high speed op-amp design: compensation and topologies for...

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Distinguished Lecture IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 1 High Speed Op-Amp Design: Compensation and Topologies for Two and Three Stage Designs R. Jacob (Jake) Baker (UNLV, [email protected] ) Abstract : As CMOS technology continues to evolve, the supply voltages are decreasing while at the same time the transistor threshold voltages are remaining relatively constant. Making matters worse, the inherent gain available from the nano- CMOS transistors is dropping. Traditional techniques for achieving high gain by vertically stacking (i.e. cascoding) transistors becomes less useful in sub-100nm processes. Horizontal cascading (multi-stage) must be used in order to realize op-amps in low supply voltage processes. This seminar discusses new design techniques for the realization of multi-stage op-amps. Both single- and fully-differential op-amps are presented where low power, small VDD, and high speed are important. The proposed, and experimentally verified, op-amps exhibit significant improvements in speed over the traditional op-amp designs while at the same time having smaller layout area.

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Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 1

High Speed Op-Amp Design: Compensation and Topologies for Two and Three Stage Designs

R. Jacob (Jake) Baker (UNLV, [email protected])

Abstract :

As CMOS technology continues to evolve, the supply voltages are decreasing while at the same time the transistor threshold voltages are remaining relatively constant. Making matters worse, the inherent gain available from the nano-CMOS transistors is dropping. Traditional techniques for achieving high gain by vertically stacking (i.e. cascoding) transistors becomes less useful in sub-100nm processes. Horizontal cascading (multi-stage) must be used in order to realize op-amps in low supply voltage processes. This seminar discusses new design techniques for the realization of multi-stage op-amps. Both single- and fully-differential op-amps are presented where low power, small VDD, and high speed are important. The proposed, and experimentally verified, op-amps exhibit significant improvements in speed over the traditional op-amp designs while at the same time having smaller layout area.

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 2

Outline

q Introduction q Two-stage Op-Amp Compensation q Multi-stage Op-Amp Design q Multi-stage Fully-Differential Op-Amps q Conclusion

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 3

Op-Amps and CMOS Scaling

q The Operational Amplifier (op-amp) is a fundamental building block in Mixed Signal design. ü  Employed profusely in data converters, filters, sensors, drivers etc.

q Continued scaling in CMOS technology has been challenging the established paradigms for op-amp design.

q With downscaling in channel length (L) ü  Transition frequency increases (more speed). ü Open-loop gain reduces (lower gains). ü  Supply voltage is scaled down (lower headroom) [1].

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 4

CMOS Scaling Trends

q VDD is scaling down but VTHN is almost constant. ü Design headroom is shrinking faster.

q Transistor open-loop gain is dropping (~10’s in nano-CMOS) ü  Results in lower op-amp open-loop gain. But we need gain!

q Random offsets due to device mismatches. [3], [4].

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 5

Integration of Analog into Nano-CMOS?

q Design low-VDD op-amps. ü  Replace vertical stacking (cascoding) by horizontal cascading of gain

stages (see the next slide).

q Explore more effective op-amp compensation techniques. q Offset tolerant designs. q Also minimize power and layout area to keep up with the

digital trend. q Better power supply noise rejection (PSRR).

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 6

Cascoding vs Cascading in Op-Amps A Telescopic Two-stage Op-Amp

A Cascade of low-VDD Amplifier Blocks.

(Compensation not shown here)

1

VDD VDD

Vbiasn

vp vm

VDD

CL

vout

2

VDD VDD

Vbiasn

VDD VDD

Vbiasn

n-1

n

Stage 1 Stage 2 Stage (n-1) Stage n

VDDmin>4Vovn+Vovp+VTHP with wide-swing biasing. [1]

VDDmin=2Vovn+Vovp+VTHP.

q  Even if we employ wide-swing biasing for low-voltage designs, three- or higher stage op-amps will be indispensable in realizing large open-loop DC gain.

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 7

TWO-STAGE OP-AMP COMPENSATION

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 8

Direct (or Miller) Compensation

1

2

vm vp vout

Vbias4

Vbias3

CC 10pF

Unlabeled NMOS are 10/2.Unlabeled PMOS are 22/2.

VDD VDD VDD

30pF

CL

M3 M4

M1 M2

M6TL

M6BL

M6TR

M6BR

M8T

M8B

M7

220/2

100/2

100/2

x10

750Ω

iC fb

iC ff

q  Compensation capacitor (Cc) between the output of the gain stages causes pole-splitting and achieves dominant pole compensation.

q  An RHP zero exists at ü  Due to feed-forward component of

the compensation current (iC). q  The second pole is located at q  The unity-gain frequency is

v All the op-amps presented have been designed in AMI C5N 0.5µm CMOS process with scale=0.3 µm and Lmin=2. The op-amps drive a 30pF off-chip load offered by the test-setup.

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 9

Drawbacks of Direct (Miller) Compensation

q  The RHP zero decreases phase margin ü  Requires large CC for

compensation (10pF here for a 30pF load!).

q  Slow-speed for a given load, CL.

q  Poor PSRR ü  Supply noise feeds to the output

through CC. q  Large layout size.

