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  • EE4340 / EECT 5340 Analog IC Analysis and Design Fall 2014

    Topic 7. Differential Amplifiers

    Jin Liu Ph.D.

    Professor

    UT Dallas

  • Page 2

    Differential Amplifiers Very Important

    Differential amplifier is among the most important circuit inventions

    Differential operation has become the dominant choice in todays high-performance analog and mixed signal circuits

  • Page 3

    Single-ended and Differential Operation

    A single-ended signal is measured with respect to a fixed potential

    A differential signal is measured between two nodes that have equal and opposite signal excursions around a fixed potential.

    Common-mode (CM) level.

  • Page 4

    Immunity of Environmental Noise

    Corruption of a signal due to

    coupling

    Reduction of coupling

    by differential operation

    V+ = Vcm+Vid/2

    V- = Vcm-Vid/2

    Vcm = (V+ + V-)/2

    Vid = V+ - V-

  • Page 5

    Effect of Supply Noise

  • Page 6

    Differential Distribution of Noisy Lines

  • Page 7

    Major Advantages of Differential Signaling

    Immunity of Environmental Noise

    Noise coupling from digital lines

    Power supply noise

    Differential noisy lines

    Increase the maximum achievable voltage swing (x2)

    -1v

    1v

    0v Single-ended swing: 2v

    -1v to 1v

    Differential swing: 4v

    -2v to 2v

  • Page 8

    Basic Differential Pair

    AKA: Source-coupled pair or long tailed pair

  • Page 9

    Input-output Characteristics

    When Vin1

  • Page 10

    Input Common Mode Range (ICMR)

