High Bandwidth Low Power Operational Amplifier Design and...

62
High Bandwidth Low Power Operational Amplifier Design and Compensation Techniques Final Oral Master/ PhD Qualifier May 1 rst 2009 Vaibhav Kumar

Transcript of High Bandwidth Low Power Operational Amplifier Design and...

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High Bandwidth Low Power Operational Amplifier Design and Compensation

TechniquesFinal Oral Master/ PhD Qualifier

May 1rst 2009Vaibhav Kumar

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AbstractDevelopment of a new compensation technique forbandwidth extended Operational Amplifiers in scaledCMOS process

Proposed easy to follow Design Guideline for practicaldesign where power, speed and manufacturability arecritical

In comparison to state of the art performs up to 100times better in Figure of Merit (FOM)

10/20/2009 VAIBHAV KUMAR - IOWA STATE UNIVERSITY 2

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Agenda

• Introduction

• Literature Review

• Indirect Feedback Frequency Compensation

• Design Procedure and Specifications

• Simulation Results

• Analog Layout

• Future Research (part of PhD Qualifier)10/20/2009 3VAIBHAV KUMAR - IOWA STATE UNIVERSITY

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INTRODUCTION

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IntroductionThe Operational Amplifier (op-amp) is a fundamental building block in all electronic circuits

Employed profusely in data converters, filters, sensors, drivers etc…..

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Future Process TrendsContinued CMOS Scaling (pushing into the nanoscale arena) has been challenging the established paradigm for op amp design.Consequences due to downscaling in channel length for op amp design

Transition frequency (increased speed)

Open-loop gain reduction

Supply Voltage reduction (lower headroom)

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EBT L

Vf ∝

omEB

Lg r V∝

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Supply and Threshold Voltage Trends

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Figure 1: Supply voltage (Vdd) and threshold voltage (Vth) trends in future CMOS semiconductor processes technology (ITRS) [1]

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Transition Frequency Trends

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Figure 3: Transistor transition frequency (fT) trends in future CMOS semiconductor processes technology (ITRS) [1]

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Entering the NANO CMOS domainWhy do we need CMOS scaling ??

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Strongly driven by Digital VLSI Circuit NeedsGoals: in each Generation

2X increase in density1.5X increase in speed

What about “ANALOG SPEED” ??it is orders of magnitude behind digitalwhy??

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Analog Speed IssueAt the center of all analog circuits is an

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OPERATIONAL AMPLIFIER

β

Almost always used in Closed Loop Feedback Configuration

Need to worry about STABILITYof the closed loop system

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Applying the Lens of Stability

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Prevalent Compensation Techniques including Miller Compensation provide poor bandwidth efficiency

Result in OP-AMP which are very slow

Extending the OP-AMP bandwidth has been a pursuit for all analog designers

Research Goal of this work Find a practical way to increase bandwidth efficiency

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Integration of AMS into Nano CMOSBetter Op-Amp compensation TechniquesDesign low-VDD Op Amps

Replace vertical stacking of transistors (cascoding) by horizontal assembly of stages (cascading)

Better supply rejection noise (PSRR)Minimize

PowerLayout Area

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Effects of AMS Design being Squeezed with Scaling

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Reduced head room challenges compared to traditional AMS designs

Process Variation makes design centering tough

Raises the question for future Analog VDD scaling…

Figure 5: Effects of scaling down Analog Supplies

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LITERATURE REVIEW

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Traditional Op Amp Compensation TechniqueParallel Compensation

Capacitor is connected in parallel to the output resistance of gain stage of the Op Amp to modify pole

Pole Splitting (Single Miller Compensation)Slow speed (unless large bias and large devices are used) for a given load CL

Have the right half plane zeroPoor PSRRPoor Slewing

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-1/R2C2 -1/R1C2

pole splitting-1

gm2R2R1C1

-gm2C1+C2

gm2Cc

Direct (Miller) Compensation

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VsA2A1

Vout VsA2A1

Cc

Vout

Rout

AA

-gm1Vd

R1 C1

V1

-gm2V1

R2

CL

Vout

Cc

Ic=(vout-vs)1/sCc

Figure 7: Small Signal Model for SMC

Figure 6: Two Stage Miller Compensation

Figure 8: Pole Splitting effect of SMC

Transfer Function

Pole/Zero LocationsBandwidth Reduction

RHP Zero

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Miller CompensationCompensation capacitor is between the output of the two stage. This results in pole splitting between the dominant and non dominant poleA RHP zero exists at

