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Chapter 4 Differential Amplifiers

Chapter 4 Differential Amplifiers

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Page 1: Chapter 4 Differential Amplifiers

Chapter 4pDifferential Amplifiers

Page 2: Chapter 4 Differential Amplifiers

CMOS Differential Amplifiers

Basic Concepts-L15Basic Concepts L15

Page 3: Chapter 4 Differential Amplifiers

Single ended vs Differential SignalsSingle-ended vs. Differential Signals

Si l d d i l M d ith• Single-ended signal: Measured with respect to a fixed potential, typically groundground.

• Differential signal: Measured between two symmetric nodes (nodes have equal and y ( qopposite signal excursions around a fixed potential, called a “common-mode” level)

Page 4: Chapter 4 Differential Amplifiers

Why Differential?Why Differential?

• In a single amplifier VDD fluctuations appear directly on the amplified signalappear directly on the amplified signal.

• In a differential pair, if we measure VX-V h fl i lVY the fluctuations cancel out.

Page 5: Chapter 4 Differential Amplifiers

Why Differential?Why Differential?

• In a single CS amplifier, the maximum swing is VDD-(VGS-VTH)swing is VDD (VGS VTH)

• In a differential pair it can be shown h h i f V V hthat the swing of VX-VY can reach 2[VDD-(VGS-VTH)]. DD ( GS TH)

Page 6: Chapter 4 Differential Amplifiers

Clock Noise ReductionClock Noise Reduction

Page 7: Chapter 4 Differential Amplifiers

Other advantages of differential amplifying

• Simpler biasing• Higher linearityHigher linearity

Page 8: Chapter 4 Differential Amplifiers

Simple Symmetric Differential Pair won’t do!Simple Symmetric Differential Pair won t do!Good features: R j ti fRejection of VDD fluctuationsfluctuations, Larger swing.

Key problem: Input signal common-signal commonmode affects bias conditions, and differential amplification.

Page 9: Chapter 4 Differential Amplifiers

Solution: Source-coupled (“long-tailed”) Pair, biasing with a current source

If Vin1=Vin2 then ID1=ID2=ISS/2

Then V =V =V R I /2Then Vout1=Vout2=VDD-RDISS/2

Page 10: Chapter 4 Differential Amplifiers

“Current stealing “ phenomenonCurrent stealing phenomenon

If Vi 1>>Vi 2 then M2If Vin1>>Vin2, then M2 turns off and M1steals all the currentsteals all the current.

If Vin1<<Vin2 then M2k ll htakes all the current.

Page 11: Chapter 4 Differential Amplifiers

Common Mode ResponseCommon-Mode Response

Can Vin,CM be arbitrarily large or small?

Page 12: Chapter 4 Differential Amplifiers

Vin,CM must be large enough for M3 to be in ,C 3saturation

M1,M2 operate like Source Followers: VPincreases as Vin,CM increases – must be larger than Vb-VTH3

Page 13: Chapter 4 Differential Amplifiers

Vin,CM must not be too large to keep M1 and ,CM2 from entering Triode Mode

],2

min[)( 1,331 DDTHSS

DDDCMinTHGSGS VVIRVVVVV +−≤≤−+

Page 14: Chapter 4 Differential Amplifiers

Consequences of Vin,CM going “off ,Crange”

• As long as common mode voltage is within theAs long as common mode voltage is within the permitted range, differential gain is almost insensitive to itinsensitive to it.

• Once too small or too large – gain falls off.

Page 15: Chapter 4 Differential Amplifiers

Common-Mode Input vs. Output Swing Tradeoff

E h d i ltEach drain voltage can go as high as VDD and as low

V Vas Vin,CM-VTH.The larger Vin,CM the smaller th ithe swing.

Page 16: Chapter 4 Differential Amplifiers

Two types of Differential GainsTwo types of Differential Gains

“Single-gended”: Vout1(or Vout2)

VV

( out2)with respect to ground.

?)(21

21 =−−

=inin

outoutv VV

VVdiffAg

?.).(21

1 =−

=inin

outv VV

VESA21 inin

Page 17: Chapter 4 Differential Amplifiers

Current Division MechanismCurrent Division Mechanism

Calculate ID1 and ID2 in terms of Vin1 and V assuming the circuit is symmetric MVin2, assuming the circuit is symmetric, M1

and M2 are saturated, and λ=0.

