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Fundamentals of Microelectronics

CH1 Why Microelectronics? CH2 Basic Physics of Semiconductors CH3 Diode Circuits CH4 Physics of Bipolar Transistors CH5 Bipolar Amplifiers CH6 Physics of MOS Transistors CH7 CMOS Amplifiers CH8 Operational Amplifier As A Black Box

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Chapter 7 CMOS Amplifiers

7.1 General Considerations

7.2 Common-Source Stage

7.3 Common-Gate Stage

7.4 Source Follower

7.5 Summary and Additional Examples

CH7 CMOS Amplifiers 3

Chapter Outline

CH7 CMOS Amplifiers 4

MOS Biasing

Voltage at X is determined by VDD, R1, and R2. VGS can be found using the equation above, and ID can be

found by using the NMOS current equation.

( )

Soxn

THDD

THGS

RL

WCV

VRR

VRVVVVV

µ

1

2

1

21

21

211

=

−

+++−−=

CH7 CMOS Amplifiers 5

Self-Biased MOS Stage

The circuit above is analyzed by noting M1 is in saturation and no potential drop appears across RG.

DDDSGSDD VIRVRI =++

CH7 CMOS Amplifiers 6

Current Sources

When in saturation region, a MOSFET behaves as a current source.

NMOS draws current from a point to ground (sinks current), whereas PMOS draws current from VDD to a point (sources current).

CH7 CMOS Amplifiers 7

Common-Source Stage

DDoxnv

Dmv

RIL

WCA

RgA

µ

λ

2

0

−=

−==

CH7 CMOS Amplifiers 8

Operation in Saturation

In order to maintain operation in saturation, Vout cannot fall below Vin by more than one threshold voltage.

The condition above ensures operation in saturation.

( )THGSDDDD VVVIR −−<

9

CS Stage with λ=0

Lout

in

Lmv

RRR

RgA

=∞=−=

CH7 CMOS Amplifiers 10

CS Stage with λ ≠ 0

However, Early effect and channel length modulation affect CE and CS stages in a similar manner.

( )

OLout

in

OLmv

rRRR

rRgA

||

||

=∞=−=

CH7 CMOS Amplifiers 11

CS Gain Variation with Channel Length

Since λ is inversely proportional to L, the voltage gain actually becomes proportional to the square root of L.

D

oxn

D

oxn

v IWLC

IL

WCA µ

λ

µ 22∝=

CH7 CMOS Amplifiers 12

CS Stage with Current-Source Load

To alleviate the headroom problem, an active current-source load is used.

This is advantageous because a current-source has a high output resistance and can tolerate a small voltage drop across it.

( )21

211

||||

OOout

OOmv

rrRrrgA

=−=

CH7 CMOS Amplifiers 13

PMOS CS Stage with NMOS as Load

Similarly, with PMOS as input stage and NMOS as the load, the voltage gain is the same as before.

)||( 212 OOmv rrgA −=

CH7 CMOS Amplifiers 14

CS Stage with Diode-Connected Load

Lower gain, but less dependent on process parameters.

( )( )

−=

−=⋅−=

122

1

2

1

21

||||1

//1

OOm

mv

mmv

rrg

gA

LWLW

ggA

15

CS Stage with Diode-Connected PMOS Device

Note that PMOS circuit symbol is usually drawn with the source on top of the drain.

−= 21

12 ||||1

oom

mv rrg

gA

CH7 CMOS Amplifiers 16

CS Stage with Degeneration

Similar to bipolar counterpart, when a CS stage is degenerated, its gain, I/O impedances, and linearity change.

0

1

=

+−=

λ

Sm

Dv

Rg

RA

CH7 CMOS Amplifiers 17

Example of CS Stage with Degeneration

A diode-connected device degenerates a CS stage.

21

11mm

Dv

gg

RA+

−=

CH7 CMOS Amplifiers 18

CS Stage with Gate Resistance

Since at low frequencies, the gate conducts no current, gate resistance does not affect the gain or I/O impedances.

0=GRV

CH7 CMOS Amplifiers 19

Output Impedance of CS Stage with Degeneration

Similar to the bipolar counterpart, degeneration boosts output impedance.

OSOmout rRrgr +≈

CH7 CMOS Amplifiers 20

Output Impedance Example (I)

When 1/gm is parallel with rO2, we often just consider 1/gm.

2211

111mm

mOout gggrR +

+=

CH7 CMOS Amplifiers 21

Output Impedance Example (II)

In this example, the impedance that degenerates the CS stage is rO, instead of 1/gm in the previous example.

