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    CapacitancesCapacitances

    Alpana AgarwalAssistant Professor

    Email: [email protected], [email protected]

    Electronics & Communication Engineering Department

    Thapar University, Patiala

    Alpana Agarwal, Thapar University 210/13/2007

    CapacitanceCapacitance

    Any two conductors separated by an insulatorhave capacitance

    Essential for transient and ac responses

    Most of them are distributed & not lumped

    On-chip capacitances, used for hand estimation

    Gate to channel capacitor is very important Creates channel charge necessary for operation

    Source and drain have capacitance to body Across reverse-biased diodes

    Called diffusion capacitance because it is associatedwith source/drain diffusion

    More parasitic capacitances

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    Alpana Agarwal, Thapar University 310/13/2007

    CMOS Inverter: DynamicCMOS Inverter: Dynamic

    VDD

    Rn

    Vout = 0

    Vin = V DD

    CL tpHL = f(Rn, CL)

    Todays focus

    Covered earlier

    Transient, or dynamic, response determines the maximumspeed at which a device can be operated.

    Alpana Agarwal, Thapar University 410/13/2007

    Sources of CapacitanceSources of Capacitance

    Cw

    CDB2

    CDB1

    CGD12

    CG4

    CG3

    wiring (interconnect) capacitance

    intrinsic MOS transistor capacitances

    Vout2Vin

    extrinsic MOS transistor (fanout) capacitances

    Vout

    VoutVin

    M2

    M1

    M4

    M3

    Vout2

    CL

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    Alpana Agarwal, Thapar University 510/13/2007

    MOS Intrinsic CapacitancesMOS Intrinsic Capacitances

    Structure capacitances

    Channel capacitances

    Depletion regions of the reverse-biased pn-junctions of the drainand source

    Alpana Agarwal, Thapar University 610/13/2007

    MOS Structure CapacitancesMOS Structure Capacitances

    LDSource

    n+Drain

    n+W

    Ldrawn

    Poly Gate

    n+n+

    tox

    Leff

    Top view

    lateral diffusion

    CGSO = CGDO = Cox LD W = Co W

    Overlap capacitance (linear)

    LD

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    Alpana Agarwal, Thapar University 710/13/2007

    MOS Channel CapacitancesMOS Channel Capacitances

    S D

    p substrate

    B

    GVGS +

    -

    n+n+

    depletionregion

    n channel

    CGS = CGCS + CGSO CGD = CGCD + CGDO

    CGB = CGCB

    The gate-to-bulk capacitance depends upon theoperating region and the terminal voltages

    Alpana Agarwal, Thapar University 810/13/2007

    Average Distribution of ChannelAverage Distribution of ChannelCapacitanceCapacitance

    (2/3)CoxWL +2CoW

    (2/3)CoxWL0(2/3)CoxWL0Saturation

    CoxWL + 2CoWCoxWLCoxWL/2CoxWL/20Resistive

    CoxWL + 2CoWCoxWL00CoxWLCutoff

    CGCGCCGCDCGCSCGCBOperationRegion

    Channel capacitance components are nonlinear and varywith operating voltage

    Most important regions are cutoff and saturation since thatis where the device spends most of its time

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    Alpana Agarwal, Thapar University 910/13/2007

    MOS Diffusion CapacitancesMOS Diffusion Capacitances

    S D

    p substrate

    B

    GVGS +

    -

    n+n+

    depletionregion

    n channel

    CSB

    = CSdiff

    CDB

    = CDdiff

    The junction (or diffusion) capacitance is from the reverse-biased source-body and drain-body pn-junctions.

    Alpana Agarwal, Thapar University 1010/13/2007

    Source Junction ViewSource Junction View

    side walls

    channel

    W

    xj

    channel-stopimplant (NA+)

    source

    bottom plate(ND)

    LSource

    substrate (NA)

    Cdiff = Cbp + Csw = Cj AREA + Cjsw PERIMETER

    = Cj LSource W + Cjsw (2LSource + W)

    junctiondepth

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    Alpana Agarwal, Thapar University 1110/13/2007

    Review: Reverse Bias DiodeReview: Reverse Bias Diode

    All diodes in MOS digital circuits are reverse biased;

    the dynamic response of the diode is determined by depletion-region charge or junction capacitance

    Cj = Cj0/((1 VD)/0)m

    where Cj0 is the capacitance under zero-bias conditions (afunction of physical parameters), 0 is the built-in potential (afunction of physical parameters and temperature) and m is thegrading coefficient

    m = for an abruptjunction (transition from n to p-material is instantaneous)

    m = 1/3 for a linear (or graded) junction (transition is gradual)