Since the voltage at node P is equal to THD

GS VWIV +=

2Since the voltage at node P is equal to

VP=Vin1-VGS1=Vin2-VGS2,

V V V V

n LWk '

Vin1-Vin2=VGS1-VGS2

Page 18: Chapter 4 Differential Amplifiers

Current Division MechanismCurrent Division MechanismGiven the inputs andGiven the inputs and ISS: Solve two equations with twoequations with two unknowns for the transistor currents:transistor currents:

2121

22 DDinin W

IW

IVV −=−'' nn

IIILWk

LWk

21 DDSS III +=

Page 19: Chapter 4 Differential Amplifiers

CMOS Differential Amplifiers

Small-Signal Differential Gain-L16Small Signal Differential Gain L16

Page 20: Chapter 4 Differential Amplifiers

Current Difference PropertiesCurrent Difference PropertiesEven though each e t oug eaccurrent is an even function of its respective gate-source voltage, the current difference iscurrent difference is an odd function of the input voltage

2)(4)(1 SS VVIVVWCII = μ

p gdifference

212121 )()(2 inin

OXn

ininOXnDD VV

LWC

VVL

CII −−−=−μ

μ

Page 21: Chapter 4 Differential Amplifiers

Differential Transconductance Gain vs. Input Voltage

4I

)(2

/4 2

21 ininoxn

SS

oxnm

D

VVLWC

IWCGI

−−==

Δ μμ∂∂

)(42 221 inin

SSm

in VVWC

ILV−−

Δ

μ

oxn LCμ

Page 22: Chapter 4 Differential Amplifiers

Maximum Differential Transconductance Gain Occurs at ΔVin=0

IWCG ⎟⎞

⎜⎛= μ max, SSoxnm I

LCG ⎟

⎠⎜⎝

= μ

Page 23: Chapter 4 Differential Amplifiers

Differential Voltage GainDifferential Voltage Gain

inmDDDoutout VGRIRVV Δ=Δ=− 21

Page 24: Chapter 4 Differential Amplifiers

Differential Voltage Gain near ΔV = 0Differential Voltage Gain near ΔVin= 0

|| max, DSSoxnDmout

V RILWCRG

VVA μ==ΔΔ

= ,in LVΔ

Page 25: Chapter 4 Differential Amplifiers

Differential Transconductance Gain Falls to Zero at ΔVin= ΔVin1

21 W

IV SSin =Δ

LWCoxnμ

Page 26: Chapter 4 Differential Amplifiers

Current Difference PropertiesCurrent Difference PropertiesIt appears as if ΔID also t appea s as D a sobecomes zero at ΔVin2=(4ISS/(µnCOXW/L))1/2

But this is incorrect.

ΔV > ΔV at which a totalΔVin2> ΔVin1 at which a total current stealing occurs.

2)(4)(1 SS VVIVVWCII = μ 212121 )()(2 inin

OXn

ininOXnDD VV

LWC

VVL

CII −−−=−μ

μ

Page 27: Chapter 4 Differential Amplifiers

ΔVin= ΔVin1 is the maximum differential input that the amplifier can “handle”

21 W

IV SSin =Δ

LWCoxnμ

Page 28: Chapter 4 Differential Amplifiers

Also note that at ΔVin=0 each transistor carries a current of ISS/2 and therefore :

I )( 2,1

LWC

IVVoxn

SSTHGS

μ=−

L

Compare this equilibrium )( 121

inTHGS

VVV Δ=−

overdrive to the maximum differential input permitted:

2

)( 2,1THGS VV

2IV SS=Δ 1

LWC

Voxn

in

μ=Δ

Page 29: Chapter 4 Differential Amplifiers

It means that if we try to increase ΔVin1, for a given ISS, we need larger overdrive voltage in each transistor, and this is accomplished by reducing W/L

)( 2,1 WC

IVV SSTHGS =−

)( 121

inTHGS

VVV Δ=−

LCoxnμ

2

)( 2,1THGS VV

2IV SS=Δ 1

LWC

Voxn

in

μ=Δ

Page 30: Chapter 4 Differential Amplifiers

Small-Signal Differential Voltage Gain

• For |ΔVi |≈0 (sufficiently small) we have:For |ΔVin| 0 (sufficiently small) we have:

|| out RRIWCRGVA Δ || max, DmDSSoxnDmin

outV RgRI

LCRG

VA ===

Δ= μ

Where g is that of a NMOS with a current ofWhere gm is that of a NMOS with a current of ISS/2

Page 31: Chapter 4 Differential Amplifiers

Differential Gain: What does each input “see”?