1

2

vm vp vout

Vbias4

Vbias3

CC

10pF

Unlabeled NMOS are 10/2.Unlabeled PMOS are 22/2.

VDD VDD VDD

30pFCL

M3 M4

M1 M2

M6TL

M6BL

M6TR

M6BR

M8T

M8B

M7

220/2

100/2

100/2

x10

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 10

Indirect Compensation

q  The RHP zero can be eliminated by blocking the feed-forward compensation current component by using ü  A common gate stage, ü  A voltage buffer, ü  Common gate “embedded” in the

cascode diff-amp, or ü  A current mirror buffer.

q  Now, the compensation current is fed-back from the output to node-1 indirectly through a low-Z node-A.

q  Since node-1 is not loaded by CC, this results in higher unity-gain frequency (fun).

An indirect-compensated op-amp using a common-gate stage.

1

2

Unlabeled NMOS are 10/2.Unlabeled PMOS are 22/2.

VDD VDD VDD

30pF

220/2

100/2

100/2

x10

VDD

Vbias3

Vbias4

vm

vp

voutCc

CL

ic

MCGA

M3 M4

M1

M6TL

M6BL

M6TR

M6BR

M8T

M8B

M7

M2

M9

M10T

M10B

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 11

Indirect Compensation in a Cascoded Op-Amp

1

2

vm vp voutCC

1.5pF

Unlabeled NMOS are 10/2.Unlabeled PMOS are 44/2.

VDD VDD

VDD

30pFCL

Vbias2

Vbias3

Vbias4

A

50/2

50/2

110/2

M1 M2

M6TL

M6BL

M6TR

M6BR

M3T

M3B

M4T

M4B

M8T

M8B

M7

ic

Indirect-compensation using cascoded current mirror load.

1

2vm vp

voutCC

1.5pF

Unlabeled NMOS are 10/2.Unlabeled PMOS are 22/2.

VDD VDD

VDD

30pF

CL

Vbias3

Vbias4

A

100/2

100/2

220/2

M1B M2B

M5T

M5B

M3

M1T

M4

M2T

M8T

M8B

M7

VDD

M4Vbias1

30/2

30/2

10/10

ic

Indirect-compensation using cascoded diff-pair.

q  Employing the common gate device “embedded” in the cascode structure for indirect compensation avoids a separate buffer stage. ü  Lower power consumption. ü  Also voltage buffer reduces the swing which is avoided here.

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 12

Analytical Modeling of Indirect Compensation

A1 A2

Cc

1 2

vin vout

DifferentialAmplifier Gain Stage

RcA

ic

Block Diagram

Small signal analytical model

RC is the resistance attached to node-A.

icvoutsCc Rc

≈+1

+

-

+

-

1 2

gm1vs gm2v1R1 C1 R2 C2 vout

Cc

Rc

The compensation current (iC) is indirectly fed-back to node-1.

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 13

Derivation of the Small-Signal Model

The small-signal model for a common gate indirect compensated op-amp topology is approximated to the simplified model seen in the last slide.

Resistance roc is assumed to be large.

gmc>>roc-1, RA

-1, CC>>CA

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 14

Analytical Results for Indirect Compensation

σz1

−ω un

p1p2p3

Pole-zero plot

q  Pole p2 is much farther away from fun. ü  Can use smaller gm2=>less power!

q  LHP zero improves phase margin. q  Much faster op-amp with lower

power and smaller CC. q  Better slew rate as CC is smaller.

LHP zero

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 15

Indirect Compensation Using Split-Length Devices

q  As VDD scales down, cascoding is becoming tough. Then how to realize indirect compensation as we have no low-Z node available?

q  Solution: Employ split-length devices to create a low-Z node. ü  Creates a pseudo-cascode stack but its really a single device.

q  In the NMOS case, the lower device is always in triode hence node-A is a low-Z node. Similarly for the PMOS, node-A is low-Z.

A

VDD M1T

W/L1

M1BW/L2

M1W/(L1+L2)

Equivalent

M1T

W/L1

M1BW/L2

M1W/(L1+L2)

VDD Triode

Triode

Low-Z node

Low-Z node

EquivalentA

NMOS PMOS Split-length 44/4(=22/2)

PMOS layout

S

D

A

Low-Z node

G

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 16

Split-Length Current Mirror Load (SLCL) Op-Amp

1

2

vm vp vout

Vbias4

Vbias3

CC

2pF

Unlabeled NMOS are 10/2.Unlabeled PMOS are 22/2.