    Nonlinear dependence (that decreases with increasing reverse

    bias)

    +

    -VD

    Alpana Agarwal, Thapar University 1210/13/2007

    MOS Capacitance ModelMOS Capacitance Model

    CGS

    CSB CDB

    CGD

    CGB

    S

    G

    B

    D

    CGS = CGCS + CGSO CGD = CGCD + CGDO

    CGB = CGCB

    CSB = CSdiff CDB = CDdiff

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    Alpana Agarwal, Thapar University 1310/13/2007

    Transistor Capacitance ValuesTransistor Capacitance Valuesfor 0.25for 0.25

    0.90.320.220.90.481.90.276PMOS

    0.90.440.280.90.520.316NMOS

    bsw(V)

    mjswCjsw(fF/m)

    b(V)

    mjCj(fF/m2)

    Co(fF/m)

    Cox(fF/m2)

    Example: For an NMOS with L = 0.24 m, W = 0.36 m,

    Ldrain = Lsource = 0.625 m

    CGC = Cox WL =

    CGSO = CGDO = Cox LD W = Co W =

    so Cgate_cap = CoxWL + 2CoW =

    Cbp = Cj LSource W =

    Csw = Cjsw (2LSource + W) =

    so Cdiffusion_cap =

    Alpana Agarwal, Thapar University 1410/13/2007

    Transistor Capacitance ValuesTransistor Capacitance Valuesfor 0.25for 0.25

    0.90.320.220.90.481.90.276PMOS

    0.90.440.280.90.520.316NMOS

    bsw(V)

    mjswCjsw(fF/m)

    b(V)

    mjCj(fF/m2)

    Co(fF/m)

    Cox(fF/m2)

    Example: For an NMOS with L = 0.24 m, W = 0.36 m,Ldrain = Lsource = 0.625 m

    CGC = Cox WL =

    CGSO = CGDO = Cox LD W = Co W =

    so Cgate_cap = CoxWL + 2CoW =

    Cbp = Cj LSource W =

    Csw = Cjsw (2LSource + W) =

    so Cdiffusion_cap =

    0.11 fF

    0.52 fF

    0.74 fF

    0.45 fF

    0.45 fF

    0.90 fF

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    Alpana Agarwal, Thapar University 1510/13/2007

    Review: Sources of CapacitanceReview: Sources of Capacitance

    Vout

    Cw

    Vin

    CDB2

    CDB1

    CGD12

    M2

    M1

    M4

    M3

    Vout2

    CG4

    CG3

    wiring (interconnect) capacitance

    intrinsic MOS transistor capacitances

    Vout2Vin

    extrinsic MOS transistor (fanout) capacitances

    Vout

    CL

    ndrain

    pdrain

    Alpana Agarwal, Thapar University 1610/13/2007

    Extrinsic (FanExtrinsic (Fan--Out) CapacitanceOut) Capacitance

    The extrinsic, or fan-out, capacitance is the total gatecapacitance of the loading gates M3 and M4.

    Cfan-out = Cgate (NMOS) + Cgate (PMOS)

    = (CGSOn+ CGDOn+ WnLnCox) + (CGSOp+ CGDOp+WpLpCox)

    Simplification of the actual situation

    Assumes all the components of Cgate are between Vout and GND (or VDD)

    Assumes the channel capacitances of the loading gates are constant

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    Alpana Agarwal, Thapar University 1710/13/2007

    Layout of Two Chained InvertersLayout of Two Chained Inverters

    InOut

    Metal1

    VDD

    GND

    1.2m=2

    1.125/0.25

    0.375/0.25

    PMOS

    NMOS

    Polysilicon

    2.3750.72.3750.71.125/0.25PMOS

    1.8750.31.8750.30.375/0.25NMOSPS (m)AS (m

    2

    )PD (m)AD (m2

    )W/L

    0.125 0.5

    Alpana Agarwal, Thapar University 1810/13/2007

    Components of CComponents of CLL (0.25(0.25mm))

    6.06.1CL

    0.120.12from extractionCw

    2.282.28(2 Cop)Wp + CoxWpLpCG4

    0.760.76(2 Con)Wn + CoxWnLnCG3

    1.151.5KeqbppADpCj + KeqswpPDpCjswCDB2

    0.900.66KeqbpnADnCj + KeqswnPDnCjswCDB1

    0.610.612 Cop WpCGD2

    0.230.232 Con WnCGD1

    Value (fF)LH

    Value (fF)HL

    Expression

    C Term

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    Alpana Agarwal, Thapar University 1910/13/2007

    Wiring CapacitanceWiring Capacitance

    The wiring capacitance depends upon the lengthand width of the connecting wires and is a function of the fan-out from the driving gate and thenumber of fan-out gates.