• By superposition let’s short Vin2 to ground and see the effect of Vi 1see the effect of Vin1:

• The effect of Vin1 on VXis the same as that of a CS amplifierCS amplifier (degenerated by the resistance seen looking into the source of M )into the source of M2) on VD

Page 32: Chapter 4 Differential Amplifiers

Differential Gain: Effect of V on VDifferential Gain: Effect of Vin1 on VX

Neglecting λ2 and gmb2 RS≈1/gm2

11DX R

VV −

21

111mm

in

ggV +

21 mm gg

Page 33: Chapter 4 Differential Amplifiers

Differential Gain: Effect of V on VDifferential Gain: Effect of Vin1 on VY

The effect of Vin1 on VY is the same as that of a Source F ll (M ) lifi d i i C GFollower (M1) amplifier driving a Common-Gate amplifier (M2)

1inT VV = 1

1T

inT

R =1m

T g

Page 34: Chapter 4 Differential Amplifiers

Differential Gain: Effect of V on VDifferential Gain: Effect of Vin1 on VY

The effect of Vin1 on VY is the same as that of a Source F ll (M ) lifi d i i C GFollower (M1) amplifier driving a Common-Gate amplifier (M2)

RV

111

D

in

Y RVV

+≈

21

1

mm

in

gg+

Page 35: Chapter 4 Differential Amplifiers

V V as function of V if V =0VX-VY as function of Vin1 if Vin2=0

2R11__ 11

2)(1 inDmin

DVtodueYX VRgVRVV

in−=

+

−=−

21 mm gg

Because gm1=gm2=gm

Page 36: Chapter 4 Differential Amplifiers

By Symmetry: VX-VY as function of Vin2 if Vin1=0

2R22__ 11

2)(2 inDmin

DVtodueYX VRgVRVV

in=

+=−

21 mm gg

Page 37: Chapter 4 Differential Amplifiers

V V as function of V and VVX-VY as function of Vin2 and Vin1

12__)( inDminDmbothtodueYX VRgVRgVV −=−

yielding the gain g R regardless whereyielding the gain gmRD regardless where and how the inputs are applied

Page 38: Chapter 4 Differential Amplifiers

Single-ended Differential Voltage Gain

gV221

, Dm

inin

XSEV Rg

VVVA −=−

=

2

21, D

m

inin

YSEV Rg

VVVA =−

=

21 inin

Page 39: Chapter 4 Differential Amplifiers

Comparison: Differential voltage gain of a differential amplifier vs voltage gain of a CSdifferential amplifier vs. voltage gain of a CS

amplifier• If the same current source ISS drives the

differential amplifier and the CS, each transistor √of the differential amplifier has gm which is 1/√2

of that of the CS transistor. Differential gain √reduces by a factor of 1/√2 .

• If both amplifiers have the same W/L in each transistor and the same load, and we want the gain to be the same, then if we use ISS at CS, we SSneed to use 2ISS at the differential amplifier.

Page 40: Chapter 4 Differential Amplifiers

The “Virtual Ground” ConceptThe Virtual Ground Concept

• In a symmetric device (as above), if inputs change anti-y ( ), p gsymmetrically (one goes up by a certain amount, and the other goes down by the same amount), then VP does not changechange.

• For small-signal analysis point P becomes “virtual ground”.g

Page 41: Chapter 4 Differential Amplifiers

The “Virtual Ground” ConceptThe Virtual Ground Concept

• Explanation: Consider the complete “Kirchhoff path” V D D VVin1 D1 D2 Vin2.

• By symmetry of the devices, and anti-symmetry of sources, using voltage-division argument, VP stayssources, using voltage division argument, VP stays constant.

• See book (pp. 114-115) for 2-3 more explanations.

Page 42: Chapter 4 Differential Amplifiers

The “Half Circuit” ConceptThe Half-Circuit Concept

• For small-signal analysis because point P isFor small signal analysis, because point P is “ground” (this is valid only if inputs are anti-symmetric and devices are symmetric!) we cansymmetric and devices are symmetric!), we can analyze each CS “half-circuit” separately.