    1. Tie both inputs together

    2. Sweep the input voltage and

    find the input voltage range in

    which all transistors are

    saturated

    Vin,CM=Vgs1+Vod3=Vth1+Vod1+Vod3

  • Page 11

    Input Common Mode Range

    ],2

    min[ 2,1,31 DDTSS

    DDDCMinODGS VVI

    RVVVV

    VGS1=VT1+sqrt{2*Iss/2/[K*(W/L)1]}

    Iss Id1=Id2=Id3/2=Iss/2

    VOD3=sqrt{2*Iss/[K*(W/L)3]}

  • Page 12

    Large Signal Analysis

    Suppose M1 and M2 are saturated

    21

    2

    21

    21

    2

    21

    2121

    2

    2121

    2)(2

    1

    )2(2

    )(

    22

    2,)(

    2

    1

    DDSSininoxn

    DDSS

    oxn

    inin

    oxn

    D

    oxn

    Dinin

    T

    oxn

    DGSTGSoxnD

    GSGSinin

    IIIVVL

    WC

    III

    L

    WC

    VV

    L

    WC

    I

    L

    WC

    IVV

    V

    L

    WC

    IVVV

    L

    WCI

    VVVV

  • Page 13

    Large Signal Analysis

    2

    212121

    2

    21

    2

    21

    22

    21

    2

    21

    4

    21

    22

    21

    2

    21

    22

    21

    2

    2121

    21

    2

    21

    24

    21

    2

    21

    2

    21

    )(4

    )(2

    1

    ])(4

    [)()(4

    1)(

    )()()(4

    1)(

    )()()(4

    4)()()(4

    1

    2)(2

    1

    inin

    oxn

    SSininoxnDD

    inin

    oxn

    SSininoxnDD

    ininoxnSSininoxnDD

    DDSSDDDDDD

    DDSSininoxnSSininoxn

    DDSSininoxn

    VV

    L

    WC

    IVV

    L

    WCII

    VV

    L

    WC

    IVV

    L

    WCII

    VVL

    WCIVV

    L

    WCII

    IIIIIIIII

    IIIVVL

    WCIVV

    L

    WC

    IIIVVL

    WC

    Squaring both sides,

    Also

    Then

  • Page 14

    Large Signal Analysis

    0,

    4

    24

    2

    1||

    ,

    )(4

    |)(|2

    1

    2

    2

    2121

    2

    212121

    inSSoxn

    in

    oxn

    SS

    in

    oxn

    SS

    oxn

    in

    D

    inininDDD

    inin

    oxn

    SSininoxnDD

    VIL

    WCGm

    V

    L

    WC

    I

    V

    L

    WC

    I

    L

    WC

    V

    I

    VVVIII

    VV

    L

    WC

    IVV

    L

    WCII

    Sign of Id1-Id2, and Vin1-Vin2

  • Page 15

    Large Signal Analysis

    DSSoxnv

    DDDDDDoutout

    inSSoxn

    RIL

    WCA

    IRIRVDDIRVDDVV

    VIL

    WCGm

    ||

    )()(

    0,

    1221

  • Page 16

    Small Signal Analysis Differential Mode

    Half-circuit concept Node P is a virtual AC ground

  • Page 17

    Lemma

    Consider above circuit, where D1 and D2 represent any

    three-terminal active device. Suppose Vin1 changes from Vo

    to Vo+Vin and Vin2 from Vo to Vo-Vin. Then, if the

    circuit remains linear, Vp does not change

  • Page 18

    Prove

    Assume V1 and V2 have equilibrium value of Va and change

    by V1 and V2. The output currents then change by gmV1

    and gmV2. Since I1+I2=IT, gmV1+gmV2=0, i.e. V1= -

    V2. Also, Vin1-V1=Vin2-V2, thus Vo+Vin-(Va+V1)=Vo-

    Vin-(Va+V2). Consequently, 2Vin=V1-V2=2V1.

  • Page 19

    Small Signal Gain - Differential

    )||(

    ,

    )]||()||([2

    1

    )(2

    1

    2)(

    )||(

    )||(

    2,12,1

    2,1212,121

    2211

    11

    11121

    21

    22

    12

    11

    1

    oDm

    ooommm

    oDmoDm

    in

    y

    in

    x

    in

    yx

    inin

    yx

    inin

    outout

    oDm

    in

    y

    in

    y

    oDm

    in

    x

    rRggain

    rrrggg

    rRgrRggain

    v

    v

    v

    vgain

    v

    vv

    vv

    vv

    vv

    vvgain

    rRgv

    v

    v

    v

    rRgv

    v

    12 inin vv

  • Page 20

    Differential Pair with MOS Loads - Gain

    4,3

    2,1

    4,3

    2,1

    1

    4,34,32,12,1

    2,14,34,3

    2,1

    )/(

    )/(

    )||||(

    1

    LW

    LW

    g

    gA

    grrgA

    ggggA

    p

    n

    m

    m

    v

    moomv

    oom

    mv

    )||(

    1

    4,32,12,1

    4,32,1

    2,1

    oomv

    oo

    mv

    rrgA

    gggA

  • Page 21

    Differential Pair with MOS Loads _ICMR

    Vin>Vgs1+Vds(sat, Iss), Vgs1=sqrt[2*Iss/2/(KW/L)]+Vth1

    For M1 in sat, Vout>Vin-Vth1,

    Vin

  • Page 22

    Differential Pair with MOS Loads _Output Swing

    Vcm+Vid/2

    Vcm-Vid/2

    Vout1Vdd-Vsg3, (Id3=Iss)

    Vout1>Vcm-Vth1

    Vout1Vcm-Vth1

    Vcm+Vid/2

    Vcm-Vid/2

  • Page 23

    Differential Pair with MOS Loads

    )||( 7551331 oomoommv rrgrrggA

  • Page 24

    Common Mode Response

    SS

    m

    D

    CMin

    CMoutoutoutCMv

    inind

    ininCM

    dCMin

    dCMin

    Rg

    R

    v

    vvvvA

    VVV

    VVV

    VVV

    VVV

    2

    1

    2/)(

    2

    5.0

    5.0

    ,

    21,

    21

    21

    2

    1

    In symmetric circuit, input CM

    variations disturb the bias points,

    alternating the small signal gain

    and possibly limiting the output

    voltage swings. Node P is not a AC ground!!