VDD VDD VDD

30pFCL

M3B M4B

M1 M2

M6TL

M6BL

M6TR

M6BR

M8T

M8B

M7T

M3T M4T

M7B

50/2

50/2

220/2

220/2

Aic

funz1

p2,3

q  The current mirror load devices are split-length to create low-Z node-A.

q  Here, fun=20MHz, PM=75° and ts=60ns.

ts

Frequency Response

Small step-input settling in follower configuration

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 17

SLCL Op-Amp Analysis

12vout

A

1gmp

id1id2vs2

1gmp

gm vs12

+-

−vs2

CL

Cc

v=0

12vout

A

1gmp

id1vs2

CL

Cc

−gg vm

mp s1

(a) (b)

+

-

+

-

1 2

gm2v1R1 C1vout

Cc

v1

rop

CA

+

-vsgA

C2R2

A

−gg vm

mp s1

1gmp

gmpvsgA

icvout

sCc gmp

≈+1 1

+

-

+

-

1 2

gm2v1R1 C1vout

Cc

v1C2R2ic

gm vs1 1gmp

gm vs12

1gmp

q  Here fz1=3.77fun ü  LHP zero appears at a higher

frequency than fun.

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 18

Split-Length Diff-Pair (SLDP) Op-Amp

q  The diff-pair devices are split-length to create low-Z node-A.

q  Here, fun=35MHz, PM=62°, ts=75ns. q  Better PSRR due to isolation of node-A

from the supply rails.

Frequency Response

Small step-input settling in follower configuration

1

2

vm vpvout

Vbias4

Vbias3

CC2pF

Unlabeled NMOS are 10/2.Unlabeled PMOS are 22/2.

VDD VDD VDD

30pF

CL

M3 M4

M1B M2B

M6TL

M6BL

M6TR

M6BR

M8T

M8B

M7

M1T M2T20/2

20/2

20/2

20/2

ic

110/2

50/2

50/2

A fun

p2,3

z1

ts

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 19

SLDP Op-Amp Analysis

12vout

A

id1id2vs2

−vs2

CL

Cc

v=0

1gmn

1gmn

12vout

A

id2 vs2

CL

Cc1gmn

rop

(a) (b)

idgmnvs

2 4= −

q  Here fz1=0.94fun, ü  LHP zero appears slightly before

fun and flattens the magnitude response.

ü  This may degrade the phase margin.

q  Not as good as SLCL, but is of great utility in multi-stage op-amp design due to higher PSRR.

+

-

+

-

1 2

gm2v1CAvoutvA

ron

C1

+

-vgs1

C2R2

A

gmnvgs1vs2

1gmn R1gmnvs

4

Cc

1gmn

icvout

sCc gmn

≈+1 1

+

-

+

-

1 2

gm2v1R1 C1vout

Cc

v1C2R2ic

gmnvs2 1

gmn

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 20

Test Chip 1: Two-stage Op-Amps

Miller 3-Stage Indirect

SLCL Indirect

SLDP Indirect

Miller with Rz

q  AMI C5N 0.5µm CMOS, 1.5mmX1.5mm die size.

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 21

Test Results and Performance Comparison

vin

vout

vin

vout

vin

vout

Miller with Rz (ts=250ns)

SLCL Indirect (ts=60ns)

SLDP Indirect (ts=75ns)

Performance comparison of the op-amps for CL=30pF.

q  10X gain bandwidth (fun). q  4X faster settling time. q  55% smaller layout area. q  40% less power consumption.

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 22

MULTI-STAGE OP-AMP DESIGN

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 23

Three-Stage Op-Amps

q  Higher gain can be achieved by cascading three gain stages. ü  ~100dB in 0.5µm CMOS

q  Results in at least a third order system ü  3 poles and two zeros. ü  RHP zero(s) degrade the phase

margin. q  Hard to compensate and stabilize. q  Large power consumption compared

to the two-stage op-amps.

zLHP

s plane

σp1p2,3

zRHP

−ωun

Clustered non-dominant poles

Pole-zero plot

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 24

Biasing of Multi-Stage Op-Amps

1

VDD VDD

Vbiasn

vp vm

~Vbiasp

Vbiasp

M1 M2

M3L M3R

M4 M5

3

VDD

CL

vout

M12

M11

2

VDD VDD

Vbiasn

~Vbiasp Vbiasp

M6 M7

M8L M8R

M9 M10Current flowing in this branch is set

by Vbiasp.

q  Diff-amps should be employed in inner gain stages to properly bias second and third gain stages ü  Current in third stage is

precisely set. ü  Robust against large offsets. ü  Boosts the CMRR of the op-

amp (needed). q  Common source second stage

should be avoided. ü  Will work in feedback

configuration but will have offsets in nano-CMOS processes.

1

VDD VDD VDD

Vbiasn

vp vm

2

~Vbiasp

Vbiasp

Unknown Voltage level, can move up or down.

M1 M2

M3L M3R

M4 M5M6

M7

3

VDD

CL

vout

Current in this branch is unknownM8

M9

Robust Biasing

Fallible Biasing

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 25

Conventional Three-Stage Topologies

1

2

VDD VDD VDD VDD VDD VDD

CL

vm vp voutCc1

Cc2

Rc

VB1

VB2

VB4VB5

VB3gm1

gm2

gm3

3

40uA

10uA 10uA

10uA

10uA

100uA

100pF

q  Requires p3=2p2=4ωun for stability (Butterworth response) ü  Huge power consumption

q  RHP zero appears before the LHP zero and degrades the phase margin.

q  Second stage is non-inverting ü  Implemented using a current

mirror. ü  Excess forward path delay (not

modeled or discussed in the literature).