Due to the feedforward component of the compensation current (Ic)

The second pole exists at

The unity gain frequency is at fun = gm1/2πCc

ISSUES WITH MILLER COMPENSATIONRHP zero reduces the phase margin of the amplifier and thus causes instability

Requires large Cc for stability Slow speed for a given load, CL

Poor PSRRSupply noise feeds through the compensation capacitor to the output

Requires large die area

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Miller Compensation with Zero Nulling ResistorA common method to cancel the RHP zero is by using a series resistor with compensation capacitorThe new location of the zero is

The resistor Rz can be implemented using a transistor in triode region

However introduces a third pole to the system

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Need More Stable Op AmpsWe can increase Rz and create a LHP zero to improve phase margin

Becomes difficult to manage the location of the Rz over temperature and process variations

Stability of the op amp is a becoming a problem because of the non-dominant pole associated with the output (f2) is too lowIncrease f2 requires increase of gm of the output stage

Increase areaIncrease output stage current (Id2)

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Need a more practical way to CompensateAvoid using Miller Compensation

Avoid connecting a compensation capacitor between two high impedance nodes !Literature has many examples illustrating how to avoid miller connections for high speed

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This research develops Indirect Feedback Frequency CompensationA more practical way to compensateFeedback compensation current indirectly using

Common Gate AmplifierCascoded Structures

Improved PSRRSmaller Die Area (Compensation capacitor reduced 4~10 times)Much Faster ..!

VsA2A1 Buffer

Cc

Differential Amplifier Gain Stage Output Buffer

Vout

iccRi

A

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Indirect Feedback - History• First proposed by B.K. Ahuja in “AN IMPROVED FREQUENCY COMPENSATION

TECHNIQUE FOR CMOS OPERATIONAL-AMPLIFIERS,” Ieee Journal of Solid-State Circuits, vol. 18, no. 6, pp. 629-633, 1983

• However it is still seldom used in practice ??• Looks very similar to Miller compensation• Prompts most designers to use design strategy for Miller-Rz compensation• However the Indirect Compensation Scheme has much different pole/zero

locations and conditions that need to be satisfied to tap the true potential of the compensation scheme

• Thus this work Provides analytical model/solution for the architectureProposes a design procedure based on the analytical resultsDesign Example using the proposed design procedureSimulation Results show the performance is orders of magnitude higher than miller compensation and far better than state of the art

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INDIRECT FEEDBACK FREQUENCY COMPENSATION

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Indirect Feedback Frequency Compensation

Improvements due to a simple changeThe compensation current is indirectly fedback from low impedance node VA to V1

The RHP pole zero can be eliminated as the feedforward current is blocked by the common gate amplifierNode V1 is now not loaded by the compensation capacitor (as previously) and thus results in a much faster second stage and increased unity gain frequency

AND MUCH MORE ………

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M1 M2

M3 M4

M5

M6c

VDD

VSS

Cc

Vin- Vin+

M9

ic

VA

V1

Mb3M7

Mb1

Isupply

Mb2

Mb4

Mb5 Mb6

Vout

Vbb

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Small Signal Analysis

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Cc

gm1Vd

R1 C1

V1 VA

gmcVA

roc

1/gmc RA CA gm5V1 R2CL

Vout

TAKING KCL AT EACHNODE

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Simplified Transfer Function

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The transfer function can be simplified and approximated as:-

The coefficients can be evaluated as

Evaluating the poles and zerosAssuming the pole |p1| >> |p2|, |p3|

The denominator can now beapproximated

Real Poles Complex Poles

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The third order transfer function as 3 poles and 1 zeroDominant Pole location

Non-dominant Real Poles locationCondition For Real Poles

LHP Zero Location

bserving the Pole/Zero Locations

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Remains at the same location

Large gmc ?

