ECE 342 Electronic Circuits. 3. MOS Transistors

Similar documents
ECE 546 Lecture 10 MOS Transistors

ECE 342 Electronic Circuits. Lecture 6 MOS Transistors

ECE 497 JS Lecture - 12 Device Technologies

ECE 342 Solid State Devices & Circuits 4. CMOS

Lecture 12: MOSFET Devices

MOSFET: Introduction

MOS Transistor Theory

The Devices. Digital Integrated Circuits A Design Perspective. Jan M. Rabaey Anantha Chandrakasan Borivoje Nikolic. July 30, 2002

CMPEN 411 VLSI Digital Circuits. Lecture 03: MOS Transistor

MOS Transistor Properties Review

MOS Transistor I-V Characteristics and Parasitics

Lecture 3: CMOS Transistor Theory

Fig. 1 CMOS Transistor Circuits (a) Inverter Out = NOT In, (b) NOR-gate C = NOT (A or B)

Today s lecture. EE141- Spring 2003 Lecture 4. Design Rules CMOS Inverter MOS Transistor Model

MOS Transistor Theory

Practice 3: Semiconductors

Integrated Circuits & Systems

Lecture 15: MOS Transistor models: Body effects, SPICE models. Context. In the last lecture, we discussed the modes of operation of a MOS FET:

EE105 - Fall 2006 Microelectronic Devices and Circuits

The Devices: MOS Transistors

EE105 - Fall 2005 Microelectronic Devices and Circuits

Introduction and Background

ELEC 3908, Physical Electronics, Lecture 26. MOSFET Small Signal Modelling

Device Models (PN Diode, MOSFET )

CMOS INVERTER. Last Lecture. Metrics for qualifying digital circuits. »Cost» Reliability» Speed (delay)»performance

Device Models (PN Diode, MOSFET )

ECE 523/421 - Analog Electronics University of New Mexico Solutions Homework 3

MOS Transistors. Prof. Krishna Saraswat. Department of Electrical Engineering Stanford University Stanford, CA

EEC 118 Lecture #2: MOSFET Structure and Basic Operation. Rajeevan Amirtharajah University of California, Davis Jeff Parkhurst Intel Corporation

Digital Integrated Circuits A Design Perspective. Jan M. Rabaey Anantha Chandrakasan Borivoje Nikolic. The Devices. July 30, Devices.

Chapter 4 Field-Effect Transistors

Lecture 4: CMOS Transistor Theory

ECE 415/515 ANALOG INTEGRATED CIRCUIT DESIGN

DC and Transient Responses (i.e. delay) (some comments on power too!)

2007 Fall: Electronic Circuits 2 CHAPTER 10. Deog-Kyoon Jeong School of Electrical Engineering

Review of Band Energy Diagrams MIS & MOS Capacitor MOS TRANSISTORS MOSFET Capacitances MOSFET Static Model

P. R. Nelson 1 ECE418 - VLSI. Midterm Exam. Solutions

FIELD-EFFECT TRANSISTORS

SECTION: Circle one: Alam Lundstrom. ECE 305 Exam 5 SOLUTIONS: Spring 2016 April 18, 2016 M. A. Alam and M.S. Lundstrom Purdue University

Circuits. L2: MOS Models-2 (1 st Aug. 2013) B. Mazhari Dept. of EE, IIT Kanpur. B. Mazhari, IITK. G-Number

Fundamentals of the Metal Oxide Semiconductor Field-Effect Transistor

EE 230 Lecture 31. THE MOS TRANSISTOR Model Simplifcations THE Bipolar Junction TRANSISTOR

The Devices. Digital Integrated Circuits A Design Perspective. Jan M. Rabaey Anantha Chandrakasan Borivoje Nikolic. July 30, 2002

Lecture 12: MOS Capacitors, transistors. Context

Operation and Modeling of. The MOS Transistor. Second Edition. Yannis Tsividis Columbia University. New York Oxford OXFORD UNIVERSITY PRESS

ELEC 3908, Physical Electronics, Lecture 23. The MOSFET Square Law Model

EE 560 MOS TRANSISTOR THEORY

Lecture 04 Review of MOSFET

The Physical Structure (NMOS)

Lecture 11: MOS Transistor

Microelectronics Part 1: Main CMOS circuits design rules

Lecture 13 MOSFET as an amplifier with an introduction to MOSFET small-signal model and small-signal schematics. Lena Peterson

Lecture 23: Negative Resistance Osc, Differential Osc, and VCOs

Lecture 5: CMOS Transistor Theory

Section 12: Intro to Devices

CMPEN 411 VLSI Digital Circuits. Lecture 04: CMOS Inverter (static view)

