MOSFETS: Gain & non-linearity

Similar documents
CMOS Technology. 1. Why CMOS 2. Qualitative MOSFET model 3. Building a MOSFET 4. CMOS logic gates. Handouts: Lecture Slides. metal ndiff.

Processing Information: The Digital Abstraction. Concrete Encodings of Information

LECTURE 14. (Guest Lecturer: Prof. Tsu-Jae King) Last Lecture: Today:

INTRODUCTION TO MOS TECHNOLOGY

Design cycle for MEMS

CMOS VLSI Design (A3425)

Lecture 3: Transistors

Lecture 16. Complementary metal oxide semiconductor (CMOS) CMOS 1-1

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

EE 42/100 Lecture 23: CMOS Transistors and Logic Gates. Rev A 4/15/2012 (10:39 AM) Prof. Ali M. Niknejad

Lecture #29. Moore s Law

CS/ECE 5710/6710. Composite Layout

problem grade total

Digital Electronics Part II - Circuits

MOS Field Effect Transistors

PHYSICAL STRUCTURE OF CMOS INTEGRATED CIRCUITS. Dr. Mohammed M. Farag

Conduction Characteristics of MOS Transistors (for fixed Vds)! Topic 2. Basic MOS theory & SPICE simulation. MOS Transistor

Topic 2. Basic MOS theory & SPICE simulation

Conduction Characteristics of MOS Transistors (for fixed Vds) Topic 2. Basic MOS theory & SPICE simulation. MOS Transistor

Field-Effect Transistor (FET) is one of the two major transistors; FET derives its name from its working mechanism;

ECE/CoE 0132: FETs and Gates

Transistor was first invented by William.B.Shockley, Walter Brattain and John Bardeen of Bell Labratories. In 1961, first IC was introduced.

ECE520 VLSI Design. Lecture 5: Basic CMOS Inverter. Payman Zarkesh-Ha

Digital Design and System Implementation. Overview of Physical Implementations

Semiconductor Physics and Devices

Basic Fabrication Steps

! MOS Device Layout. ! Inverter Layout. ! Gate Layout and Stick Diagrams. ! Design Rules. ! Standard Cells. ! CMOS Process Enhancements

Digital Electronics. By: FARHAD FARADJI, Ph.D. Assistant Professor, Electrical and Computer Engineering, K. N. Toosi University of Technology

MOS TRANSISTOR THEORY

Session 10: Solid State Physics MOSFET

EE301 Electronics I , Fall

UNIVERSITY OF CALIFORNIA AT BERKELEY College of Engineering Department of Electrical Engineering and Computer Sciences.

Module-3: Metal Oxide Semiconductor (MOS) & Emitter coupled logic (ECL) families

ECE 5745 Complex Digital ASIC Design Topic 2: CMOS Devices

Semiconductor Memory: DRAM and SRAM. Department of Electrical and Computer Engineering, National University of Singapore

Lecture 15. Field Effect Transistor (FET) Wednesday 29/11/2017 MOSFET 1-1

Physical Bits: Transistors and Logic

ENEE307 Lab 7 MOS Transistors 2: Small Signal Amplifiers and Digital Circuits

Introduction to Electronic Devices

I E I C since I B is very small

Digital logic families

Field Effect Transistors (FET s) University of Connecticut 136

Integrated diodes. The forward voltage drop only slightly depends on the forward current. ELEKTRONIKOS ĮTAISAI

Lecture 02: Logic Families. R.J. Harris & D.G. Bailey

EEC 118 Lecture #11: CMOS Design Guidelines Alternative Static Logic Families

Depletion-mode operation ( 공핍형 ): Using an input gate voltage to effectively decrease the channel size of an FET

CMOS Digital Logic Design with Verilog. Chapter1 Digital IC Design &Technology

Digital Electronics. Assign 1 and 0 to a range of voltage (or current), with a separation that minimizes a transition region. Positive Logic.

Digital circuits. Bởi: Sy Hien Dinh

UNIT-1 Bipolar Junction Transistors. Text Book:, Microelectronic Circuits 6 ed., by Sedra and Smith, Oxford Press

An introduction to Depletion-mode MOSFETs By Linden Harrison

Jack Keil Wolf Lecture. ESE 570: Digital Integrated Circuits and VLSI Fundamentals. Lecture Outline. MOSFET N-Type, P-Type.

CHAPTER 6 DIGITAL CIRCUIT DESIGN USING SINGLE ELECTRON TRANSISTOR LOGIC

EECS150 - Digital Design Lecture 19 CMOS Implementation Technologies. Recap and Outline

UNIT III VLSI CIRCUIT DESIGN PROCESSES. In this chapter we will be studying how to get the schematic into stick diagrams or layouts.