Improves Phase Margin

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Analytical Results Summary

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Pole / Zero Location

Real Poles Condition

Quick Facts

Pole p2 moved to much higher frequency

Can use much smaller gm5 Less Power

LHP zero improves the phase margin

Much faster op-amp with lower power and CC

Will EXPLORE more ….

Extended by a factor >1

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M1 M2

M3 M4

M5

VDD

VSS

Cc

Vin- Vin+

M9

ic

V1

M7Mb1

Isupply

Mc1 Mc2

Vbb

A

if

Vout

Vcc

Alternative Implementations of Indirect Feedback

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The common gate amplifier is embedded in the cascode actionSimilar to the common gate amplifier analyzed in the previous section, the LHP zero and the three poles are given by Equations provided previouslyReduction in Power at cost of Flexibility choosing the transconductance of gmc

M1 M2

M3 M4

M5

VDD

VSS

Cc

Vin- Vin+

M9

ic

V1

M7Mb1

Isupply

Mc1 Mc2

Vbb

A

Vout

Vcc

Similar to cascoded PMOS loadsHowever additional RHP zero located at:

RHP zeroHigh Frequency

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Summarizing the Advantages of Indirect Feedback

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Pole splitting can be achieved with a much smaller compensation capacitor (Cc)

Faster Op Amp Much Smaller Area

Lower Value of second stage transconductance (gm5) value required

Lower Power and Less Total Current Required

Improved PSRR

Analytically the reason the non-dominant pole shifted to a higher frequency is because the compensation capacitor now does not load the first stage output.

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DESIGN PROCEDURE AND SPECIFICATIONS

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Op Amp Design Dilemma

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Need a clear robust design procedure …

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Pre - Design Procedure Guidelines

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To quantify how good of a job our transistor does, we can therefore define the following “figure of merits (FOM)

Tranconductor Efficiency Transit Frequency

Good RegionFor AMI 0.5CNVEB ≈ 0.1-0.2 V

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Indirect Feedback Design Procedure Summary

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Noise Specification

Slew Rate Specification

Output Swing Specification

Gain-Bandwidth Requirement

Real Poles Requirement

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Class A Output Stage Design

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Bad Output Stage DesignNot Controlling current in the output stage leads to:

Bad input-referred offsetPotential for large power dissipationNot controlling output stage gm (and thus stability)

Class A output stages also suffer from poor slew rate

M1 M2

M3 M4

M5

M6c

VDD

VSS

Cc

Vin- Vin+

M9

ic

VA

V1

Mb3M7

Mb1

Isupply

Mb2

Mb4

Mb5 Mb6

Vout

Vbb

M1 M2

M3 M4

M5

VDD

Cc

V1

Mc1 Mc2Vbb

Vout

SR = inf

CLM1 M2

M3 M4

M5

VDD

Cc

V1

Mc1 Mc2Vbb

Vout

Iss2CL

SR =

CL

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Class AB Output Stage Design

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Class AB Output StageThe Class AB output stage is realized by have a floating current source biased between the output stages transistors behaving like a push pull:

Slew Rate Improved during dischargingControlled output stage current and gmSlew rate limitation shifted to the compensation capacitor which is small in the proposed compensation scheme and thus achieves much higher slew rate

M1 M2

M3 M4

M5

VDD

Cc

V1

Mc1 Mc2Vbb

Vout

CL

Mpcasc

M6

Mncasc

Iss2

M1 M2

M3 M4

M5

VDD

Cc

V1

Mc1 Mc2Vbb

Vout

CL

Mpcasc

M6

Mncasc

Iss2

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Figure of Merit (FOM)

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To perform a comparison in terms of speed among the many compensation approaches independently of the particular amplifier topology, design choices, and technology, a figure of merit (FOM) that relates the load capacitance CL, the gain-bandwidth product ωGBW, and the total current consumption of the amplifier I-Total has been proposed [ref].

