Analysis and Design of Analog Integrated Circuits Lecture 6. Current Mirrors

Similar documents
Analysis and Design of Analog Integrated Circuits Lecture 8. Cascode Techniques

6.776 High Speed Communication Circuits Lecture 7 High Freqeuncy, Broadband Amplifiers

6.976 High Speed Communication Circuits and Systems Lecture 5 High Speed, Broadband Amplifiers

The Differential Amplifier. BJT Differential Pair

Design cycle for MEMS

Analysis and Design of Analog Integrated Circuits Lecture 20. Advanced Opamp Topologies (Part II)

6.776 High Speed Communication Circuits Lecture 6 MOS Transistors, Passive Components, Gain- Bandwidth Issue for Broadband Amplifiers

Basic Circuits. Current Mirror, Gain stage, Source Follower, Cascode, Differential Pair,

Current Mirrors and Biasing Prof. Ali M. Niknejad Prof. Rikky Muller

SKEL 4283 Analog CMOS IC Design Current Mirrors

Current Mirrors. Basic BJT Current Mirror. Current mirrors are basic building blocks of analog design. Figure shows the basic NPN current mirror.

Lecture 13. Biasing and Loading Single Stage FET Amplifiers. The Building Blocks of Analog Circuits - III

Chapter 4: Differential Amplifiers

ECE 255, MOSFET Amplifiers

ECE 255, MOSFET Basic Configurations

Experiment 10 Current Sources and Voltage Sources

MOS IC Amplifiers. Token Ring LAN JSSC 12/89

Lecture 34: Designing amplifiers, biasing, frequency response. Context

ECE315 / ECE515 Lecture 7 Date:

F9 Differential and Multistage Amplifiers

Gechstudentszone.wordpress.com

EECS3611 Analog Integrated Circuit Design. Lecture 3. Current Source and Current Mirror

Chapter 13: Introduction to Switched- Capacitor Circuits

Current Mirrors. Current Source and Sink, Small Signal and Large Signal Analysis of MOS. Knowledge of Various kinds of Current Mirrors

Session 2 MOS Transistor for RF Circuits

ECEN 474/704 Lab 5: Frequency Response of Inverting Amplifiers

Operational Amplifiers

Lecture 14. FET Current and Voltage Sources and Current Mirrors. The Building Blocks of Analog Circuits - IV

Analysis and Design of Analog Integrated Circuits Lecture 18. Key Opamp Specifications

Lecture 2, Amplifiers 1. Analog building blocks

Preliminary Exam, Fall 2013 Department of Electrical and Computer Engineering University of California, Irvine EECS 170B

4.5 Biasing in MOS Amplifier Circuits

CHAPTER 8 DIFFERENTIAL AND MULTISTAGE AMPLIFIERS

Experiment #7 MOSFET Dynamic Circuits II

Current Mirrors. Prof. Tai-Haur Kuo, EE, NCKU, Tainan City, Taiwan 4-1

ECE315 / ECE515 Lecture 9 Date:

ECEN 474/704 Lab 6: Differential Pairs

Chapter 4. CMOS Cascode Amplifiers. 4.1 Introduction. 4.2 CMOS Cascode Amplifiers

EE105 Fall 2015 Microelectronic Devices and Circuits

Differential Amplifiers/Demo

Lab 4: Supply Independent Current Source Design

Building Blocks of Integrated-Circuit Amplifiers

Multistage Amplifiers

Building Blocks of Integrated-Circuit Amplifiers

D n ox GS THN DS GS THN DS GS THN. D n ox GS THN DS GS THN DS GS THN

BJT Amplifier. Superposition principle (linear amplifier)

Design and Analysis of High Gain Differential Amplifier Using Various Topologies

EE105 Fall 2015 Microelectronic Devices and Circuits Multi-Stage Amplifiers. Prof. Ming C. Wu 511 Sutardja Dai Hall (SDH)

Microelectronics Circuit Analysis and Design

Lecture 33: Context. Prof. J. S. Smith

Current Source/Sinks

Review Sheet for Midterm #2

EE301 Electronics I , Fall

Experiment 5 Single-Stage MOS Amplifiers

Electronic Circuits for Mechatronics ELCT 609 Lecture 7: MOS-FET Amplifiers

Chapter 5. Operational Amplifiers and Source Followers. 5.1 Operational Amplifier