Page 43: Chapter 4 Differential Amplifiers

Differential Gain with λ effectDifferential Gain with λ effect

• Based on the half-circuit concept gainBased on the half circuit concept, gain calculation is highly simplified. We get:

• V /V = g (R ||r )=V /( V )• VX/Vin1=-gm(RD||ro)=VY/(-Vin1)• (VX-VY)/2Vin1=-gm(RD||ro)

Page 44: Chapter 4 Differential Amplifiers

In general Vin1 and Vin2 are arbitrary (not necessarily anti-symmetric): What do we do?

Page 45: Chapter 4 Differential Amplifiers

Analysis of Differential Amplifiers for arbitrary inputs

A l i it t l• As long as circuit operates more or less linearly, we use superposition of two analyses:

• Differential input analysis, using anti-p y , gsymmetric inputs derived from the difference between the inputs.d e e ce bet ee t e puts

• Common-mode analysis, where an input equals to the average of both inputs isequals to the average of both inputs is applied to both transistors.

Page 46: Chapter 4 Differential Amplifiers

CMOS Differential Amplifiers

Common-Mode Analysis –L17Common Mode Analysis L17

Page 47: Chapter 4 Differential Amplifiers

Goal: No common-mode signal at amplifier’s output

• If amplifier is not 100% symmetric, CM signals will not be fully cancelled out.g y

• If the DC current source (biasing the amplifier) is not ideal (that is has a finiteamplifier) is not ideal (that is, has a finite output resistance) then CM signal appears at each single-ended output.

Page 48: Chapter 4 Differential Amplifiers

Single-ended Common-Mode Response of a symmetric amplifier

Consider a small-signal analysis forsignal analysis for the common-mode signalsignal.

Current source is represented by its output resistance RSS

Page 49: Chapter 4 Differential Amplifiers

Single-ended Common-Mode Response of a symmetric amplifier

As Vin,CM changes so does VP As aso does VP. As a result, ID currents change and VX andchange, and VX and VY change.

VX-VY continues to be zero.

Page 50: Chapter 4 Differential Amplifiers

Single-ended Common-Mode Response of a symmetric amplifier

To find VX as function of Vi CM wefunction of Vin,CM we may do a “half circuit analysis”circuit analysis , splitting RSS into two parallel 2RSStwo parallel 2RSSresistors, or equivalentlyequivalently, connect transistors in parallel (asin parallel (as shown).

Page 51: Chapter 4 Differential Amplifiers

Single-ended Common-Mode Gain of a symmetric amplifier assuming λ=0 and γ=0

C

Y

C

X

C

outCMV V

VVV

VVA ===,

D

CMinCMinCMin

RVVV

−=2/

,,,

SSm Rg +)2/(1

M +M hasM1+M2 has twice the width and biasand bias current, therefore g istherefore gm is doubled.

Page 52: Chapter 4 Differential Amplifiers

Most Primitive Differential Amplifier: Resistor in place of current source

• Example: Let VDD=3V (W/L)1=(W/L)2=25/0 5Example: Let VDD 3V, (W/L)1 (W/L)2 25/0.5• µnCOX=50µA/V2, VTH=0.6V, λ=0, γ=0, RSS=500Ω

B I I 0 5 A h• Because ID1=ID2=0.5mA, we have:

VVIVV D 2312 1 + VV

LWC

VV TH

OXn

GSGS 23.121 =+==μ

Page 53: Chapter 4 Differential Amplifiers

“Resistor current source” exampleResistor current source example

VVIVV D 2312 1 + VV

LWC

VV TH

OXn

DGSGS 23.11

21 =+==μ

• Also: VS=I RSS=0 5VAlso: VS IssRSS 0.5V• Bias voltage at gates Vin,CM=VGS1+VS=1.73V

Thi lt t th 0 5 A• This voltage creates the necessary 0.5mA current in each of the transistors.

Page 54: Chapter 4 Differential Amplifiers

“Resistor current source” example – differential gain design

1WΩ

==632

12 1DOXnm ILWCg μ

If RD=3.16KΩ then differential voltage gain =If RD 3.16KΩ then differential voltage gain gmRD=5

Page 55: Chapter 4 Differential Amplifiers

“Resistor current source” example – with such RD are transistors in Saturation?

Vout1=Vout2=VDD-IDRD=1.42V > Vin,CM – VTH=1.73 – 0.6 = 1.13V by 290mV (the overdrive)

Page 56: Chapter 4 Differential Amplifiers

“Resistor current source” example –Common-Mode Response

If Vin,CM increases by 50mV, what will happen to each output?

