nmos n' pmos

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  • 8/8/2019 nmos n' pmos

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    Lecture 20-1

    MOSFET transistor I-V characteristics

    iD K 2 vGS Vt( )vDS vDS2

    [ ]=

    iD

    vGS

    vDS--

    ++

    iD

    K vGS

    Vt

    ( )2

    [ ] 1 vDS

    +( )=

    KW

    2L------K

    n=

    Kn

    Cox

    n

    =iD

    K 2 vGS

    Vt

    ( )vDS

    [ ]=Linear region:

    vDS

    sat

    vGS

    Vt

    =

    vDS

    vGS

    Vt

    Triode region:

    vDS

    vGS

    Vt

    0

    VS1B=0

    VBVS2B=0

    VS1B=0

    VS2B>0

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    Lecture 20-4

    Body Effect

    Positive VSB for NMOSFETs tends to increase QB, hence decrease QI, for a

    fixed VGS

    VB

    VGS > Vt

    +

    n+n+ QB0

    VS>0

    QI

    VDS > 0

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    Lecture 20-5

    Body Effect

    Modeled as a change in the threshold voltage as a function of VSB

    The source is, by definition for NMOSFET, at a lower positive potential thanthe drain, which is why we use it as our reference voltage

    Vt

    Vt0

    2f

    VSB

    + 2f

    ( )+=

    SPICE will calculate this variation in threshold voltage, or you can over-rideits calculation by directly specifying gamma

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    Lecture 20-6

    Temperature Variations

    The threshold voltage varies with temperature due to carrier generation in thesubstrate --- tends to decrease with increasing temperature

    ~2mV for every 1C increase

    K also changes with temperature due to change in mobility

    Tends to dominate temperature variation for large iD

    Will iD increase or decrease with temperature?

    Vt Vt0 2f VSB+ 2f( )+=

    T1

    T2 > T1

    I1

    2---

    nC

    ox

    W

    L----- v

    GSV

    t( )

    2

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    Lecture 20-7

    Where is drain, where is source?

    S

    D

    GB

    D

    GB

    S

    n-channel transistor p-channel transistor

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    Lecture 20-8

    PMOSFETs

    All of the voltages are negative Carrier mobility is about half of what it is for n channels

    p+

    n

    S DG

    B

    p+

    The bulk is now connected to the most positive potential in the circuit

    Strong inversion occurs when the channel becomes as p-type as it was n-type

    The inversion layer is a positive charge that is sourced by the larger potential

    and drained at the smallest potential The threshold voltage is negative for an enhancement PMOSFET

    Note that the flatband voltage (which is negative) effects now tend toincrease the PFET threshold while they decreased the NFET threshold

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    Lecture 20-9

    PMOS

    The equations are the same, but all of the voltages are negative Triode region:

    iD K 2 vGS Vt( ) vDS vDS2[ ]=

    vGS

    Vt

    vDS

    vGS

    Vt

    K 12---nCoxWL

    -----= AV

    2-------

    iD is also negative --- positive charge flows into the drain

    Saturation expression is the same as it is for NFETs:

    iD

    satK v

    GSV

    t( )

    2[ ] 1 v

    DS+( )=

    +V dd

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    Lecture 20-10

    PMOS

    Characteristic appears to be the same, except that all of the voltages arenegative

    -5 -4 -3 -2 -1 0

    -100

    -90

    -80

    -70

    -60

    -50

    -40

    -30

    -20

    -10

    0

    10

    W=1 micronL=1 micronsV t0= -1 volt

    Kp=2e-5 (A/v2)

    phi =-0.6

    ND=1e15

    IDS

    (A)

    VDS

    VGS=-2.5V

    VGS=-2.0V

    VGS=-1.5V

    VGS=-1.0V

    VGS=-3.0V

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    Lecture 20-11

    PMOS

    But it is generally displayed as:

    W=1 micronL=1 micronsV t0= -1 volt

    Kp=2e-5 (A/v 2)phi =-0.6

    ND=1e15

    -IDS(A)

    -VDS

    VGS=-2.5V

    VGS=-2.0V

    VGS=-1.5V

    VGS=-1.0V

    VGS=-3.0V

    0 1 2 3 4 5

    -10

    0

    10

    20

    30

    40

    50

    60

    70

    80

    90

    100

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    Lecture 20-12

    Depletion Mode NMOSFET

    Depletion mode FETs have a channel implanted such that there is conductionwith VGS=0

    The operation is the same as the enhancement mode FET, but the thresholdvoltage is shifted

    Vt is negative for depletion NMOS, and positive for depletion PMOS

    VGS

    n+n+

    VS VDS

    n+

    p

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    Lecture 20-13

    Depletion Mode NMOSFET

    Negative gate voltage is required to turn the channel off

    W=1 micronL=1 micronsV t0= -2 volt

    Kp=2e-5 (A/v2

    )

    IDS(mA)

    VDS

    VGS

    =1.0V

    VGS=0.0V

    VGS

    =-1.0V

    VGS=-2.0V

    VGS=2.0V

    0 1 2 3 4 5

    0.0

    0.2

    0.4

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    Lecture 20-14

    Depletion Mode NMOSFET

    The iDS vs. vGS characteristic is still quadratic in saturation

    W=1 micronL=1 micronsV t0= -2 voltKp=2e-5 (A/v

    2)

    IDS(m

    A)

    VGS

    -4 -3 -2 -1 0 1 2 3 4 5

    0

    1

    2

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    Lecture 20-15

    Examples

    Find the largest value that RD can have before the transistor fails to operate insaturation

    5V

    -5V

    5k

    RD

    Vt

    2V=

    Kn

    20A V2

    =

    L 10m=

    W 400m=

    0=

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    Lecture 20-16

    Examples

    Find the drain currents and voltages for both transistors

    10V

    10k 15k

    Vt

    2V=

    Kn

    20A V2

    =

    L 10m=

    W 100m=

    0=

    10V

    M2 M1

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    Lecture 20-17

    Examples

    What is the effective resistance of the transistor in the triode region?

    10V

    24.8k Vt 1V=

    K 0.5m A V2=

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    Lecture 20-18

    Examples

    Select the Rs so that the gate voltage is 4V, the drain voltage is 4V and thecurrent is 1mA.

    10V

    RD

    Vt

    2V=

    K 1m A V

    2

    = 0=

    RS

    10V

    RG1

    RG2

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    Lecture 20-19

    Examples

    Select the Rs so that the transistor is in saturation with a drain current of1.0mA and a drain voltage of 5V

    Vt 1 V=K 0.5m A V

    2=

    0=

    RD

    10V

    RG1

    RG2

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    Lecture 20-20

    Examples

    Solve for the drain current and voltage

    20V

    32k

    Vt

    2 V=

    K 1m A V2

    =

    0=

    4k10M