Designing a 960 MHz CMOS LNA and Mixer using ADS. EE 5390 RFIC Design Michelle Montoya Alfredo Perez. April 15, 2004

ES 330 Electronics II Homework # 6 Soltuions (Fall 2016 Due Wednesday, October 26, 2016)

UNIVERSITY OF CALIFORNIA AT BERKELEY College of Engineering Department of Electrical Engineering and Computer Sciences. Discussion Notes #9

55:041 Electronic Circuits The University of Iowa Fall Exam 1 Solution

EE5310/EE3002: Analog Circuits. on 18th Sep. 2014

Homework Assignment 07

Summary of Lecture Notes on Metal-Oxide-Semiconductor, Field-Effect Transistors (MOSFETs)

444 Index. F Fermi potential, 146 FGMOS transistor, 20 23, 57, 83, 84, 98, 205, 208, 213, 215, 216, 241, 242, 251, 280, 311, 318, 332, 354, 407

ECE315 / ECE515 Lecture 8 Date:

Metal-Oxide-Silicon (MOS) devices PMOS. n-type

Experiment 9- Single Stage Amplifiers with Passive Loads - MOS

Unit 3: Integrated-circuit amplifiers (contd.)

Reading. Lecture 33: Context. Lecture Outline. Chapter 9, multi-stage amplifiers. Prof. J. S. Smith

Laboratory 1 Single-Stage MOSFET Amplifier Analysis and Design Due Date: Week of February 20, 2014, at the beginning of your lab section

Lecture 16: MOS Transistor models: Linear models, SPICE models. Context. In the last lecture, we discussed the MOS transistor, and

Lecture 20 Transistor Amplifiers (II) Other Amplifier Stages

CMOS VLSI Design (A3425)

CS and CE amplifiers with loads:

ECE/CoE 0132: FETs and Gates

Advanced Operational Amplifiers

CMOS Cascode Transconductance Amplifier

Chapter 4 Single-stage MOS amplifiers

Short Channel Bandgap Voltage Reference

Improved Inverter: Current-Source Pull-Up. MOS Inverter with Current-Source Pull-Up. What else could be connected between the drain and V DD?

Assoc. Prof. Dr. Burak Kelleci

Microelectronics Circuit Analysis and Design. MOS Capacitor Under Bias: Electric Field and Charge. Basic Structure of MOS Capacitor 9/25/2013

6.776 High Speed Communication Circuits and Systems Lecture 14 Voltage Controlled Oscillators

C H A P T E R 5. Amplifier Design

F7 Transistor Amplifiers

Laboratory #9 MOSFET Biasing and Current Mirror

Lecture 240 Cascode Op Amps (3/28/10) Page 240-1

Microelectronics Part 2: Basic analog CMOS circuits

Experiment #6 MOSFET Dynamic circuits

EMCA mini project report

Introduction to MOSFET MOSFET (Metal Oxide Semiconductor Field Effect Transistor)

Lecture 300 Low Voltage Op Amps (3/28/10) Page 300-1

University of Southern C alifornia School Of Engineering Department Of Electrical Engineering

INTRODUCTION TO ELECTRONICS EHB 222E

ECE 546 Lecture 12 Integrated Circuits

Exam Below are two schematics of current sources implemented with MOSFETs. Which current source has the best compliance voltage?

Microelectronics Exercises of Topic 5 ICT Systems Engineering EPSEM - UPC

Fundamentals of Microelectronics

Nonlinear Macromodeling of Amplifiers and Applications to Filter Design.

CHAPTER 4 ULTRA WIDE BAND LOW NOISE AMPLIFIER DESIGN

Transcription:

Analysis and Design of Analog Integrated Circuits ecture 6 Current Mirrors Michael H. Perrott February 8, 2012 Copyright 2012 by Michael H. Perrott All rights reserved.