-A1 +A2

Cc1

1 2

vs vout -A33

Cc2

Nested Miller Compensation (NMC) [6]

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 26

Conventional Three-Stage Topologies contd.

gm1 +gm2

Cc1

1vs vout -gm3

Cc2

2 3

-gmf1

-gmf2

q  Employs feed-forward gm’s to eliminate zeros. ü  gmf1=gm1 and gmf2=gm2

q  Class AB output stage. q  Hard to implement gmf1 which

tracks gm1 for large signal swings. ü  Also wasteful of power.

q  gmf2 is a power device and will not always be equal to gm2. ü  Compensation breaks down.

q  Still consumes large power.

Nested Gm-C Compensation (NGCC) [7]

1

2

3

VDD

vm vpgm1

VDD VDD VDD VDD

VB1

VDD

20uA

Cc1

VB2

CL

voutCc2

gm2gmf1

gm3

gmf224/3

60/3

120/3 180/3120/3

24/3 24/3

48/3

48/3

120/3

48/3

420/3

24/3

20uA 70uA

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 27

Conventional Three-Stage Topologies contd.

q  Four poles and double LHP zeros ü  One LHP zero z1 cancels the pole p3.

ü  Other LHP zero z2 enhances phase margin.

q  Set p2=2ωun for PM=60°. q  Relatively low power. q  Still design criterions are complex. q  Complicated bias circuit.

ü  More power. q  Excess forward path delay.

Transconductance with Capacitive Feedback Compensation (TCFC) [14]

1

2

VDD VDD VDD VDD VDD VDD

vm vp

vout

CC2

VB1

VB3

VB7

VB2gm1

gm3

3

gm2/2gmf

VB4

VB5

1:2

VB6gmt

CC1

-A1 +A21 2

vs vout -A33

CC2

-gmf

+gmt

CC1

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 28

Three-Stage Topologies: Latest in the literature

q  Employs reverse nesting of compensation capacitors ü  Since output is only loaded by only

CC2, results in potentially higher fun. ü  Third stage is always non-inverting.

q  Uses pole-zero cancellation to realize higher phase margins.

q  Excess forward path delay. q  Biasing not robust against process

variations. How do you control the current in the output buffer?

Reverse Nested Miller with Voltage Buffer and Resistance (RNMC-VBR) [8]

-A1 -A2

Cc1

1 2

vs vout +A33

Cc2

Rc2

Rc1CG

1

VDD

vm vpgm1

VDD

20uA

23

VDD VDD VDD VDD

vout

CL

Cc1

Cc2

gm2

gm3

gmf

gmVB

RC1

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 29

Three-Stage Topologies: Latest in the literature contd.

q  Reversed nested with elimination of RHP zero. ü  High gain block (HGB) realizes gain

by cascading stages. ü  High speed block (HSB) implements

compensation at high frequencies. q  Complex design criterions. q  Excess forward path delay. Again,

uses a non-inverting gain stage. q  Employs a complicated bias circuit.

ü  More power consumption.

Active Feedback Frequency Compensation (AFFC) [9]

-A1 +A2

Ca

1 2

vs vout -A33

Cm

-gmf

+gma

High-Gain Block (HGB)

High-Speed Block (HSB)

Input Block

1

2

VDD VDD VDD VDD VDD VDD

vm vp vout

Cm

VB

VB2

VB5

VB1gm1

gm3

3

gm2 gmf

VDD

VB1

VB4

Ca

gma

HGB HSB

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 30

Three-Stage Topologies: Latest in the literature contd.

q  Various topologies have been recently reported by combining the earlier techniques. ü  RNMC feed-forward with nulling resistor (RNMCFNR) [17]. ü  Reverse active feedback frequency compensation (RAFFC) [17].

q  Further improvements are required in ü  Eliminating excess forward path delay arising due to the compulsory non-

inverting stages. ü  Robust biasing against random offsets in nano-CMOS. ü  Further reduction in power and circuit complexity. ü  Better PSRR.

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 31

Indirect Compensation in Three-Stage Op-Amps

q  Indirectly feedback the compensation currents ic1 and ic2. ü  Reversed Nested

q  Thus named RNIC.

q  Employ diff-amp stages for robust biasing and higher CMRR.

q  Use SLDP for higher PSRR. q  Minimum forward path delay. q  No compulsion on the polarity of gain

stages. ü  Can realize any permutation of stage

polarities by just changing the sign of the fed-back compensation current using ‘fbr’ and ‘fbl’ nodes.

q  Low-voltage design. q  Note Class A (we’ll modify after

theory is discussed).

-A1 +A2

Cc1

1 2

vs voutic1

-A33

Cc2

ic2-

+

VDD VDD VDD

Vbiasn

vpfbl fbr

Cc2

CL

vm

VDD VDD

voutCc1

fbl

fbr

+ve

-ve

ic1

ic2

1

2

3

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 32

Indirect Compensation in Three-Stage Op-Amps contd.