1211 OOOmout rrrgR +≈

CH7 CMOS Amplifiers 22

CS Core with Biasing

Degeneration is used to stabilize bias point, and a bypass capacitor can be used to obtain a larger small-signal voltage gain at the frequency of interest.

DmG

v

Sm

D

Gv Rg

RRRRRA

Rg

RRRR

RRA21

21

21

21

||||,1||

||+

−=+

−⋅

+=

CH7 CMOS Amplifiers 23

Common-Gate Stage

Common-gate stage is similar to common-base stage: a rise in input causes a rise in output. So the gain is positive.

Dmv RgA =

CH7 CMOS Amplifiers 24

Signal Levels in CG Stage

In order to maintain M1 in saturation, the signal swing at Vout cannot fall below Vb-VTH.

CH7 CMOS Amplifiers 25

I/O Impedances of CG Stage

The input and output impedances of CG stage are similar to those of CB stage.

Dout RR =m

in gR 1

= 0=λ

CH7 CMOS Amplifiers 26

CG Stage with Source Resistance

When a source resistance is present, the voltage gain is equal to that of a CS stage with degeneration, only positive.

Sm

Dv

Rg

RA+

= 1

CH7 CMOS Amplifiers 27

Generalized CG Behavior

When a gate resistance is present it does not affect the gain and I/O impedances since there is no potential drop across it ( at low frequencies).

The output impedance of a CG stage with source resistance is identical to that of CS stage with degeneration.

( ) OSOmout rRrgR ++= 1

CH7 CMOS Amplifiers 28

Example of CG Stage

Diode-connected M2 acts as a resistor to provide the bias current.

DOSm

Omout RrRg

rgR ||||11

211

+

≈( ) Smm

Dm

in

out

RggRg

vv

21

1

1 ++=

CH7 CMOS Amplifiers 29

CG Stage with Biasing

R1 and R2 provide gate bias voltage, and R3 provides a path for DC bias current of M1 to flow to ground.

( )( ) Dm

Sm

m

in

out RgRgR

gRvv

⋅+

=/1||

/1||3

3

CH7 CMOS Amplifiers 30

Source Follower Stage

1<vA

CH7 CMOS Amplifiers 31

Source Follower Core

Similar to the emitter follower, the source follower can be analyzed as a resistor divider.

LOm

LO

in

out

Rrg

Rrvv

||1||

+=

CH7 CMOS Amplifiers 32

Source Follower Example

In this example, M2 acts as a current source.

211

21

||1||

OOm

OOv

rrg

rrA+

=

CH7 CMOS Amplifiers 33

Output Resistance of Source Follower

The output impedance of a source follower is relatively low, whereas the input impedance is infinite ( at low frequencies); thus, a good candidate as a buffer.

Lm

LOm

out Rg

Rrg

R ||1||||1≈=

CH7 CMOS Amplifiers 34

Source Follower with Biasing

RG sets the gate voltage to VDD, whereas RS sets the drain current.

The quadratic equation above can be solved for ID.

( )2

21

THSDDDoxnD VRIVL

WCI −−= µ

CH7 CMOS Amplifiers 35

Supply-Independent Biasing

If Rs is replaced by a current source, drain current IDbecomes independent of supply voltage.

CH7 CMOS Amplifiers 36

Example of a CS Stage (I)

M1 acts as the input device and M2, M3 as the load.

3213

3213

1

||||||1

||||||1

OOOm

out

OOOm

mv

rrrg

R

rrrg

gA

=

−=

CH7 CMOS Amplifiers 37

Example of a CS Stage (II)

M1 acts as the input device, M3 as the source resistance, and M2 as the load.

331

2

||11O

mm

Ov

rgg

rA+

−=

CH7 CMOS Amplifiers 38

Examples of CS and CG Stages

With the input connected to different locations, the two circuits, although identical in other aspects, behave differently.

Sm

OCGv

Rg

rA+

= 12

_[ ] 11112_ ||)1( OOSOmmCSv rrRrggA ++−=

CH7 CMOS Amplifiers 39

By replacing the left side with a Thevenin equivalent, and recognizing the right side is actually a CG stage, the voltage gain can be easily obtained.

Example of a Composite Stage (I)

21

11mm

Dv

gg

RA+

=

CH7 CMOS Amplifiers 40

Example of a Composite Stage (II)

This example shows that by probing different places in a circuit, different types of output can be obtained.

Vout1 is a result of M1 acting as a source follower whereas Vout2 is a result of M1 acting as a CS stage with degeneration.

12

2

4332

1||1

||||1

mO

m

OOm

in

out

gr

g

rrg

vv

+−=