amplifiers - CS J. Liu Associate Professor UT Dallas

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8/4/2019 3.Single Stage Amp I

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EE6326 Analog IC Design – Fall 2007

Topic 3. Single-stage Amplifiers

- CS

J. Liu

Associate Professor

UT Dallas

8/4/2019 3.Single Stage Amp I

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Page 2

Single Stage Amplifier

Common source (inverting) amplifiers

Source follower (common drain)

Common gate stage

Cascode stage*

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Page 3

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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Page 4

Common Source Amplifiers

AKA

Inverters

Inverting Amplifiers

ConfigurationsResistive load

Diode connected load

Current source loadTriode load

Source degeneration

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Page 5

Inverting Amplifier with Resistive Load

G

D

S

VDD

R D

VinVout

Vin iDiD

Voltage across R D

Vout

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Page 6

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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Page 7

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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Page 8

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

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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Page 9

Inverting Amplifier with Resistive Load- Large Signal Transfer Function

G

D

S

VDD

R D

Vin

Vout

iD

M1

 DT oxn

V VinVout 

 RV Vin L

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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Page 10

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

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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Page 11

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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Page 12

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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Page 13

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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Page 14

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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Page 15

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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Page 16

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 

−=−=

=

∞=

)/1||(

)/1(||

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Page 17

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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Page 18

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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Page 19

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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l f h d d

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Page 21

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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Page 22

Inverting Amplifier with Diode-connectedLoad - Large Signal Transfer Function

G1

D1

S1

VDD

VoutiD

M1

S2

D2

M2

G2

 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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Page 23

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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Page 24

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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Page 25

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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Page 26

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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Page 27

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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Page 28

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 

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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Page 29

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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Page 30

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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Page 31

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 

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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Page 32

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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Page 33

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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Page 34

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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Page 35

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 

1

21

1

21

1

−=

+

−=

+=

∞≈

Inverting Amplifier with Current Source

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Page 36

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.

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Page 37

HW #3

Due on 9/11

More exercise if desired (in Razavi book)

3.1, 3.2, 3.3, 3.4

3.15 (a) (c) (d)

3.16 (a) (b) (c)

3.21 (a) (b) (c)