6.012 Electronic Devices and Circuits Spring 2005

ESE 570: Digital Integrated Circuits and VLSI Fundamentals

! PN Junction. ! MOS Transistor Topology. ! Threshold. ! Operating Regions. " Resistive. " Saturation. " Subthreshold (next class)

Microelectronics Main CMOS design rules & basic circuits

ECE 546 Lecture 11 MOS Amplifiers

ECE315 / ECE515 Lecture-2 Date:

1/13/12 V DS. I d V GS. C ox ( = f (V GS ,V DS ,V SB = I D. + i d + I ΔV + I ΔV BS V BS. 19 January 2012

Chapter 2 CMOS Transistor Theory. Jin-Fu Li Department of Electrical Engineering National Central University Jungli, Taiwan

Introduction to CMOS VLSI. Chapter 2: CMOS Transistor Theory. Harris, 2004 Updated by Li Chen, Outline

The Devices. Devices

THE INVERTER. Inverter

EE105 Fall 2014 Microelectronic Devices and Circuits. NMOS Transistor Capacitances: Saturation Region

Design of Analog Integrated Circuits

EE 230 Lecture 33. Nonlinear Circuits and Nonlinear Devices. Diode BJT MOSFET

University of Pennsylvania Department of Electrical Engineering. ESE 570 Midterm Exam March 14, 2013 FORMULAS AND DATA

and V DS V GS V T (the saturation region) I DS = k 2 (V GS V T )2 (1+ V DS )

L ECE 4211 UConn F. Jain Scaling Laws for NanoFETs Chapter 10 Logic Gate Scaling

Chapter 13 Small-Signal Modeling and Linear Amplification

Important! EE141- Fall 2002 Lecture 5. CMOS Inverter MOS Transistor Model

ESE 570: Digital Integrated Circuits and VLSI Fundamentals

ECE-305: Fall 2017 MOS Capacitors and Transistors

CMOS Inverter (static view)

Lecture 12 Digital Circuits (II) MOS INVERTER CIRCUITS

ENGR890 Digital VLSI Design Fall Lecture 4: CMOS Inverter (static view)

EE5311- Digital IC Design

Name: Answers. Grade: Q1 Q2 Q3 Q4 Q5 Total. ESE370 Fall 2015

CHAPTER 5 MOS FIELD-EFFECT TRANSISTORS

EE 330 Lecture 16. MOS Device Modeling p-channel n-channel comparisons Model consistency and relationships CMOS Process Flow

VLSI Design and Simulation

Field-Effect (FET) transistors

Digital Electronics Part II - Circuits

Lecture 29 - The Long Metal-Oxide-Semiconductor Field-Effect Transistor (cont.) April 20, 2007

EEC 116 Lecture #3: CMOS Inverters MOS Scaling. Rajeevan Amirtharajah University of California, Davis Jeff Parkhurst Intel Corporation

ECE 438: Digital Integrated Circuits Assignment #4 Solution The Inverter

Lecture 15 OUTLINE. MOSFET structure & operation (qualitative) Review of electrostatics The (N)MOS capacitor

ECE 342 Electronic Circuits. Lecture 34 CMOS Logic

Figure 1: MOSFET symbols.

HW 5 posted due in two weeks Lab this week Midterm graded Project to be launched in week 7

Extensive reading materials on reserve, including

ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems. Today. Refinement. Last Time. No Field. Body Contact

Lecture 10 MOSFET (III) MOSFET Equivalent Circuit Models

ECE 342 Electronic Circuits. Lecture 35 CMOS Delay Model

EKV MOS Transistor Modelling & RF Application

EE382M-14 CMOS Analog Integrated Circuit Design

Transcription:

ECE 342 Electronic Circuits 3. MOS Transistors Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois jschutt@emlab.uiuc.edu 1

NMOS Transistor Typically L = 0.1 to 3 m, W = 0.2 to 100 m, and the thickness of the oxide layer (t ox ) is in the range of 2 to 50 nm. 2

NMOS Transistor NMOS Transistor N-Channel MOSFET Built on p-type substrate MOS devices are smaller than BJTs MOS devices consume less power than BJTs 3

NMOS Transistor - Layout Top View Cross Section 4

MOS Regions of Operation Resistive Triode V V GS DS V T small Nonlinear V GS V T V < ( V V ) DS GS T Active Saturation V GS V T V V V DS GS T 5