VDD VDD VDD

Vbiasn

vpfbl fbr

Cc2

CL

vm

VDD VDD

voutCc1

fbl

fbr

+ve

-ve

ic1

ic2

1

2

3

q  Note the red arrows showing the node movements and the signs of the compensation currents. ü  fbr and fbl are the low-Z nodes used for indirect compensation (have

resistances Rc1 and Rc2 attached to them). q  The CC’s are connected across two-nodes which move in opposite

direction for overall negative feedback the compensation loops. q  Note feedback and forward delays!

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 33

Analysis of the Indirect Compensated 3-Stage Op-Amp

iv

sCc Rc c12

1 11≈ +

+

-

+

-

1 2

gm1vs gm2v1R1 C1 R2

C2v2

Cc1

Rc1

v1

+

-

3

gm3v2 R3

C3 vout

Cc2

Rc2

iv

sC Rcout

c c2 2 21≈ +

ic1 ic2

Two LHP zeros Four non-dominant poles.

q  Plug in the indirect compensation model developed for the two-stage op-amps.

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 34

Pole-zero Cancellation q  Poles p4,5 are parasitic conjugated poles located far away in frequency.

ü  Appear due to the loading of the nodes fbr and fbl.

q  The small signal transfer function can be written as

q  The quadratic expression in the denominator describing the poles p2 and p3 can be canceled by the numerator which describes the LHP zeros. ü  Results in LHP zeros z1 and z2 canceling the poles p2 and p3 resp.

q  The resulting expression looks like a single pole system for low frequencies. →Phase margin close to 90°.

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 35

Pole-zero Cancellation contd.

s plane

σp1

p2,z1−ωun

p3,z2

Non-dominant pole zero doublets

p4,5

Design Equations

q  Place pole-zero doublets (p2-z1 and p3-z2) out of fun for clean transients. ü  i.e. fp2, fp3 > fun.

q  Best possible pole-zero arrangement for low power design.

q  Results into design equations independent of parasitics (C3≈CL here).

q  Rc1 and Rc2 are realized by adding poly R’s in series with CC1 and CC2. ü  Also Rc1, Rc2≥Rc0, the impedance

attached to the low-Z nodes fbr/fbl. q  Robust against even 50% process

variations in R’s and C’s as long as the pole-zero doublets stay out of fun.

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 36

Pole-zero cancelled Class-A Op-Amp

Unlabeled NMOS are 10/2.Unlabeled PMOS are 22/2.

VDD VDD VDD

30pF

20/2

20/2

20/2

20/2

Vbiasn

vpfbl fbr

220/2

100/2

CL

vm

VDD VDD

vout

1

2

3

M4 M5

M1T

M1B

M2T

M2B

M3L M3R M7L M7R

M8 M9

M5 M6

M10

M11

Cc2fbr

R2c

Cc1

fblR1c

30/2 30/2

7.65K

4.08K

1p

2p

q  A Here, the poly resistors are estimated as

q  Low power, simple, robust and manufacturable topology*. v  The presented three-stage op-amps have been designed with transient and SR performances to

be comparable to their two-stage counterparts.

Distinguished Lecture

IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 37

Pole-zero cancelled Class-AB Op-Amp 1

q  A dual-gain path, low-power Class-AB op-amp topology (RNIC-1).

q  The design equation for Rc1 is modified as

Unlabeled NMOS are 10/2.Unlabeled PMOS are 22/2.

VDD VDD

VDD

30pF

20/2

20/2

20/2

20/2

Vbiasn

vpfbl fbr

220/2

100/2

Cc2 CL

vm

VDD VDD

vout

Cc1

fblfbr

1

2

3

M4 M5

M1T

M1B

M2T

M2B

M3L M3R M7L M7R

M8 M9

M5 M6

M10

M11

R1cR2c

Vbiasp

66/2 66/2

124 1p 2p1.14K

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IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 38

Pole-zero cancelled Class-AB Op-Amp 2

q  A single-gain path, Class-AB op-amp topology for good THD performance. ü  Floating current source for biasing the output buffer. ü  Here, Vncas= 2VGS and Vpcas=VDD - 2VSG. ü  Note the lack of gratuitous forward delay.

Unlabeled NMOS are 10/2.Unlabeled PMOS are 22/2.

VDD VDD

VDD

30pF

20/2

20/2

20/2

20/2

Vbiasn

vpfbl fbr

220/2

100/2

CL

vm

VDD VDD

vout

1

2

3

M4 M5

M1T

M1B

M2T

M2B

M3L M3R M7L M7R

M8 M9

M5 M6

M10

M11

Vbiasp

66/2 66/2

Vbiasn

VDD

Vpcas

Vncas

10/211/2

MFCP

MFCNCc1

fblR1c

Cc2fbr

R2c

7.65K

4.08K

1p

2p

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IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 39

Simulation of Three-stage Op-Amps

-150

-100

-50

0

50

100

Mag

nitud

e (d

B)

102 104 106 108 1010-225

-180

-135

-90

-45

0

Phas

e (d

eg)

Bode Diagram

Frequency (Hz)

q  Analytical model of the Class-AB (RNIC-1) topology is simulated in MATLAB.

q  The pole-zero plot illustrates the double pole-zero cancelation (collocation). ü  p4 and p5 are parasitic poles located at frequencies close to that of the fT limited

(or mirror) poles. q  Here, fun≈30MHz and PM=90° for CL=30pF.