4.1 Device Structure and Physical Operation

EECS150 - Digital Design Lecture 15 - CMOS Implementation Technologies. Overview of Physical Implementations

EECS150 - Digital Design Lecture 9 - CMOS Implementation Technologies

Week 7: Common-Collector Amplifier, MOS Field Effect Transistor

ECE520 VLSI Design. Lecture 2: Basic MOS Physics. Payman Zarkesh-Ha

Shorthand Notation for NMOS and PMOS Transistors

ECE 484 VLSI Digital Circuits Fall Lecture 02: Design Metrics

MTLE-6120: Advanced Electronic Properties of Materials. Semiconductor transistors for logic and memory. Reading: Kasap

ESE 570: Digital Integrated Circuits and VLSI Fundamentals

UNIT-VI FIELD EFFECT TRANSISTOR. 1. Explain about the Field Effect Transistor and also mention types of FET s.

MOSFET & IC Basics - GATE Problems (Part - I)

Lecture 9: Cell Design Issues

HW#3 Solution. Dr. Parker. Spring 2014

TECHNO INDIA BATANAGAR (DEPARTMENT OF ELECTRONICS & COMMUNICATION ENGINEERING) QUESTION BANK- 2018

Microelectronics, BSc course

+1 (479)

ECE 340 Lecture 37 : Metal- Insulator-Semiconductor FET Class Outline:

Chapter 6 DIFFERENT TYPES OF LOGIC GATES

Field Effect Transistor (FET) FET 1-1

Combinational Logic. Prof. MacDonald

FET(Field Effect Transistor)

Chapter 6 DIFFERENT TYPES OF LOGIC GATES

Architecture of Computers and Parallel Systems Part 9: Digital Circuits

Chapter 1. Introduction

2009 Spring CS211 Digital Systems & Lab 1 CHAPTER 3: TECHNOLOGY (PART 2)

Chapter 6: Field-Effect Transistors

MEASUREMENT AND INSTRUMENTATION STUDY NOTES UNIT-I

Microcontroller Systems. ELET 3232 Topic 13: Load Analysis

EE 330 Lecture 5. Improved Device Models Propagation Delay in Logic Circuits

EE 330 Lecture 27. Bipolar Processes. Special Bipolar Processes. Comparison of MOS and Bipolar Proces JFET. Thyristors SCR TRIAC

Lecture 13. Metal Oxide Semiconductor Field Effect Transistor (MOSFET) MOSFET 1-1

Introduction to CMOS VLSI Design (E158) Lecture 9: Cell Design

ECE 2300 Digital Logic & Computer Organization

UNIT 3: FIELD EFFECT TRANSISTORS

Field Effect Transistors (npn)

Design of Low power and Area Efficient 8-bit ALU using GDI Full Adder and Multiplexer

NAME: Last First Signature

Lecture 6: Electronics Beyond the Logic Switches Xufeng Kou School of Information Science and Technology ShanghaiTech University

Reading. Lecture 17: MOS transistors digital. Context. Digital techniques:

Q1. Explain the construction and principle of operation of N-Channel and P-Channel Junction Field Effect Transistor (JFET).

Difference between BJTs and FETs. Junction Field Effect Transistors (JFET)

Exam 1 ECE 410 Fall 2002

Low Power 8-Bit ALU Design Using Full Adder and Multiplexer

MOSFET Terminals. The voltage applied to the GATE terminal determines whether current can flow between the SOURCE & DRAIN terminals.

6. Field-Effect Transistor

Transcription:

MOFET: ain & non-linearity source gate Polysilicon wire Heavily doped (n-type or p-type) diffusions W Inter-layer io 2 insulation Very thin (<20Å) high-quality io 2 insulating layer isolates gate from channel region. L drain Channel region: electric field from charges on gate locally inverts type of substrate to create a conducting channel between source and drain. bulk oped (p-type or n-type) silicon substrate MOFETs (metal-oxide-semiconductor field-effect transistors) are four-terminal voltage-controlled switches. Current flows between the diffusion terminals if the voltage on the gate terminal is large enough to create a conducting channel, otherwise the mosfet is off and the diffusion terminals are not connected. Why are MO devices King? L03 - CMO Technology 5

FETs as switches The four terminals of a Field Effect Transistor (gate, source, drain and bulk) connect to conducting surfaces that generate a complicated set of electric fields in the channel region which depend on the relative voltages of each terminal. gate inversion happens here n source E h drain n p E v bulk INVERION: A sufficiently strong vertical field will attract enough electrons to the surface to create a conducting n-type channel between the source and drain. CONUCTION: If a channel exists, a horizontal field will cause a drift current from the drain to the source. L03 - CMO Technology 6

Linear operating region V > V TH 0 < V < V sat I L Why is this bigger here than on other side? Larger creates deeper channel which increases I I I proportional to µ 0 (W/L) Increasing Larger V increases drift current but also reduces vertical field component which in turn makes channel less deep. At some point, electrons are traveling as fast as possible through the channel ( velocity saturation ) and the current stops growing linearly. V L03 - CMO Technology 7

aturated operating region V > V TH V sat < V I L = L - δl δl V sat -V TH This looks just like a fet with a channel length of L < L. horter L implies greater I. As V increases, δl gets larger. V I = -V TH When V = -V TH the vertical field component is reduced and the channel is pinched-off. Electrons just keep traveling across depletion region Increasing V V L03 - CMO Technology 8

