Lecture 21 Today we will Revisit the CMOS inverter, concentrating on logic 0 and logic 1 inputs Come up with an easy model for MOS transistors involved.

Lecture 21

Today we will Revisit the CMOS inverter, concentrating on logic 0

and logic 1 inputs Come up with an easy model for MOS transistors

involved in CMOS digital computation Investigate the “complementary” nature of CMOS

logic circuits Introduce CMOS NAND and NOR Determine the effective R and C for CMOS logic

transitions

D

S

VDD (Logic 1)

D

S

VOUT

VIN

VGS(n) = VIN

VGS(p) = VIN – VDD

VDS(n) = VOUT

+ VGS(n) -

+ V GS(p) -

+VDS(n)

_

CMOS Inverter

VDS(n)

(=VOUT)

ID(n)

VDD

NMOS I-V curve

PMOS I-V curve(written in terms of NMOS variables)

CMOS Analysis

VIN < VTH(n)

(e.g., logic 0)

As VIN goes up, VGS(n) gets biggerand VGS(p) gets less negative.

NMOS cutoff (open circuit)

PMOS triode (with VDS(p) = 0 V)

VDS(n)

(=VOUT)

ID(n)

VDD

NMOS I-V curve

PMOS I-V curve(written in terms of NMOS variables)

CMOS Analysis

VIN > VDD + VTH(p)

(e.g., logic 1)PMOS cutoff (open circuit)

NMOS triode (with VDS(n) = 0 V)

Model for Digital Computation

This leads us to a simpler model for transistors in CMOS circuits, when VIN is fully logic 0 or logic 1.

D

G

S

VGS = 0 VVGS = VDD (for NMOS)VGS = -VDD (for PMOS)

D

G

S

Transistor is cutoff.

Zero current flow.

Transistor is not cutoff, but zero current flow of partner transistor causes VDS = 0 V.

Practice

VOUT

VDD

VIN

= VDD

VOUT

VDD

VIN

= 0 V

Use this model to find VOUT for the circuits below.

CMOS NANDVDD

A

B

S

S S

S

PMOS1

NMOS1

PMOS2

NMOS2

AB

More Practice

Verify the logical operation of the CMOS NAND circuit:

VDD

A= 0V

S

S S

SB

= 0V

VDD

A= 0V

S

S S

SB

= VDD

More Practice

Verify the logical operation of the CMOS NAND circuit:

VDD

A= VDD

S

S S

SB

= 0V

VDD

A= VDD

S

S S

SB

= VDD

CMOS Networks

Notice that VOUT gets connected to either VDD or ground by “active” (not cutoff) transistors.

We say that these active transistors are “pulling up” or “pulling down” the output.

NMOS transistors = pull-down network PMOS transistors = pull-up network These networks had better be complementary or

VOUT could be “floating”—or attached to both VDD and ground at the same time.

CMOS NAND vs. NOR

VDD

A

B

S

S S

S

AB

VDD

A

B

S

S S

S

CMOS NOR

A+B

CMOS NAND

Complementary Networks

If inputs A and B are connected to parallel NMOS, A and B must be connected to series PMOS.

The reverse is also true. Determining the logic function from CMOS circuit is

not hard: Look at the NMOS half. It will tell you when the

output is logic zero. Parallel transistors: “like or” Series transistors: “like and”

Resistance and Capacitance

The separation of charge by the oxide insulator creates a natural capacitance in the transistor from gate to source.

The silicon through which ID flows has a natural resistance. There are other sources of capacitance and resistance too.

n-typemetal metaloxide insulator

metal

p-type

metal

gate

drain

n-type+ + + + + +

___

_

_ _

h hh h

- +

_ _ _

h

VGS > VTH(n)

h hh h h

e e e ee

Gate Delay—The Full Picture

Suppose VIN abruptly changed from logic 0 to logic 1.

VOUT1 may not change quickly, since is attached to the gates of the next inverter.

These gates must collect/discharge electrons to change voltage. Each gate attached to the output contributes a capacitance.

D

S

VDD

D

S

VOUT1

D

S

VDD

D

S

VOUT2

VIN

e

e

Gate Delay—The Full Picture

Where will these electrons come from/go to? No charges can pass through the cutoff transistor. Charges will go through the pull-down/pull-up transistors to

ground. These transistors contribute resistance.

D

S

VDD

D

S

VOUT1

D

S

VDD

D

S

VOUT2

VIN

e

e

Computing Gate Delay

1. Determine the capacitance of each gate attached to the output. These combine in parallel. Higher fan-out = more capacitance.

2. Determine which transistors are pulling-up or pulling-down the output. Each contributes a resistance, and may need to be combined in series and/or parallel.

3. The C from 1) and R from 2) are the RC for the VOUT1 transition.

D

S

VDD

D

S

VOUT1

D

S

VDD

D

S

VOUT2

VIN

tp = (ln 2)RC

Example

Suppose we have the following circuit:

If A and B both transition from

logic 1 to logic 0 at t = 0,

find the voltage at the NAND

output, VOUT(t), for t ≥ 0.

A

B

Logic 0 = 0 V

Logic 1 = 1 V

NMOS resistance

Rn = 1 k

PMOS resistance

Rp = 2 k

Gate capacitance

CG = 50 pF

Answer

A and B both transition from 0 to 1. Since VOUT comes out of a NAND of A with B, VOUT transitions from 1 to 0.

VOUT(0) = 1 V VOUT,f = 0 V Since the output is transitioning from 1 to 0, it is being pulled

down. Both NMOS transistors in the NAND were previously cutoff, but are now active. The NMOS in the NAND are in series, so the resistances add:

R = 2 RN = 2 k The output in question feeds into 2 logic gate inputs (one

inverter, one NOR). Each CMOS input is attached to two transistors. Thus we have 2 x 2 = 4 gate capacitances to charge. All capacitances are in parallel, so they add:

C = 4 CG = 200 pF

VOUT(t) = 0 + (1-0) e-t/(2 k 200 pF) V

VOUT(t) = e-t/(400 ns) V