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IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 40

Simulation of Three-stage Op-Amps contd.

q  SPICE simulation of the same Class AB op-amp. q  CL=30pF: fun=30MHz, PM≈88°, ts=70ns, 0.84mW, SR=20V/µs. q  As fast as a two-stage op-amp with only 20% more power, at 50% VDD and with

the same layout area (simpler bias circuit). q  Operates at VDD as low as 1.25V in a 5V process (25% of VDD). q  SPICE simulation match with the MATLAB simulation

ü  Our theory for three-stage indirect compensation is validated.

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IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 41

Chip 2: Low-VDD 3-Stage Op-Amps

PZC Class AB CL=30pF

PZC Class A CL=30pF

Class A CL=30pF

PZC Class AB Dual gain path

CL=500pF

PZC Class AB Single gain path

CL=500pF

PZC High Performance

Class AB CL=500pF Best

Performance

q AMI C5N 0.5µm CMOS, 1.5mmX1.5mm die size.

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Performance Comparison

q  Figures of Merit ü  FoMS=funCL/Power ü  FoML=SR.CL/Power ü  IFoMS=funCL/IDD

ü  IFoML=SR.CL/IDD

q  RNIC op-amp designed for 500pF load for a fair comparison.

q  FoMs>2X than state-of-the-art at VDD=3V.

q  Comparable performance even at lower VDD=2V.

q  Practical, stable and production worthy.

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Performance Comparison contd.

0

10000

20000

30000

40000

50000

60000

MNMCNGCC

NMCFNR

DFCFCAFFC

ACBCFTCFC

DPZCF

RNMC VB NR

SMFFC

RNMCFNR

RAFFC

RAFFC LP

RNIC-2

(This w

ork)

RNIC-3

(This w

ork)

RNIC-2A

(This

work

)

RNIC-3A

(This

work

)

FOM_S

FOM_L

IFOM_S

IFOM_L

q  Higher performance figures than state-of-the-art.

q  10X faster settling. q  Better phase margins. q  Layout area same or smaller.

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Flowchart for RNIC Op-Amp Design Start with the initial

specifications on fun, CL, Av, and SR.

Select the overdrive (% of VDD) which will set VGS, fT and transistor gain gm*ro.

Identify gm1. Can initially set gm2 equal to gm1 or a to lower value.

Select Cc2 = gm1/fun

Select Cc1 and gm3 such that the p2-z1 and p3-z2 doublet locations are outside fun.

Calculate R1c and R2c.

Is either of R1c and R2c negative?

Are the parasitic poles p4,5 degrading

PM by closing on fun?

Simulate the design for frequency response

and transient settling.

Does the design meet the

specifications?

No

Lower power?

Smaller layout area?

More Speed?

Better SR?

Split DC gain AOLDC across A1, A2 and A3.

Move the corresponding pi-zj doublet to a lower frequency by changing Cci and Rci. May

have to sacrifice fun.

Yes

End

Yes

Increase gm1 or decrease Cc2.

Yes

No

Decrease gm3 or gm2. In the worst case

scenario decrease gm1.

Yes

No

Reduce Cc1, Cc2 or gm3.

Yes

No

Increase bias current in the first stage (i.e. ISS1) or use

smaller CC’sYesNothing works!

Revisit biasing. No

Increase gm2.Yes

No

No

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IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 45

N-Stage Indirect Compensation Theory

A1 -A21 2

vs vout -A33

+-

-An-1 -Ann-1 n

Cc1

Cc2

Ccn−2

Ccn−1

ic1ic2

icn−1icn−2

q  The three-stage indirect compensation theory has been extended to N-stages and the closed form small signal transfer function is obtained.

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IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 46

MULTI-STAGE FULLY-DIFFERENTIAL OP-AMPS

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Fully Differential Op-Amps

q  Analog signal processing uses ‘only’ fully differential (FD) circuits. ü  Cancels switch non-linearities and even

order harmonics. ü  Double the dynamic range.

q  Needs additional circuitry to maintain the output common-mode level. ü  Common-mode feedback circuit

(CMFB) is employed.

CMFB

Vref

VCMFB

CL

CLvinm

vinp

vop

vom

vop-vom=-A(vinp-vinm)

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Three-Stage FD Op-Amp Design: Problems

-A1 +A2

Cc1

vp vop -A3

Cc2

-+ 1p 2p 3p

-A1 +A2

Cc1

vm vom -A3

Cc2

-+ 1m 2m 3m

CMFB vCM

q  The CMFB loop disturbs the DC biasing of the intermediate gain stages. ü  Degrades the gain, performance and may cause instability.

Unlabeled NMOS are 10/2.Unlabeled PMOS are 22/2.