Small Signal FOM

DC Transient FOM

Single Stage Comparison

Total TranscoductanceGm in multi-stage op amp

MHz pfmA•

V s pfmAµ •

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Design Example – Op Amp Specifications

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Op Amp Specification

Supply Voltages ± 1.25 V

Load Capacitance: CL 100 pF

Total Current (max) 30 μA

DC gain: Ao 70 dB

Unity-gain Frequency: fu 2 MHz

Phase Margin: φM 60°

Slew Rate: SR 1 V/μs

Input Common Mode Range: VCMR ± 1 V

Output Swing: Vout {max,min} ± 0.5 V

Input Referred Noise 15 nV/√Hz

Very Low Power

Large Load

Good Stability

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Design Example – Device Sizing

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Op Amp Sizing

Transistor Multiplier Size (μm)

M1,22 4.05/0.9

M3,42 3.6/2.4

M56 10.05/1.5

M612 15/1.05

M76 1.65/1.05

M9,b1110 1.65/4.05

Mb11 1.65/4.05

Mb21 1.65/1.05

Mb312 1.65/1.05

Mb41 2.4/1.05

Mb51 12/1.05

Mb612 12/1.05

Mb72 3/1.2

Mb81 1.65/1.05

Mb9,1010 1.95/0.6

Cc- 5 pF

Isupply- 1.25uA

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SIMULATION RESULTS

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Summary of Simulated Results

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Simulated Results

Specification Specifications Simulation

DC gain: Ao 70 dB 72.45 dB

Unity-Gain Frequency: fu 2 MHz 2.01 MHz

Phase Margin: φM 60° 61.83°

Slew Rate: SR+/- ± 1 V/μs 1/-2.45 V/μs

Input Common Mode Range:

VCMR + / VCMR=

± 0.5 V 1.1/-0.75 V

Output Swing:

Vout MAX/Vout MIN

± 1 V 1.14/-1.1

ITotal 30 μA 30 μA

Power - 75 μW

High Speed

+

Low Power

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AC Frequency Response (CL = 100pf)

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Bandwidth Extension

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Large Signal Transient Response (CL = 100pf)

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Sine Wave Transient Response (CL = 100pf)

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Robustness of Analytical Results

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Small Error

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Alternative Indirect Feedback Compensation Scheme Results

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Comparison of Alternative Indirect Feedback Compensation

Specification Common Gate Cascode NMOS Cascode

PMOS

DC gain: Ao 72.45 dB 91.1 dB 86.1 dB

Unity-Gain

Frequency: fu

2.01 MHz 1.99 MHz 2.2 MHz

Phase Margin: φM 61.83˚ 61.29˚ 61.7˚

M1 M2

M3 M4

M5

VDD

VSS

Cc

Vin- Vin+

M9

ic

V1

M7Mb1

Isupply

Mc1 Mc2

Vbb

A

Vout

Vcc

M1 M2

M3 M4

M5

VDD

VSS

Cc

Vin- Vin+

M9

ic

V1

M7Mb1

Isupply

Mc1 Mc2

Vbb

A

if

Vout

Vcc

M1 M2

M3 M4

M5

M6c

VDD

VSS

Cc

Vin- Vin+

M9

ic

VA

V1

Mb3M7

Mb1

Isupply

Mb2

Mb4

Mb5 Mb6

Vout

Vbb

Common Gate Cascode PMOSCascode NMOS

Improved gain dueTo cascoding

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Performance Comparison to Miller Compensation and Single Stage Amplifiers

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M1 M2

M3 M4

M5

M6c

VDD

VSS

Cc

Vin- Vin+

M9

ic

VA

V1

Mb3M7

Mb1

Isupply

Mb2

Mb4

Mb5 Mb6

Vout

Vbb

Indirect Feedback

Comparison with Miller Compensation and Single Stage Amplifiers

Specification Single Stage Single Miler

Compensation

Indirect Feedback

Compensation

DC gain: Ao 36.93 dB 70.45 dB 72.45

Unity-Gain

Frequency: fu

1.098 MHz 293.1 KHz 2.01 MHz

Phase Margin: φM 90˚ 60.29˚ 61.7˚

Cc Required -NA- 35 pF 5 pF

Miller CompensationSingle Stage

Winner

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Performance Comparison to Literature

