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Allen and Holberg - CMOS Analog Circuit Design

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Allen and Holberg - CMOS Analog Circuit Design

Page V.1-7

EXAMPLES

1.What is the on resistance of an enhancement MOS switch if VS = 0V, VG = 10V, W/L = 1, VTO = 1V, and K' = 25µA/V2?

Assume that vDS 0V. Therefore,

RON

vDS

=

L/W

iD

K'(VG-VS -VT)

 

 

 

106

 

RON =

25(10-1) = 4444Ω

2.If VG=10V at t=0, what is the W/L value necessary to discharge C1 to

with 5% of its intial charge at t=0.1µS? Assume K'=25µA/V2

and VTO = 1V.

 

 

 

 

v(t)

=

5exp(-t/RC)

 

 

 

-7

 

 

 

10

-7

10

 

 

= 20

 

 

exp RC

 

RC = ln(20)

Therefore, R = 106 x 103Ω

VG

C2=10pF

+

5V+ - C1=20pF

-

Thus,

10x103

L/W

 

L/W

 

6

=

K'(VG-VS-VT)

=

(2.5x10-5)(9)

Gives

W

= 2.67

 

 

 

L

 

 

 

Allen and Holberg - CMOS Analog Circuit Design

Page V.1-8

INFLUENCE OF PARASITIC CAPACITANCES

MOSFET Model for Charge Feedthrough Analysis

Distributed Model

G

CGDO

CGSO

D

S

RCH

CGC=Cox

Simplified Distributed Model

 

G

CGDO

CGSO

Cox

Cox

2

2

D

S

RCH

CGSO = Voltage independent (1st-order), gate-source, overlap cap. CGDO = Voltage independent (1st order), drain-source overlap cap. CGC = Gate-to-channel capacitance (Cox)

RCH = Distributed drain-to-source channel resistance

Allen and Holberg - CMOS Analog Circuit Design

Page V.1-9

Charge Injection Sensitivity to Gate Signal Rate

Model:

vG

dvG

 

dt

+

 

vIN

CHold

-

Case 1 - Slow Fall Time:

Gate is inverted as vG goes negative .

Channel time constant small enough so that the charge on CHold is absorbed

by vIN.

• When gate voltage reaches vIN+VT, the device turns off and feedthru occurs via the overlap capacitance.

Case 2 - Fast Fall Time:

Gate is inverted as vG goes negative.

Fall rate is faster than the channel time constant so that feedthru occurs via the channel capacitance onto CHold which is not absorbed by vIN.

Feedthru continues when vG reaches vIN+VT.

Total feedthru consists of that due to both the channel capacitance and the overlap capacitances.

Other Considerations:

Source resistance effects the amount of charge shared between the drain and the source.

The maximum gate voltage before negative transition effects the amount of charge injected.

Allen and Holberg - CMOS Analog Circuit Design

Page V.1-10

Intuition about Fast and Slow Regimes

To develop some intuition about the fast and slow cases, it is useful to model the gave voltage as a piecewise constant waveform (a quantized waveform) and consider the charge flow at each transition as illustrated below. In this figure, the range of voltage at CL illustrated represent the period while the transistor is on.

In both cases, the quantized voltage step is the same, but the time between steps is different. The voltage accross CL is observed to be an exponential whose time

constant is due to the channel resistance and channel capacitance and does not change from fast case to slow case.

vCL

V

Voltage vGATE

Time

(d)

V

Voltage

Time

(e)

Allen and Holberg - CMOS Analog Circuit Design

Page V.1-11

Illustration of Parasitic Capacitances

φ1

 

CGS

 

CGD

 

+

 

VSS

 

+vC1

 

 

 

V

C

C

C

BS

BD

1

 

IN

 

 

 

-

-

 

 

 

 

 

 

 

CGS and CGD result in clock feedthrough

CBS and CBD cause loading on the desired capacitances

Clock Feedthrough

Assume slow fall and rise times

φ1

Switch ON

 

φ1 Switch OFF

 

φ1

 

CGS

+

VSS

 

VIN

CBS

-

Clock signal couples through CGD on the rising part of signal when switch is off, but

V charges C1 to the right value regardless.

IN

Clock signal couples through CGD CGD on the falling part of the signal when the switch is off.

C1 +vC1

-

vC1

 

CGD

 

Δφ1

CGD

Δφ1

CGD

= -

 

 

-

 

= -

(vin + VT)

 

C1+CGD

 

 

C1

 

 

C1

Allen and Holberg - CMOS Analog Circuit Design Page V.1-12

EXAMPLE - Switched

Capacitor

Integrator (slow clock edge

regime)

 

 

 

φ

 

 

 

Switch ON

 

 

 

Switch OFF vIN+VT

 

 

 

 

 

 

Switch ON

 

VT

 

Switch OFF

 

T

 

 

φ

t1 t 2 t 3 t 4

φ2

 

1

 

 

 

M1

 

 

C2

 

 

M2

+

 

 

+

 

 

 

V

C

VSS

vOUT

SS

 

VIN

1

 

 

 

 

 

-

-

 

assuming: CGS1=CGS2=CGD1=CGD2 = CG

Net feedthrough on C1 at t2:

 

CG

 

 

 

 

 

 

VC1 = CG+C1 (VIN + VT)

 

 

 

 

 

CG

 

 

 

CG

 

VC1 = VIN

1

C +C

 

VT

C +C

 

 

 

1

G

 

 

G

1

At t3, additional charge has been added due to CGS overlap of M2 as φ2 goes positive. Note that M2 has not turned on yet.