MOS Transistor Operation As V G increases from zero Holes in the p substrate are repelled from the gate area leaving negative ions behind A depletion region is created No current flows since no carriers are available As V G increases The width of the depletion region and the potential at the oxide-silicon interface also increase When the interface potential reaches a sufficiently positive value, electrons flow in the channel. The transistor is turned on As V G rises further The charge in the depletion region remains relatively constant The channel current continues to increase 6

MOS Triode Region - 1 W ID Cox VGS VT VDS L V V V DS GS T C ox t ox ox 3.9 o t ox C ox : gate oxide capacitance : electron mobility L: channel length W: channel width V T : threshold voltage 7

MOS Triode Region FET is like a linear resistor with r ds 1 C W V L V n ox GS T 8

MOS Triode Region - 2 V GS V T V V V DS GS T Charge distribution is nonuniform across channel Less charge induced in proximity of drain W 1 I C V V V V L 2 2 D n ox GS T DS DS 9

MOS Active Region V V V V Saturation occurs at pinch off when DS GS T DSP V GS V T V V V DS GS T (saturation) W I C V V 2L 2 D n ox GS T 10

NMOS Drain Current 11

NMOS Circuit Symbols 12

NMOS IV Characteristics characteristics for a device with k n (W/L) = 1.0 ma/v 2. 13

MOS Threshold Voltage The value of V G for which the channel is inverted is called the threshold voltage V T (or V t ). Characteristics of the threshold voltage Depends on equilibrium potential Controlled by inversion in channel Adjusted by implantation of dopants into the channel Can be positive or negative Influenced by the body effect 14

nmos Device Types Enhancement Mode Normally off & requires positive potential on gate Good at passing low voltages Cannot pass full V DD (pinch off) Depletion Mode Normally on (negative threshold voltage) Channel is implanted with positive ions (V T ) Provides inverter with full output swings 15

Types of MOSFETS 16

MOS Active Region Saturation Channel is pinched off Increase in V DS has little effect on i D Square-law behavior wrt (V GS -V T ) Acts like a current source 17

Diode-Connected Transistor When the drain and gate of a MOSFET are connected together the result is a two-terminal device known as a diode-connected transistor V GD V T for saturation region. Since V GD is zero, then the device is always in the saturation region. 18

incremental resistance Diode-Connected Transistor 1 W i i k V V 2 L 2 ' D n GS t If we replace by and use r ' ' VGS V k kn W L 2 ' ik V Vt 1 i 1 1 V W W L L ' 2 k' V Vt kn Vov V V V t ov 1 2 19

Example An MOS process technology has L min = 0.4 m, t ox = 8 nm, = 450 cm 2 /V.s, V T = 0.7V (a)find C ox and k n = n C ox (b) W/L = 8 m/0.8m. Calculate V GS, V DSmin for operation in saturation with I D = 100 A (c)find V GS for the device in (b) to operate as a 1 k resistor for small v DS 20

Example - Solution 11 ox 3.4510 Cox 4.3210 F/ m 4.32 ff/ m 9 t 810 ox 3 2 2 k C 450 cm / V. s4.32 ff/ m 194 A/ V ' 2 2 2 n n ox For operation in saturation region C 4.32 ff/ m 1 ' W i 2 D kn VGS VT 2 L 100 1 194 8 V 0.7 2 GS VGS 0.7 0.32V VGS 1.02V 2 0.8 VDS min VGS VT 0.32V ox 2 V DS min 0.32 V 21

Example (con t) Triode region with v DS very small r DS vds 1 i ' W D small v DS kn VGS VT L 100 1 6 19410 10V GS 0.7 VGS 0.7 0.52 V VGS 1.22 V 22

Body Effect The body effect V T varies with bias between source and body Leads to modulation of V T Potential on substrate affects threshold voltage V ( ) T VSB VTo 2F VSB 2F 1/2 1/2 F kt N a ln q ni Fermi potential of material 2qN 1/2 a C ox s Body bias coefficient 23

Channel-Length Modulation With depletion layer widening, the channel length is in effect reduced from L to L-L Channel-length modulation This leads to the following I-V relationship 1 i k W v V v 2 L ' 2 D n GS T 1 DS Where is a process technology parameter 24

Channel-Length Modulation Channel-length modulation causes i D to increase with v DS in saturation region 25

Problem A MOSFET has V T = 1 V with measured data: Find V GS (V) V DS (V) I D (A) 2 1 80 2 8 91 ( a) VGS VT VDS VGS VT Pinchoff ( b) V V V V V 1V Active region GS T DS GS T 26