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Conference Author Total Id (mA) GBW (MHz) Slew Rate (V/μs) CL (pf) IFOMs (MHz•pf)/mA IFOML ((V/μs)•pf)/mA

ECCTD -2007 [25] Pennisi 1.950 700.00 2000.00 0.3 107.69 307.69

TCAS - 2005 [24] Mahattanakul 0.076 5.00 6.00 5 330.69 396.83

WESEAS -2006 [26] Franz 12.800 1060.00 863.00 4 331.25 269.69

JCSC 2008 [27] Hamed 7.667 300.00 -NA- 8.5 332.61 -NA-

JSSC - 1995 [28] Kovacs 0.110 4.50 -NA- 10 409.09 -NA-

AICSP - 2009 [29] Pugliese 0.318 27.10 25.00 10 851.71 785.71

TCAS - 1997 [6] Palumbo 0.158 28.00 6.59 5 886.08 208.54

E-Letter 2007 [30] Pugliese 0.032 6.70 1.00 10 2125.96 317.31

ECCTD - 2005 [31] Loikkanen 0.210 6.80 6.40 200 6476.19 6095.24

TCAS - 2008 [18] Palumbo 0.150 9.89 -NA- 100 6593.33 -NA-

This Work - Cascode NMOS Kumar 0.025 1.99 1.50 100 7960.00 6000.00

This Work - Common Gate Kumar 0.025 2.00 2.00 100 8000.00 8000.00This Work - Cascode PMOS Kumar 0.025 2.20 2.00 100 8800.00 8000.00

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ANALOG LAYOUT

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Floor Planning

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Diff Input

TAIL CURRENT

PMOS OUT

CURRENT SOURCE CG

NMOS OUT

RESISTOR AVSS

AVDD

BIAS PMOS

BIAS NMOS

SIGNAL PATH

COMPENSATION CAPACITOR

PMOS LOAD

PMOS LOAD

CMFB PMOS CG LOAD

CG AMPLIFIER

SIGNAL PATH

SIGNAL PATHSIGNAL PATH

FLOOR PLANNING

INP

INNVOUT

ConsiderationsOrientation of TransistorsPower DistributionRouting EaseCurrent Mirror Matching

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Final Layout

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Comments and Conclusions

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We need to increase Unity Gain Frequency of the amplifierThe only way to do this are to decrease the compensation

capacitor and/or increase the diff-amps transconductance fun = gm1/2πCc

The problem with this is stability (the pole, f2 associated with the output of the op amp is comparable to fun)

Need to push f2 to a higher frequency

Moves the pole to a much higher frequency

Thus Indirect Feedback leads to significantlyFaster Lower PowerImproved PSRRSmaller Die Area

Indirect Feedback

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FUTURE RESEARCH

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Future Trends - Revisit

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Figure 2: Open loop gain trends in future CMOS semiconductor processes technology (ITRS) [1]

Where we simulate

State of the art

Difference

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Op-Amp Number of Stages

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Figure 4: Number of stages required to achieve the DC gain requirement for 10 and 14 bit resolution settling. The figure shows number of cascaded stages required with employing any cascoding for 10 bit ADC settling. It also shown the number internal stages with wide swing cascoded stage required for a 14 bit resolution settling [1]

Future holds tomulti-stage op-amps

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Multi-Stage Op Amps

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Multi-stage op amps carve the future of analog designs

Can we implement the indirect feedback frequency compensation to multi-stage amplifier?

What would the general form and design strategy for N stage indirect feedback amplifier look like ?

Do the amplifiers need to have REAL POLES?

VsA2A1

Cc

Differential Amplifier Gain Stage

iccRi

ABuffer

Output Buffer

VoutA2

Cc

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Moving the poles to the complex domain..?

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Uncompensated

Derived in [] leads to complex poles.. So the frequency response looks like?

Control DampingWith some creativeFeedback loop ??