    Wiring capacitance is growing in importance with the scaling of technology.

    Alpana Agarwal, Thapar University 2010/13/2007

    Parallel Plate Wiring CapacitanceParallel Plate Wiring Capacitance

    electrical field linesW

    H

    tdi dielectric (SiO2)

    substrate

    Cpp = (di/tdi) WL

    current flow

    permittivity

    constant(SiO2= 3.9)

    L

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    Alpana Agarwal, Thapar University 2110/13/2007

    Permittivity Values of Some DielectrPermittivity Values of Some Dielectricsics

    3.2 4.0Fluorosilicate glass (FSG)

    2.6 2.8Aromatic thermosets (SiLK)

    11.7Silicon

    9.5Alumina (package)

    7.5Silicon nitride

    5Glass epoxy (PCBs)

    3.9 4.5Silicon dioxide

    3.1 3.4Polyimides (organic)

    2.1Teflon AF

    1Free spacediMaterial

    Alpana Agarwal, Thapar University 2210/13/2007

    Sources ofSources ofInterwireInterwire CapacitanceCapacitance

    interwire

    fringe

    pp

    Cwire = Cpp + Cfringe + Cinterwire= (di/tdi)WL

    + (2di)/log(tdi/H)

    + (di/tdi)HL

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    Alpana Agarwal, Thapar University 2310/13/2007

    Impact ofImpact ofInterwireInterwire CapacitanceCapacitance

    (from [Bakoglu89])

    Alpana Agarwal, Thapar University 2410/13/2007

    InsightsInsights

    For W/H < 1.5, the fringe component dominates the parallel-plate component. Fringing capacitance can increase the overall capacitance by a factor of 10 or more.

    When W < 1.75H interwire capacitance starts to dominate

    Interwire capacitance is more pronounced for wires in the higher interconnect layers (further from the substrate)

    Rules of thumb

    Never run wires in diffusion

    Use poly only for short runs Shorter wires lower R and C

    Thinner wires lower C but higher R

    Wire delay nearly proportional to L2

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    Alpana Agarwal, Thapar University 2510/13/2007

    Wiring CapacitancesWiring Capacitances

    52271914121212

    38149.16.65.45.45.2Al5

    452718151514

    35158.976.86.5Al4

    4927201918

    4115109.48.9Al3

    45292725

    36171513Al2

    544740

    574130Al1

    5488Poly

    Al4Al3Al2Al1PolyActiveField

    fringe in aF/mpp in aF/m2

    1158585859540Interwire Cap

    Al5Al4Al3Al2Al1Poly

    per unit wire length in aF/m for minimally-spaced wires

    Alpana Agarwal, Thapar University 2610/13/2007

    Dealing with CapacitanceDealing with Capacitance

    Low capacitance (low-k) dielectrics (insulators)such as polymide or even air instead of SiO2 family of materials that are low-k dielectrics

    must also be suitable thermally and mechanically and

    compatible with (copper) interconnect

    Copper interconnect allows wires to be thinnerwithout increasing their resistance, thereby decreasing interwire capacitance

    SOI (silicon on insulator) to reduce junction capacitance

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    Alpana Agarwal, Thapar University 2710/13/2007

    Gate CapacitanceGate Capacitance

    Approximate channel as connected to source Cgs = oxWL/tox = CoxWL = CpermicronW

    Cpermicron is typically about 2 fF/m

    n+ n+

    p-type body

    W

    L

    tox

    SiO2

    gate oxide(good insulator,

    ox= 3.9

    0)

    polysilicongate

    Alpana Agarwal, Thapar University 2810/13/2007

    Diffusion CapacitanceDiffusion Capacitance

    Csb, Cdb Undesirable, called parasitic capacitance

    Capacitance depends on area and perimeter

    Use small diffusion nodes

    Comparable to Cgfor contacted diff

    Cg for uncontacted

    Varies with process

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    Questions, if any?Questions, if any?Questions, if any?Questions, if any?Questions, if any?Questions, if any?Questions, if any?Questions, if any?