Problem (cont ) Find i D at pinchoff V DSP = V GS -V T =1V 1 I k W V V V 2 L ' 2 D n GS T 1 DS 1 I k W V V V 2 L ' 2 D1 n GS1 T 1 DS1 1 I k W V V V 2 L ' 2 D2 n GS2 T 1 DS2 27

Problem (cont ) R 1 VDS 2 91 1.1375 1 V 80 DS1 1VDS 2 RRVDS1 ( V RV ) R1 DS 2 DS1 R 1 1.1375 1 0.0196 V V RV 81 DS 2 DS1 1 28

NMOS IV Curves 700 NMOS 600 VGS=1.0 VGS=1.5 VGS=2.0 VGS=2.5 500 400 IDS 300 200 100 0 0 0.5 1 1.5 2 2.5 Vds 29

NMOS IV Curves 30

MOSFET Circuit at DC Problem 1 The MOSFET in the circuit shown has V t = 1V, k n = 100A/V 2 and = 0. Find the required values of W/L and of R so that when v I =V DD =+5 V, r DS =50 and v o = 50 mv. v V 5 V, v V 0.05V I GS o DS VDS 0.05 rds 50 ID 0.001 A1 ma I 50 D R VDD vo 5 0.05 4.95 k I 1 D 31

MOSFET Circuit at DC Problem 1 (cont ) VDS VGS Vt triode region ' W I D kn VGS Vt VDS L V 2 2 DS 2 3 W 0.05 1 10010 5 10.05 L W L 50 2 32

The NMOS transistors in the circuit shown have V t = 1V, n C ox = 120A/V 2, = 0 and L 1 =L 2 =1m. Find the required values of gate width for each of Q 1 and Q 2 and the value of R, to obtain the voltage and current values indicated. V MOSFET Circuit at DC Problem 2 GS1 1.5 V 1 ' W Using I 2 D kn VGS Vt 2 L 1 W 120 A 1.5 1 2 W2 2m 2 1 5 3.5 R 12.5 k 0.120 33

Gate Capacitance V 0 V 0, V small GT GT DS Capacitance Depends on bias Fringing fields are present Account for overlap C V GT 0, V large DS 34

Capacitance Gate Capacitance C G determines the amount of charge to switch gate Several distributed components Large discontinuity as device turns on At saturation capacitance is entirely between gate and source Define VDS X V V GS T 2 1 X Cgs Cgso WLCox 1 3 2 X 2 1 Cgd Cgdo WLCox 1 3 2 X 2 2 35

MOS Capacitances Expect capacitance between every two of the four terminals. 36

MOS Parasitics - Capacitance from gate to other 3 terminals - Diodes to body - Series resistance - Wiring parasitics 37

PMOS Transistor 0 PMOS -100-200 VGS=-1.0-300 -400-500 -600 VGS=-1.0 VGS=-1.5 VGS=-2.0 VGS=-2.5-700 -2.5-2 -1.5-1 -0.5 0 - All polarities are reversed from nmos - v GS, v DS and V t are negative - Current i D enters source and leaves through drain - Hole mobility is lower low transconductance - nmos favored over pmos Vds 38

PMOS Circuit The PMOS transistor in the circuit shown has V t = -0.7 V, p C ox = 60A/V 2, = 0 and L=0.8m. Find the values required for W and R, in order to establish a drain current of 115 A and a voltage V D of 3.5 V. R 3.5 3.04 k 0.115 1 W 2 0.8 3 0.115 60 10 1.5 ( 0.7) ma W 4.8 m 2 39

Complementary MOS CMOS Characteristics Combine nmos and pmos transistors pmos size is larger for electrical symmetry 40

CMOS Advantages Virtually, no DC power consumed No DC path between power and ground Excellent noise margins (V OL =0, V OH =V DD ) Inverter has sharp transfer curve Drawbacks Requires more transistors Process is more complicated pmos size larger to achieve electrical symmetry Latch up 41

MOSFET Switch NMOS PMOS Characteristics of MOS Switch MOS approximates switch better than BJT in off state Resistance in on state can vary from 100 to 1 k 42

CMOS Switch CMOS switch is called an inverter 43

CMOS Switch Off State OFF State (V in : low) nmos transistor is off Path from V out to V 1 is through PMOS V out : high 44

CMOS Switch On State ON State (V in : high) pmos transistor is off Path from V out to ground is through nmos V out : low 45

CMOS Inverter r dsn 1 k W V V ' N DD T L n r dsp 1 k W V V ' P DD T L p Short switching transient current low power 46