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Three Stage Topologies: Latest in the Literature

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Transconductance Capacitor Feedback

Employs some form of indirect feedback frequency compensation

Report stellar response compared to other multi-stage amplifiers

Unity Gain Frequency is given by:

Ratio can be large

Moves the poles to the complex domain

Manages the frequency peaking through a feedback loop

[2]

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One of the proposed methods• Combine Indirect Feedback Technique to Sansen’s

approach of moving poles to the complex domain

10/20/2009 VAIBHAV KUMAR - IOWA STATE UNIVERSITY 58

To control dampingFactor of complex poles Indirect Compensation

to provide compensation current

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Proposed Methods AnalysisApproach

Appropriate Circuit ImplementationTheoretical AnalysisPotential and MeritsPropose a Design ProcedureDesign exampleFabricateEvaluate the performance and use it in an application

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References• [1] "Overall Roadmap Technology Characteristics (ORTC)," 03/19/2009, 2009; http://www.itrs.net/Links/2005ITRS/Exec

Sum2005.pdf.• [2] X. H. Peng, and W. Sansen, “Transconductance with capacitances feedback compensation for multistage

amplifiers,” Ieee Journal of Solid-State Circuits, vol. 40, no. 7, pp. 1514-1520, 2005.• [3] P. J. Hurst, S. H. Lewis, J. P. Keane et al., “Miller compensation using current buffers in fully differential CMOS two-

stage operational amplifiers,” Ieee Transactions on Circuits and Systems I-Regular Papers, vol. 51, no. 2, pp. 275-285, 2004.• [4] A. Pugliese, F. A. Amoroso, G. Cappuccino et al., “Design approach for fast-settling two-stage amplifiers employing

current-buffer Miller compensation,” Analog Integrated Circuits and Signal Processing, vol. 59, no. 2, pp. 151-159, 2009.• [5] M. Kayal, and Z. Randjelovic, “Auto-zero differential difference amplifier,” Electronics Letters, vol. 36, no. 8, pp. 695-

696, 2000.• [6] H. Mahattanakul, and J. Chutichatuporn, “Design procedure for two-stage CMOS opamp with flexible noise-power

balancing scheme,” Ieee Transactions on Circuits and Systems I-Regular Papers, vol. 52, no. 8, pp. 1508-1514, 2005.• [7] P. Monsurro, G. Scotti, A. Trifiletti et al., “Very low voltage CMOS two-stage amplifier,” 2007 European Conference on

Circuit Theory and Design, Vols 1-3, pp. 743-746, 2007.• [8] F. Schlogl, H. Dietrich et al., “Operational Amplifier with Two-Stage Gain-Boost,” Proceedings of the 6th WSEAS

International Conference in Simulation, Modeling and Optimization, Vols 22-24, pp. 482-486, 2006.• [9] H. Aminzadeh, and R. Lotfi, “On the power efficiency of cascode compensation over Miller compensation in two-stage

operational amplifiers,” Journal of Circuits Systems and Computers, vol. 17, no. 1, pp. 1-13, 2008.• [10] R. J. Reay, and G. T. A. Kovacs, “AN UNCONDITIONALLY STABLE 2-STAGE CMOS AMPLIFIER,” Ieee Journal of

Solid-State Circuits, vol. 30, no. 5, pp. 591-594, 1995.• [11] A. Pugliese, F. A. Amoroso, G. Cappuccino et al., “Design approach for fast-settling two-stage amplifiers employing

current-buffer Miller compensation,” Analog Integrated Circuits and Signal Processing, vol. 59, no. 2, pp. 151-159, 2009.• [12] A. Pugliese, F. Amoroso, G. Cappuccino et al., “Settling time optimisation for two-stage CMOS amplifiers with current-

buffer Miller compensation,” Electronics Letters, vol. 43, no. 23, pp. 1257-1258, 2007.• [13] M. Loikkanen, and J. Kostamovaara, “Improving capacitive drive capability of two-stage op amps with current buffer,”

Proceedings of the 2005 European

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Acknowledgements• Dr. Degang Chen (Major Professor)• Dr. Randall Geiger• Dr. Mani Mina• Dr. Ayaman Fayed

Friends and VLSI Group (Past and Present)

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• Rien Biel • Ryan Boesch• Jake Sloat• Ben Curtin

• Tao Zeng• Siva Sudani• Bharath Karthik• Vipul Katyal

• Jingbo Duan• Chen Zhao• Jun He

Committee Members

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