2006 devmodel - [Download PPT Powerpoint]

CMOS Device Model

• Objective– Hand calculations for analog design– Efficiently and accurately simulation

• CMOS transistor models– Large signal model– Small signal model– Simulation model– Noise model

Large Signal Model• Nonlinear equations for solving dc values of

device currents given voltages• Level 1: Shichman-Hodges (VT, K', , and

NSUB)• Level 2: with second-order effects (varying

channel charge, short-channel, weak inversion, varying surface mobility, etc.)

• Level 3: Semi-empirical short-channel model• Level 4: BSIM models. Based on automatically

generated parameters from a process characterization. Good weak-strong inversion transition.

Transconductance when VDS is small

Transconductance when VDS is small

Transconductance when VDS is small

Effect of changing VDS for a large VGS

Effect of changing VDS for a given VGS

Effect of changing VDS for a given VGS

Effect of changing VDS for various VGS

VGS<=VT

Effect of changing VDS for various VGS

Effect of changing VDS for various VGS

MOST Regions of Operation

• Cut-off, or non-conducting: VGS <VT

– ID=0

• Conducting: VGS >=VT

– Saturation: VDS > VGS – VT

– Triode or linear or ohmic or non-saturation: VDS <= VGS – VT

)-)V - V((vL

WμC i DSV

DSTGSox

D 2

2

2) - V(v

L

WμC i TGS

oxD

With channel length modulation

)λV() - V(vL

WμC i DSTGS

oxD 1

22

) 22(0 | |φ - | |v| |φ V V fBSfTT

L

WK

L

WμC ox '

Capacitors Of The Mosfet

CBD and CBS include both the diffusion-bulk junction capacitance as well as the side wall junction capacitance. They are highly nonlinear in bias voltages.

C4 is the capacitance between the channel and the bulk. It is highly nonlinear and depends on the operation of the device. C4 is not measurable from terminals.

/2

Gate related capacitances

Small signal model

Typically: VDB, VSB are in such a way that there is a reversely biased pn junction.

Therefore: gbd ≈ gbs ≈ 0

In saturation:

But

In non-saturation region

High Frequency Figures of Merit T

• AC current source input to G• AC short S, D, B to gnd• Measure AC drain current output• Calculate current gain• Find frequency at which current gain = 1.

• Ignore rs and rd, Cbs, Cbd, gds, gbs, gbd all have zero voltage drop and hence zero current

• Vgs = Iin /jw(Cgs+Cgb+Cgd) ≈ Iin /jwCgs

• Io = − (gm − jw Cgd)Vgs ≈ − gmVgs

• |Io/Iin| ≈ gm/wCgs

• At T, current gain =1

• T ≈ gm/(Cgs+Cgd)≈ gm/Cgs

• or

• AC current source input to G• AC short S, D, B to gnd• Measure AC power into the gate• Assume complex conjugate load• Compute max power delivered by the transistor• Find maximum power gain• Find frequency at which power gain = 1.

High Frequency Figures of Merit max

• max: frequency at which power gain becomes 1

PL=

BSIM models• Non-uniform charge density• Band bending due to non-uniform gate voltage• Non-uniform threshold voltage

– Non-uniform channel doping, x, y, z– Short channel effects

• Charge sharing• Drain-induced barrier lowering (DIBL)

– Narrow channel effects– Temperature dependence

• Mobility change due to temp, field (x, y)• Source drain, gate, bulk resistances

“Short Channel” Effects

• VTH decreases for small L

– Large offset for diff pairs with small L

• Mobility reduction:– Velocity saturation

– Vertical field (small tox=6.5nm)

– Reduced gm: increases slower than root-ID

Threshold Voltage VTH

• Strong function of L– Use long channel for VTH matching

– But this increases cap and decreases speed

• Process variations– Run-to-run– How to characterize?– Slow/nominal/fast– Both worst-case & optimistic

Effect of Velocity Saturation

• Velocity ≈ mobility * field

• Field reaches maximum Emax

– (Vgs-Vt)/L reaches ESAT

• gm become saturated:– gm ≈ ½nCoxW*ESAT

• But Cgs still 2/3 WL Cox

• T ≈ gm/Cgs = ¾ nESAT /L

• No longer ~ 1/L^2

Threshold Reduction• When channel is short, effect of Vd extends to S• Cause barrier to drop, i.e. Vth to drop• Greatly affects sub-threshold current: 26 mV Vth

drop current * e• 100~200 mV Vth drop due to Vd not uncommon

100s or 1000 times current increase

• Use lower density active near gate but higher density for contacts

Other effects• Temperature variation• Normal-Field Mobility Degradation• Substrate current