VDD VDD

20/2

20/2

20/2

20/2

Vbiasn

vpfbl fbr

vm

VDD

20/2

20/2

VCM

vop1vom1

VCMFB1

VDD

vomCc2

fblR2c

110/2

100/2

50/2

VCMFB3

VDD

VDD

vopCc2

fbrR2c

110/2

100/2

50/2

VDD

VCM

30K

100f

30K

100f

vom

vop

VCM VCMFB1

vop2vom2

First Stage Second Stage

Output Buffer(Third Stage)

100/2 100/2

Cc1

VDD VDD

Vbiasn

VDD

vop2vom2 R1cfbr fbl

R1c

vop1 vom1 Vbiasp

Cc1

VDD

Block Diagram Circuit Implementation

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IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 49

Three-Stage FD Op-Amp Design: Solutions

-A1 +A2

Cc1

vp vop -A3

Cc2

-+ 1p 2p 3p

-A1 +A2

Cc1

vm vom -A3

Cc2

-+ 1m 2m 3m

CMFB vCM

CMFB vbiasn

CMFB vbiasp

v CMFB1

v CMFB2

v CMFB3

-A1 +A2

Cc1

vp vop -A3

Cc2

-+ 1p 2p 3p

-A1 +A2

Cc1

vm vom -A3

Cc2

-+ 1m 2m 3m

CMFB vCMvCMFB

-A1 +A2

Cc1

vp vop -A3

Cc2

-+ 1p 2p 3p

-A1 +A2

Cc1

vm vom -A3

Cc2

-+ 1m 2m 3m

CMFB vCMvCMFB

q  Employ CMFB 1.  Individually across all the stages. 2.  Only across the last two stages as the

biasing of the output buffer need not be precise.

3.  Only in the third stage (output buffer).

1.

2. 3.

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IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 50

Three-Stage FD Op-Amp Design

VDD VDD

20/2

20/2

20/2

20/2

Vbiasn

vpfbl fbr

vm

VDD

20/2

20/2

VCM

vop1vom1

Unlabeled NMOS are 10/2.Unlabeled PMOS are 22/2.

30K

100f

30K

100f

vom

vop

VCM VCMFB3

VDD VDD

Vbiasn

vop2

VDD VDD

Vbiasn

vom2Cc1

fblR1cCc1

fbrR1c

First Gain Stage

Second Gain Stage

VDD

vomCc2

fblR2c

110/2

100/2

50/2

VCMFB3

VDD

VDD

vopCc2

fbrR2c

110/2

100/2

50/2

VDD

VCM

vop2vom2

Output Buffer(Third Stage)

100/2 100/2

q  Use CMFB only in the output (third) stage. → Manufacturable design. ü  Leaves the biasing of second and third stage alone without disturbing them.

q  Employ diff-amp pairs in the second stage for robust biasing.

-A1 +A2

Cc1

vp vop -A3

Cc2

-+ 1p 2p 3p

-A1 +A2

Cc1

vm vom -A3

Cc2

-+ 1m 2m 3m

CMFB vCMvCMFB

Block Diagram Circuit Implementation

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IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 51

Three-Stage FD Op-Amp: Enlarged VDD VDD

20/2

20/2

20/2

20/2

Vbiasn

vpfbl fbr

vm

VDD

20/2

20/2

VCM

vop1vom1

Unlabeled NMOS are 10/2.Unlabeled PMOS are 22/2.

30K

100f

30K

100f

vom

vop

VCMFB3

VDD VDD

Vbiasn

vop2

VDD VDD

Vbiasn

vom2Cc1

fblR1cCc1

fbrR1c

First Gain Stage

Second Gain Stage

VDD

vomCc2

fblR2c

110/2

100/2

50/2

VCMFB3

VDD

VDD

vopCc2

fbrR2c

110/2

100/2

50/2

VDD

VCM

vop2vom2

Output Buffer(Third Stage)

100/2 100/2

VDD

Vbiasp

VCM

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Chip 3: Low-VDD FD Op-Amps

2-stage CL=30pFCMFB across all

the stages.

2-stage CL=30pFCMFB across the

output stage.

3-stage CL=30pFCMFB across the

output stage.

3-stage CL=30pFDiffamp pair for biasing

CMFB across the output stage.

3-stage CL=500pFDiffamp pair for biasing

CMFB across the output stage.

Best Performance

q AMI C5N 0.5µm CMOS, 1.5mmX1.5mm die size.

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Simulation and Performance Comparison DC behavior Transient response

82dB gain ts=275ns

q  >2.5X figure of merit (FoM).

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Flowchart for Three-Stage FD Op-Amp Design Start with the initial

specifications on fun, CL, Av, and SR.

Does the design meet specifications?

End

Yes

Design a singly-ended pole-zero cancelled three-stage op-amp for the given

specifications.

Add a CMFB circuit in the output buffer.

Convert the singly-ended op-amp into a fully differential one by mirroring it. Use a pair of

diff-pairs for the second stage for robust biasing.

Simulate the design.

NoUpdate the value of gm3 corresponding to the

output buffer and recalculate R1C and R2C.