  • Page 25

    Common Mode Response (2)

    VDD

    RD

    Vin,CM

    2RSS

    Vout

    M1

    VDD

    RD

    YX

    M2

    M1

    Vin,CM

    P

    2RSS

    RD

    2RSS

    )21(

    )21(

    )]21([

    )21(

    )]21([

    21

    ,SSm

    DmoutmCMv

    SSmo

    SSmoD

    SSmoD

    SSmoDout

    SSm

    mm

    Rg

    RgRGA

    Rgr

    RgrR

    RgrR

    RgrRR

    Rg

    gG

  • Page 26

    Common Mode Response

    Variation of output CM level, in the absence of mismatch

    Av,CM Conversion of input common-mode variations to differential variation at the output

    Circuit component mismatch

    Asymmetrical topology

    Av,CM-DM

  • Page 27

    Component Mismatch

    DSSm

    m

    CM,in

    yX

    DMCM

    DDSSm

    mCM,iny

    DSSm

    mCM,inX

    RRg21

    g

    V

    VVA

    )RR(Rg21

    gVV

    RRg21

    gVV

    Common mode change at the

    input introduces differential

    change at the output

  • Page 28

    CMRR Common Mode Rejection Ratio

    DMCM

    DM

    A

    ACMRR

  • Page 29

    Differential Amplifier with Active Current Mirror Load

    Active current mirror

    that process signal

    When Vin1 decreases and Vin2 increase, more current flows through

    M2 and M4, Vout decreases. When Vin1

  • Page 30

    Differential Amplifier with Active Current Mirror Load Large signal analysis cont.

    Active current mirror

    that process signal

    When Vin1 increase and Vin2 decreases, more current flows through

    M1 and M3, Vout increases. When Vin1>>Vin2, M2 is off, zero

    current flows through M2,M4. M4 operates in deep triode region,

    Vout=VDD

  • Page 31

    Differential Amplifier with Active Current Mirror Load Large signal analysis cont.

    Active current mirror

    that process signal

    When Vin1=Vin2, each branch has half the tail current, Vout = VF

    assuming perfect symmetry.

    In reality, however, asymmetries in the circuit may result a large

    deviation in Vout, possibly driving M2 or M4 into the triode region.

  • Page 32

    Large signal analysis Input & Output Swing

    Active current mirror

    that process signal

    For M2 to be saturated, Vout>Vin2-Vth2. For maximum swing

    range, the input common mode level should be as small as possible.

    Minimum input common mode level to keep all transistors saturated

    is Vod5+Vgs1,2

    The direct relationship between the input CM level and the output

    swing in this circuit is a critical drawback.

  • Page 33

    Small Signal Analysis

    Asymmetry in two branches causes

    small voltage swing in P.

    If ignore this swing, P can be assumed

    to be virtual ground.

    (Refer to the Razavi book on analysis

    when P is NOT assumed virtual ground.

    The final result after approximation

    leads to the same answer

    here.)

  • Page 34

    Small Signal Analysis Av, Gm and Rout

    Av=Gm Rout

    Gm is short circuit transconductance;

    it is calculated with the circuit setup

    on the left. 21

    inm

    vg

    21

    inm

    vg

    22

    inm

    vg

    )||(

    ||

    2

    22

    242,1

    24

    2,121

    21

    oomoutm

    ooout

    mmm

    in

    outm

    inm

    inm

    rrgRGAv

    rrR

    ggg

    v

    iG

    vg

    vgiout

  • Page 35

    Common Mode Properties

    Assuming symmetry,

    Vout=VF

    )||()21(

    21

    1

    )||(||

    21

    1

    2

    1

    2||

    2

    1

    4,32,14,32,1

    2,14,3

    2,1

    4,32,12,1

    2,14,3

    2,1

    2,1

    4,3

    4,3

    ,

    OOmm

    mm

    m

    OOm

    CM

    DM

    mm

    m

    m

    O

    m

    CMin

    VoutCM

    rrgRssg

    Rssgg

    g

    rrg

    A

    ACMRR

    Rssgg

    g

    Rssg

    r

    g

    VA

    Even with perfect

    symmetry, the output signal

    is corrupted by input CM

    variation a drawback that

    does not exist in fully

    differential circuits.

  • Homework #6

    Due on 10/23/2014