– Very nonlinear in Vd

• Drain to source leakage current at Vgs=0– Big concern for static power

• Gate leakage currents– Hot electron– Tunneling – Very nonlineary

• Transit Time Effects

Consequences for Design • SPICE (HSPICE or Spectre)

– BSIM3, BSIM4 models– Accurate but inappropriate for hand analysis– Verification (& optimization)

• Design:– Small signal parameter design space:

• gm, CL (speed, noise)

• gm/ID, ID (power, output range, speed)

• Av0= gmro (gain)

– Device geometries from SPICE (table, graph);

– may require iteration (e.g. CGS)

Sweep V1Measure vgs

Intrinsic voltage gain of MOSFET

Intrinsic voltage gain = gm/go = vds/vgs for constant Id

Electronic Noise• Noise phenomena• Device noise models• Representation of noise (2-ports):

– Motivation– Output spectral density– Input equivalent spectral density– Noise figure– Sampling noise (“kT/C noise”)

• SNR versus Bits• Noise versus Power Dissipation

– Dynamic range– Minimum detectable signal

Noise in Devices and Circuits

•Noise is any unwanted excitation of a circuit, any input that is not an information-bearing signal.• External noise: Unintended coupling with other parts of the physical world; in principle, can be virtually eliminated by careful design.• Intrinsic noise: Unpredictable microscopic events inherent in the device/circuit; can be reduced, but never eliminated. •Noise is especially important to consider when designing low-power systems because the signal levels (typically voltages or currents) are small.

Noise vs random process variations

• random process variations– Variations from one device to another– For any device, it is fixed after fabrication

• Noise– Unpredictable variations during operation– Unknown after fabrication– Remains unknown after measurement during

operation– May change with environment

Time domain description of noise

What is signal and what is noise?

)()()( tntstx

srmsT

s PSrmsSdttsT

P )(,)(1

02

nrmsT

n PNrmsNdttnT

P )(,)(1

02

Signal and noise power:

Physical interpretation

power

If we apply a signal (or noise) as a voltage source across a one Ohm resistor, the power delivered by the source is equal to the signal power.

Signal power can be viewer as a measure of normalized power.

Signal to noise ratio

)(log20)(log10 1010rms

rms

n

s

N

S

P

PSNR

SNR = 0 dB when signal power = noise power

Absolute noise level in dB:w.r.t. 1 mW of signal power

)log(10dB30

mW1log10din

n

nmn

P

PP

B

SNR in bits• A sine wave with magnitude 1 has power

= 1/2.• Quantize it into N=2n equal levels between

-1 and 1 (with step size = 2/2n)• Quantization error uniformly distributed

between +–1/2n

• Noise (quantization error) power=1/3 (1/2n)2

• Signal to noise ratio = 1/2 ÷ 1/3 (1/2n)2 =1.5(1/2n)2 = 1.76 + 6.02n dB or n bits

-1<=C<=+1

C=0: n1 and n2 uncorrelatedC=1: perfectly correlated

Adding uncorrelated noises

Adding correlated noises

For independent noises

Frequency domain description of noise

T

TTn dttntn

TR )()(

2

1lim)(

))(()()( nnn RfSfPSD F

dffPSDP nn )(

dffPSDP nn )(0

Given n(t) stationary, its autocorrelation is:

The power spectral density of n(t) is:

For real signals, PSD is even. can use single sided spectrum: 2x positive side

↑ single sided PSD

)()( fXtx

dffXdttx

22)()(

)()( fPSDR xx

dffPSDRdttx xx

T

TT

)()0()(lim

2

Parseval’s Theorem:

If

If x(t) stationary,

Interpretation of PSD

PSDx(f)

Pxf1 = PSDx(f1)

Types of “Noise” • “man made”

– Interference– Supply noise– …– Use shielding, careful layout, isolation, …

• “intrinsic” noise– Associated with current conduction– “fundamental” –thermal noise– “manufacturing process related” – flicker noise

Thermal Noise • Due to thermal excitation of charge carriers in a

conductor. It has a white spectral density and is proportional to absolute temperature, not dependent on bias current.

• Random fluctuations of v(t) or i(t)• Independent of current flow• Characterization:

– Zero mean, Gaussian pdf– Power spectral density constant or “white” up to about

80THz

Thermal noise dominant in resisters

Example:R = 1kΩ, B = 1MHz, 4µV rms or 4nA rms

HW

Equivalently, we can model a real resistor with an ideal resistor in parallel with a current noise source. What rms value should the current source have?

Show that when two resistors are connected in series, we can model them as ideal series resistors in series with a single noise voltage source. What’s the rms value of the voltage source?

Show that two parallel resistors can be modeled as two ideal parallel resistors in parallel with a single noise current source. What’s the rms value of the current source?