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Conclusions

q  Indirect compensation leads to significantly faster, lower power op-amps with smaller layout area.

q  Indirect compensation using split-length devices facilitates low-VDD op-amp design.

q  Novel pole-zero canceled three-stage RNIC op-amps exhibit substantial improvement over the state-of-the-art.

q  A theory for multi-stage op-amps is presented. q  New methodologies for designing multi-stage FD op-amps proposed which

improve the state-of-the-art. q  All proposed op-amps are low voltage

ü  Open new avenues for low-VDD mixed signal system design.

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Future Scope

q  Mathematical optimization of PZC op-amps. q  Design of low-VDD systems in nano-CMOS process

ü  Pipelined and Delta-Sigma data converters, ü  Analog filters, ü  Audio drivers, etc.

q  Further investigation into indirect-compensated op-amps for n≥4 stages.

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IEEE Solid-State Circuits Society – Gonzaga, April 9-10, 2015 57

References

[1] Baker, R.J., “CMOS: Circuit Design, Layout, and Simulation,” 2nd Ed., Wiley Interscience, 2005. [2] Saxena, V., “Indirect Compensation Techniques for Multi-Stage Operational Amplifiers,” M.S. Thesis, ECE

Dept., Boise State University, Oct 2007. [3] The International Technology Roadmap for Semiconductors (ITRS), 2006 [Online]. Available: http://

www.itrs.net/Links/2006Update/2006UpdateFinal.htm [4] Zhao, W., Cao, Yu, "New Generation of Predictive Technology Model for sub-45nm Design

Exploration" [Online]. Available: http://www.eas.asu.edu/~ptm/ [5] Slide courtesy: bwrc.eecs.berkeley.edu/People/Faculty/jan/presentations/ASPDACJanuary05.pdf [6] Leung, K.N., Mok, P.K.T., "Analysis of Multistage Amplifier-Frequency Compensation," IEEE Transactions on

Circuits and Systems I, Fundamental Theory and Applications, vol. 48, no. 9, Sep 2001. [7] You, F., Embabi, S.H.K., Sanchez-Sinencio, E., "Multistage Amplifier Topologies with Nested Gm-C

Compensation," IEEE Journal of Solid State Circuits, vol.32, no.12, Dec 1997. [8] Grasso, A.D., Marano, D., Palumbo, G., Pennisi, S., "Improved Reversed Nested Miller Frequency Compensation

Technique with Voltage Buffer and Resistor," IEEE Transactions on Circuits and Systems-II, Express Briefs, vol.54, no.5, May 2007.

[9] Lee, H., Mok, P.K.T., "Advances in Active-Feedback Frequency Compensation With Power Optimization and Transient Improvement," IEEE Transactions on Circuits and Systems I, Fundamental Theory and Applications, vol.51, no.9, Sep 2004.

[10] Eschauzier, R.G.H., Huijsing, J.H., "A 100-MHz 100-dB operational amplifier with multipath Nested Miller compensation," IEEE Journal of Solid State Circuits, vol. 27, no. 12, pp. 1709-1716, Dec. 1992.

[11] Leung, K. N., Mok, P. K. T., "Nested Miller compensation in low-power CMOS design," IEEE Transaction on Circuits and Systems II, Analog and Digital Signal Processing, vol. 48, no. 4, pp. 388-394, Apr. 2001.

[12] Leung, K. N., Mok, P. K. T., Ki, W. H., Sin, J. K. O., "Three-stage large capacitive load amplifier with damping factor control frequency compensation," IEEE Journal of Solid State Circuits, vol. 35, no. 2, pp. 221-230, Feb. 2000.

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References contd.

[13] Peng, X., Sansen, W., "AC boosting compensation scheme for low-power multistage amplifiers," IEEE Journal of Solid State Circuits, vol. 39, no. 11, pp. 2074-2077, Nov. 2004.

[14] Peng, X., Sansen, W., "Transconductances with capacitances feedback compensation for multistage amplifiers," IEEE Journal of Solid State Circuits, vol. 40, no. 7, pp. 1515-1520, July 2005.

[15] Ho, K.-P.,Chan, C.-F., Choy, C.-S., Pun, K.-P., "Reverse nested Miller Compensation with voltage buffer and nulling resistor," IEEE Journal of Solid State Circuits, vol. 38, no. 7, pp. 1735-1738, Oct 2003.

[16] Fan, X., Mishra, C., Sanchez-Sinencio, "Single Miller capacitor frequency compensation technique for low-power multistage amplifiers," IEEE Journal of Solid State Circuits, vol. 40, no. 3, pp. 584-592, March 2005.

[17] Grasso, A.D., Palumbo, G., Pennisi, S., "Advances in Reversed Nested Miller Compensation," IEEE Transactions on Circuits and Systems-I, Regular Papers, vol.54, no.7, July 2007.

[18] Shen, Meng-Hung et al., "A 1.2V Fully Differential Amplifier with Buffered Reverse Nested Miller and Feedforward Compensation," IEEE Asian Solid-State Circuits Conference, 2006, p 171-174.

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Questions?