Page 57: Chapter 4 Differential Amplifiers

“Resistor current source” example –Common-Mode Response

Large CM

RVA Dout 2/Δ

ggain of 1.94 is due to the

VVRVV

RgVA

D

SSm

D

CMin

outCMV

896941)50(2/||

)2/(1,,

ΔΔ

+−=

Δ=

small RSS

mVmVRg

VVSSm

DCMinX 8.9694.1)50(

)2/(1|| , =⋅=

+Δ=Δ⇒

Page 58: Chapter 4 Differential Amplifiers

Common-Mode Response with asymmetric RD assuming λ=0

ΔVX gΔVX

ΔVin ,CM

= − gm

1+ 2gmRSS

RD

ΔV gΔVY

ΔVin ,CM

= −gm

1+ 2gmRSS

(RD + ΔRD)

mYX RgVVΔ

Δ−Δ21,

DSSm

m

CMin

YX RRg

gV

Δ+

RSS above represents the current SS psource – need large RSS

Page 59: Chapter 4 Differential Amplifiers

Common-Mode Response with asymmetric RD

CM input noise corrupts the amplified differential signal, because of the asymmetry

Page 60: Chapter 4 Differential Amplifiers

For high-frequency Common-Mode input need to take into account parasitic capacitance effects, p p ,even if RSS is large. C1 is contributed by M1,M2 and ISS and contributes to the impedance “seen” by the SS p y

CM signal.

Page 61: Chapter 4 Differential Amplifiers

Mismatches in W/L, VTH and other transistor parameters all translate to mismatches in gm

PCMinmD VVgI −= )( ,11S ll i l

PCMinmD VVgI −= )( ,22

,Small-signal analysis

PSSPCMinmm VRVVgg =−+⇒ ))(( ,21

Page 62: Chapter 4 Differential Amplifiers

Mismatches in W/L, VTH and other transistor parameters all translate to mismatches in gm

PSSPCMinmm VRVVgg ,21 ))(( =−+

CMSSmm

P

SSCinmm

VRggV 21

,

)( +=⇒ CMin

SSmmP V

RggV ,

21 1)( ++⇒

Page 63: Chapter 4 Differential Amplifiers

DPCMinmX RVVgV )( ,1 −−=

DPCMinmY RVVgV )( ,2 −−=

Page 64: Chapter 4 Differential Amplifiers

Mismatches in W/L, VTH and other transistor parameters all translate to mismatches in gm

YX ggVV 21 −−D

SSmm

mm

CMin

YXDMCMV R

Rgggg

VVVA

1)( 21

21

,, ++

−==−

Page 65: Chapter 4 Differential Amplifiers

Common Mode GainsCommon-Mode Gains

• We have seen two types of common-

YX VVAmode gain:• AV,CM : Single-ended CMin

Y

CMin

XCMV VV

A,,

, ==V,CM g

output due to CM signal.

VV• AV,CM-DM : Differential output due to CM

YXDMCMV V

VVA ,−

=−output due to CM signal. CMinV ,

Page 66: Chapter 4 Differential Amplifiers

Common-Mode Rejection Ratio (CMRR) Definitions

|| DMSE A

ACMRRCMRR ==CMA

A ||DMCM

DMdiff A

ACMRRCMRR−

==

In both cases we want CMRR to be as large as possible and it translates intolarge as possible, and it translates into small matching errors and RSS as large as possiblepossible

Page 67: Chapter 4 Differential Amplifiers

CMOS Differential Amplifiers

MOS Loads – L18MOS Loads L18

Page 68: Chapter 4 Differential Amplifiers

MOS LoadsMOS Loads

• (a) Diode-connected load(b) C t S l d• (b) Current-Source load

Page 69: Chapter 4 Differential Amplifiers

MOS Loads: Analysis MethodMOS Loads: Analysis Method

• Differential Analysis: Use half-circuit method, with source node at virtual ground.

• Common-Mode Analysis: Again use half-circuit method, with appropriate accommodation for parallel transistors and for Rparallel transistors, and for RSS.