CG

VC1 (t2-t3) = CG+C1 VT

Allen and Holberg - CMOS Analog Circuit Design

Page V.1-13

Giving at the end of t3 (before M2 turns on):

 

 

CG

 

VC1

= VIN 1C +C

 

 

 

1

G

+

Once M2 turns on (at t3 ), all of the charge on C1 is transferred to C2.

C1

C1

CG

 

VO = VC1

= VIN 1

 

 

C2

C2

 

C1+CG

+

Between times at t3 and t4 additional charge is transferred to C1 from the channel capacitance of M2.

 

 

Cch

 

 

 

 

 

VO (t3-t4)= C2 (Vclk VT)

 

The final change in Vout is:

 

 

 

 

 

C1

CG

 

Cch

 

VO = VIN

1

 

 

 

(Vclk VT)

C2

C1+CG

 

 

C2

 

 

 

 

 

 

 

C1

Ideally the output voltage change is VIN C2 so the error due to charge

feedthrough is:

 

 

 

 

 

 

 

VO (error) =

C1 CG

 

 

Cch

VIN

 

 

 

 

(Vclk VT)

 

C2 C1+CG

 

C2

 

Allen and Holberg - CMOS Analog Circuit Design

Page V.1-14

Rigorous Quantitative Analysis of Fast and Slow Regimes

Consider the gate voltage traversing from VH to VL (e.g., 5.0 volts to 0.0 volts, respectively) described in the time domain as

vG = VH Ut

(3)

When operating in the slow regime defined by the relationship

β V 2

HT >> U

2CL

where VHT is defined as

VHT = VH VS VT

the error (the difference between the desired voltage VS VCL) due to charge injection can be described as

(4)

(5)

and the actual voltage,

Allen and Holberg - CMOS Analog Circuit Design Page V.1-15

 

 

C c h

 

 

 

 

 

 

 

 

 

 

 

 

 

 

W · C G D 0 +

2

π U CL + W · C G D 0 (VS + VT VL )

 

Verror =

CL

 

 

(6)

 

 

 

 

2β

 

CL

 

In the fast swithing regime defined by the relationship

 

β V HT2

<< U

 

 

 

 

 

 

(7)

 

2CL

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

 

the error voltage is given in Eq. (8) below as

 

 

 

 

Cch

 

 

 

 

 

 

 

CGD0 +

 

 

 

β

3

 

 

2

 

 

CGD0

 

Verror =

 

 

 

VHT

 

CL

 

V H T

 

+

(VS + VT VL )

(8)

 

 

 

 

 

6U CL

CL

 

The following example illustrates the application of the charge-feedthrough model given by Eq’s. (3) through (8).

Example 4.1-1 Calculation of charge feedthrough error

Calculate the effect of charge feedthrough on the circuit shown in Fig. 4.1-9 where Vs = 1.0 volts, CL = 200 fF, W/L = 0.8 m/0.8 m, and VG is given for two cases illustrated below. Use model parameters from Tables 3.1-2 and 3.2-1. Neglect L and W effects.

5

Case 2

vG

Case 1

0

0.2 ns

10 ns

Time

Case 1:

The first step is to determine the value of U in the expression vG = VH - Ut

For a transition from 5 volts to 0 volts in 0.2 ns, U = 25 109

In order to determine operating regime, the following relationship must be tested.

Allen and Holberg - CMOS Analog Circuit Design

 

 

Page V.1-16

 

β V 2

 

 

 

 

β V

2

 

 

 

 

 

HT

>> U for slow

or

 

HT

<< U for fast

 

 

2CL

2CL

 

 

 

 

 

 

 

 

 

 

Observin g that there is a backbias on the transistor switch effecting VT, VHT is

giving

VHT = VH - VS - VT = 5 - 1 - 0.887 = 3.113

 

 

 

β VHT2

 

 

 

 

 

 

 

 

 

 

 

=

110×10-6× 3.1132

2.66 × 109 << 25 × 109 thus fast regime.

 

2CL

 

2 × 200f

 

=

 

 

 

 

 

 

 

 

 

 

Applying Eq. (8) for the fast regime yields

 

 

 

 

 

 

 

 

1.58×10-15

 

3.32×10-3

176×10-18

 

Verror

176×10-18 +

2

 

 

 

 

=

 

200×10-15

 

3.113 -

+

200×10-15

(5 + 0.887 - 0)

 

 

 

 

 

 

30×10-3

 

 

Verror = 19.7 mV

Case 2:

The first step is to determine the value of U in the expression

v G = VH - Ut

For a transition from 5 volts to 0 volts in 10 ns, U = 5 × 108 thus indicating the slow regime according to the following test

2.66 × 109 >> 5 × 108

 

 

1.58×10-15

314×10-6

 

176×10-18

 

176×10-18 +

2

 

 

 

Verror =

200×10-15

 

220×10-6

+

200×10-15

(5 + 0.887 - 0 )

 

 

 

 

Verror = 10.95 mV

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