From ecture 5: Basic Single-Stage CMOS Amplifiers Common Common Gate Follower Z Z W 1 Vout i d W 1 i d W 1 i in Z Common with Degeneration Z i d W 1 Z src V src I src Z src Z S 2

A Closer ook at oad Impedance Common Common Gate Follower Z Z W 1 Vout i d W 1 i d W 1 i in Z Common with Degeneration Z Z S i d W 1 To achieve high gain (or low attenuation in the case of a source follower), it is very desirable to achieve high load impedance, Z - Unfortunately, using a simple resistor of high value has issues What are these issues? 3

Issue #1: Headroom imitations Common V dd R I d Want V ds > ΔV The bias current of the device is a direct function of R I d = V dd V ds R - V dd is < 3.6V for most modern CMOS processes - V ds must be greater than V to maintain device saturation arge R implies small I d (implies small g m, poor frequency response, etc.) 4

Issue #2: Area of Circuit Common V dd R I d Want V ds > ΔV The most common resistors for precision analog circuits are often based on unsilicided polysilicon layers - The sheet resistance of unsilicided polysilicon is often < 1k /square arge polysilicon R implies relatively large circuit area (implies high relative cost) 5

An Elegant Approach to Achieving High Gain Common V dd I bias I d V ds1 > ΔV 1 Replacement of resistor load with a current source yields the highest possible DC gain out of the amplifier - Current source determines I d of device We can make current sources out of transistors - Generally smaller area than polysilicon resistors What is the small signal gain of the above circuit? 6

A Simple Transistor Based Current V dd V bias Vsd2 > ΔV 2 M 2 I d V ds1 > ΔV 1 Simply use a PMOS load that is properly biased - If we keep the PMOS in saturation, its current is relatively constant despite V sd variations This is the desired behavior of a current source What are the nonideal issues of the above approach? 7

Issue #1: Impedance of PMOS Device V dd V bias Vsd2 > ΔV 2 M 2 Z I d V ds1 > ΔV 1 An ideal current source has infinite impedance PMOS devices have finite impedance - What is Z in the above circuit? - How does finite Z impact the gain of the circuit? We will later examine techniques to increase Z 8

Issue #1: High Bias Sensitivity V dd V bias W 2 M 2 I d V ds1 > ΔV 1 The PMOS device current, I d, is very sensitive to the value of V bias - We want I d to be relatively constant across temperature and process variations How can we achieve tighter control over I d across temperature and process variations? 9

Key Technique: Use Current Mirror V dd W 3 V bias W 2 V sd2 > ΔV 2 M 3 M 2 I bias I d V ds1 > ΔV 1 Key idea: use a different PMOS device, M 3, to transform a bias current, I bias, into bias voltage, V bias - V bias now yields a consistent current, I d, in M 2 (assumed to be in saturation) across temperature and process variations - Note that layout of M 2 and M 3 must be done properly to achieve good device matching How does I d relate to I bias? 10

NMOS Devices Can Also Be Used for Current Mirrors I bias I d W 2 M 2 V bias W 1 V ds1 > ΔV 1 We often use both NMOS and PMOS versions in designs - We ll explore this issue further later in the semester General issue: current mirrors involve direct feedback between drain and gate Can we apply proposed Thevenin modeling approach to current mirrors? 11

Issue: Thevenin Impedances Are Not Adequate R S ooking as purely Thevenin impedances But, in reality Issue: coupling between source, drain, or gate - Do we have to abandon the Thevenin method? 12

Try Proposed Thevenin Model g d i test v test R ths i s R thg v g A v v g αi s Rthd s R s Key Calculations (ignore R thd for now): 13

Proposed Thevenin Model Works! g d i test v test R ths i s R thg v g A v v g αi s Rthd s R s Now include R thd : 14

Check Thevenin Resistance Calculation Diode-Connected Device Derive Using Hybrid-π Model Resulting One-Port Model v gs g m v gs -g mb v s (g m +g mb ) r o 1 g m g m R S R S v s R S Plug in Hybrid- to do the analysis - Answer agrees with proposed Thevenin model approach Easiest to just memorize this result: Diode connected MOS looks like a resistor of value 1/g m 15

Now Apply Thevenin Approach to the Current Mirror I bias node1 node2 I ref M 2 M 2 node1 node2 node2 g1 d1 1 g m2 R thg1 v g1 g m1 v g1 R thd1 R thd1 = r o1 Diode-Connected Common Key parameter of current source: output resistance - Corresponds to r o of device 16

Cascoded Current I ref I bias V bias V bias V ds3 > ΔV 3 M 3 M 3 M 2 V ds1 > ΔV 1 r o1 Offers increased output resistance - Calculate using Thevenin resistance method - How does I ref compare to I bias? 17

Double Cascode Current I 1 I 2 V bias2 M 3 V ds3 > ΔV 3 V bias1 M 2 V ds2 > ΔV 2 M 4 V ds1 > ΔV 1 Offers further increased output resistance - Calculate using Thevenin resistance method - How does I 2 compare to I 1? 18