Page 70: Chapter 4 Differential Amplifiers

MOS Loads: Differential Gain FormulasMOS Loads: Differential Gain Formulas

rrggA )||||( 1−

NnmN

oPoNmPmNdiffV

LWg

rrggA

)/(

)||||(,

μ

−=

)||(, oPoNmNdiffV rrgA −=

Pp

Nn

mP

mN

LWgg

)/()(

μμ

−=−≈ff

Page 71: Chapter 4 Differential Amplifiers

Problems with Diode connected MOS LoadsProblems with Diode-connected MOS Loads

• Tradeoff among output voltage swing, voltage gain and CM input range:and CM input range:

• In order to achieve high gain, (W/L)P must be decrease, thereby increasing |VGSP-VTHP| and loweringdecrease, thereby increasing |VGSP VTHP| and lowering the CM level at nodes X and Y.

Page 72: Chapter 4 Differential Amplifiers

Overcoming Diode-connected Load swing problem for higher gains:

Use PMOS current sources which reduce gm of diode connected MOS instead of lowering (W/L) ofdiode-connected MOS, instead of lowering (W/L)P of load. Gain can be increased by factor of 5.

Page 73: Chapter 4 Differential Amplifiers

Problems with Current Source MOS LoadsProblems with Current-Source MOS Loads

• In sub-micron technologies, it’s hard to g ,obtain differential gains higher than 10-2020.

Page 74: Chapter 4 Differential Amplifiers

Solution to low gain problem: CascodingSolution to low-gain problem: Cascoding

)](||)[( 7551331, oomoommdiffV rrgrrggA ≈

Page 75: Chapter 4 Differential Amplifiers

CMOS Differential Amplifiers

Gilbert Cell-L19Gilbert Cell L19

Page 76: Chapter 4 Differential Amplifiers

Can we create a differential amplifier with voltage-controlled differential gain?

(a)is a VGA (Variable-Gain Amplifier). Vcontdetermines I which determines thedetermines Iss, which determines the differential gain.

Gain may be varied from 0 to some maximum value.

Page 77: Chapter 4 Differential Amplifiers

Can we create a differential amplifier with voltage-controlled differential gain?

What do we do if we want to vary the gain continuously from some negative value tocontinuously from some negative value to some positive value?

Page 78: Chapter 4 Differential Amplifiers

Can we create a differential amplifier with voltage-controlled differential gain?

In circuits (b) the two amplifiers have opposite differential gain simply by interchanging thedifferential gain simply by interchanging the order of output subtraction)

Page 79: Chapter 4 Differential Amplifiers

Can we create a differential amplifier with voltage-controlled differential gain?

If I1=I2 then Vout,1/Vin= -gmRD = - Vout,2/Vin

If I d I i it di ti th iIf we vary I1 and I2 in opposite directions, the gains will follow along these directions.

ff ?How should we combine the two differential outputs?

Page 80: Chapter 4 Differential Amplifiers

How to combine the differential outputs?

O th l ft t ll th tOn the left, we conceptually see the two voltages ADDED UP.

Gains A1 and A2 are voltage controlled.

Page 81: Chapter 4 Differential Amplifiers

How to combine the differential outputs? Math will show the implementation method.

Page 82: Chapter 4 Differential Amplifiers
Page 83: Chapter 4 Differential Amplifiers

Does it work as intended? Can gain be varied positively as well as negatively?

If I =0 then V =g RIf I1=0 then Vout=gmRD.

If I2=0 then Vout= -gmRD.

If I1=I2 then Vout=0 !!

Page 84: Chapter 4 Differential Amplifiers

Next phase in the conceptual development: Do we really need two separate controlDo we really need two separate control signals??

Recall the basic structure of a differential lifi Th i t diff f thamplifier: The inputs difference cause one of the

MOS currents to go up, and at the same time the t f th it MOS d b thcurrent of the opposite MOS goes down by the

same amount Let I1 , I2 come from diff. amp.

Page 85: Chapter 4 Differential Amplifiers

Gilbert CellGilbert Cell

Left: If |Vcont1 – Vcont2| is large we have “current stealing” and then gain is eithercurrent stealing , and then gain is either most positive or most negative.

Page 86: Chapter 4 Differential Amplifiers

Gilbert CellGilbert Cell

Right: Actual Implementation

Page 87: Chapter 4 Differential Amplifiers

Gilbert CellGilbert Cell

VOUT = kVinVcont

Page 88: Chapter 4 Differential Amplifiers

Applications of Gilbert CellApplications of Gilbert Cell

• Analog Multiplier– Mixer– Phase Detector

AM Modulation– AM Modulation• VGA: Variable-gain amplifier

– AGC (Automatic Gain Control)

It’s a versatile general-purpose tool

Page 89: Chapter 4 Differential Amplifiers

Can switch input and control signals!