NFET ummary + n p n + V 0 Operating regions: - - cut-off: < V TH linear: V TH V < V sat 0.8V I linear saturation -V TH saturation: V TH V V sat V L03 - CMO Technology 9

FETs come in two flavors y embedding p-type source and drain in a n-type substrate, we can fabricate a complement to the N-FET: n p n p n p The use of both NFETs and PFETs complimentary transistor types is a key to CMO (complementary MO) logic families. L03 - CMO Technology 10

PFET ummary - p n p + V 0 Operating regions: - + cut-off: > V TH 0.8V -V linear: V TH V > V sat - saturation: V TH V V sat -V TH saturation linear -I L03 - CMO Technology 11

CMO Inverter = 0v I PU = 1v V in = power supply I PU V out = 2v = 3v = 4v I PU vs V OUT for PULLUP V OUT I P = 0V I P = 5v = 4v = 3v = 2v = 1v I P vs V OUT for PULLOWN V OUT L03 - CMO Technology 12

CMO Inverter VTC I pd V in = 0.5V I pu I pd teady state reached when V out reaches value where I pu = I pd. I pu Vout V out V OH V in = 3.5V I pd V in = 1.5V I pu I pd V out I pu V out V in = 4.5V V OL I pu V in = 2.5V V IL V IH V in I pd V out I pd I pu V out When both fets are saturated, small changes in V in produce large changes in V out L03 - CMO Technology 13

Think witches V pullup: make this connection when near 0 so that V OUT = V V OUT pulldown: make this connection when near V so that V OUT = 0 L H H L V IL V OUT V IH V IH V OUT V IL L03 - CMO Technology 14

tandard Cell Layout for Inverter W: scaled width used in Process-independent design m1/nwell contact m1 power bus m1/pdiff contact pfet Use two narrow mosfets in parallel instead of one wide mosfet m2/m1 via m1/poly contact poly wire m1 wire nfet m1/ndiff contact m1 ground bus m1/substrate contact Physical design of a CMO gate is represented by a mask layout showing where material on each layer (ndiff, pdiff, poly, m1, m2, ) should be placed on the silicon wafer. Each manufacturing process has a set of design rules that determine minimum widths, spacings, overlaps, etc. L03 - CMO Technology 21

eyond Inverters: Complementary pullups and pulldowns Now you know what the C in CMO stands for! We want complementary pullup and pulldown logic, i.e., the pulldown should be on when the pullup is off and vice versa. pullup pulldown F(A 1,,An) on off driven 1 off on driven 0 on on driven X off off no connection ince there s plenty of capacitance on the output node, when the output becomes disconnected it remembers its previous voltage -- at least for a while. The memory is the load capacitor s charge. Leakage currents will cause eventual decay of the charge (that s why RAMs need to be refreshed!). L03 - CMO Technology 22

What a nice V OH you have... CMO complements Thanks. It runs in the family... conducts when is high conducts when is low A A conducts when A is high and is high: A. conducts when A is low or is low: A+ = A. A A conducts when A is high or is high: A+ conducts when A is low and is low: A. = A+ L03 - CMO Technology 23

A pop quiz! What function does this gate compute? A A C 0 0 0 1 1 0 1 1 1 1 NAN 1 0 L03 - CMO Technology 24

Here s another A What function does this gate compute? A C 0 0 0 1 1 0 1 1 1 0 NOR 0 0 L03 - CMO Technology 25

eneral CMO gate recipe tep 1. Figure out pulldown network that does what you want, e.g., F = A*(+C) (What combination of inputs generates a low output) A C tep 2. Walk the hierarchy replacing nfets with pfets, series subnets with parallel subnets, and parallel subnets with series subnets tep 3. Combine pfet pullup network from tep 2 with nfet pulldown network from tep 1 to form fullycomplementary CMO gate. A A A C C C ut isn t it hard to wire it all up? L03 - CMO Technology 26

Emerging ig Issue: Power moves from L to H to L V V OUT moves from H to L to H C V OUT Energy dissipated = C V 2 per gate Power consumed = f n C V 2 per chip C discharges and then recharges where f = frequency of charge/discharge n = number of gates /chip L03 - CMO Technology 27

Unfortunately Modern chip (Ultraparc III, Power4, Itanium 2) dissipates from 80W to 150W with a Vdd 1.2V (Power supply current chip is 100 Amps) Ampacity is similar to a big double oven! Cooling challenge is like making the filament of a 100W incandescent lamp cool to the touch! Worse yet Little room left to reduce Vdd nc and f continue to grow L03 - CMO Technology 28

Emerging ig Issue: Wires V out R C Today (i.e., 100nm): τ RC 50ps/mm Implies 2ns to traverse a 20mm x 20mm chip This is a long time in a 2Hz processor L03 - CMO Technology 29

MOFET features ummary PN junctions provide electrical isolation witch-like behavior controlled by hrinking geometries improves performance CMO features CMO logic is naturally inverting: 1 inputs lead to 0 outputs ood noise margins because V OL = 0, V OH = V complementary logic has high gain No static power dissipation Next time: timing, converting functionality to logic L03 - CMO Technology 30