Today's Goals. Finish MOS transistor Finish NMOS logic Start CMOS logic

Size: px
Start display at page:

Download "Today's Goals. Finish MOS transistor Finish NMOS logic Start CMOS logic"

Transcription

1 Bi Today's Goals Finish MOS transistor Finish Start

2 Bi MOS Capacitor Equations Threshold voltage Gate capacitance V T = ms Q i C i Q II C i Q d C i 2 F n-channel - - p-channel ± ± Contributions to threshold voltage For enhancement type devices: for n-channel devices threshold voltage >0 p-channel devices threshold voltage < 0 C i = 0 ox t ox - - W L

3 Bi MOS Capacitor Characteristics You MUST know/understand MOS capacitor threshold voltage formula You MUST know/understand/be able to draw MOS capacitor band diagrams Refer to Streetman's book for details!!

4 Bi I G =0 MOS Transistor Operation I D =0 when V GS <V T I D staturates when V GD <V T Pinch-off is an educational tool to justify saturation. At the drain end the electrons are out-of equilibrium, so the equilibrium concentration formula does NOT apply. Pinch-off occurs due to velocity saturation at drain end of the channel.

5 Bi

6 Bi

7 Bi MOS Transistor I-V characteristics Analytical derivation assumes Long channel Long channel implies uniform electric field within the channel Do you think measured values will match the analytical formula? Even for a physically long device? What can be done to predict the I-V curve of a transistor before fabrication? You are not responsible from the derivation of the transistor IV. You must be able to draw and understand the transistor band diagram.

8 Bi MOS Transistor I-V characteristics Operation Regimes: Off Linear Saturated Can you write equations for both NMOS and PMOS? Device transconductance parameter: K= W L ox t ox I G =0 Process transconductance parameter: k= ox t ox

9 Bi MOS Transistor I-V characteristics Operation Regimes: Off Linear Saturated Can you write equations for both NMOS and PMOS? Device transconductance parameter: K= W L ox t ox Process transconductance parameter: k= ox t ox

10 Bi MOS Transistor I-V characteristics NMOS V T 0 V GS V T OFF V GS V T V GS V T I DS 0 When linear V DS V GS V T LINEAR V DS V GS V T SAT 2 ] 2 I DS = K N [ V GS V T V DS V DS When SAT I DS = K N 2 V GS V T 2

11 Bi MOS Transistor I-V characteristics PMOS V T 0 V GS V T OFF V GS V T V GS V T I DS 0 When linear V DS V GS V T LINEAR V DS V GS V T SAT 2 ] 2 I DS = K P [ V GS V T V DS V DS When SAT I DS = K P 2 V GS V T 2

12 Bi MOS Transistor I-V characteristics NMOS/PMOS V GS V T OFF V GS V T V DS V GS V T LINEAR V GS V T V DS V GS V T SAT When linear I DS = K [ V GS V T V DS V 2 ] DS 2 When SAT I DS = K 2 V V GS T 2

13 Bi MOS Transistor I-V characteristics You MUST memorize NMOS/PMOS transistor I-V equations and characteristics

14 Bi MOS Secondary effects Body effect Subthreshold current Transit time Short channel effect Channel length modulation Velocity Saturation Gate leakage In fact, extremely important for MODERN MOS LOGIC. But complicates a first study of MOS LOGIC. These will be studied later, when we need them.

15 Bi NMOS Logic 3 types of pull-up devices Has static power dissipation Low-to-High delay is large Was used when there was no p-type MOS around

16 Bi Resistor load NMOS Logic VTC I LOAD =0 Identify the mode of the transistor and solve for I R =I DS(MN) OBSERVE: correct logic depends on the values of R and K

17 Bi Resistor load NMOS Logic VTC V I V T M NO I DMNO =0 V O =V DD OFF V i =V DD M NO LINEAR I D =K [ V DD V T V O V 2 ] O 2 I R = V DD V O R solve for V O from I D =I R Ignore the Vo^2 term to get V O = V DD R K V DD V T 1

18 Bi Resistor load NMOS Logic VTC Is M NO really in LINEAR region? K 1 ma V 2 Assume R 100 Ohm Assume V T =1V V O = =3.5V V DS = Yes device is linear BUT V O V T. If R=1000 Ohm V O 0.1V V T Correct logic operation depends on R and K

19 Bi Depletion load NMOS Logic VTC I LOAD =0 Identify the mode of the transistor and solve for -I DS(ML) =I DS(MN) OBSERVE: correct logic depends on the values of K L and K O

20 Bi P H =0 NMOS P L =V DD *I DDL Dynamic power dissipation important 2 P AC = f C L V DD

21 Bi NMOS Time to change output half-way Assume current stays equal to initial value after switching

22 Bi NMOS Fan-Out Fan out limited by tpmax emposed by system design

23 Bi design Design the pull-down network Select the Kp of pull-up transistor Pull-down network: Write down your logic function as f o =NOT(f pd ) The AND blocks in f pd will appear in series The OR block in f pd will appear in parallel Minimization of f pd for reduction in transistor count necessary

ECE 340 Lecture 40 : MOSFET I

ECE 340 Lecture 40 : MOSFET I ECE 340 Lecture 40 : MOSFET I Class Outline: MOS Capacitance-Voltage Analysis MOSFET - Output Characteristics MOSFET - Transfer Characteristics Things you should know when you leave Key Questions How do

More information

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

Microelectronics Circuit Analysis and Design. MOS Capacitor Under Bias: Electric Field and Charge. Basic Structure of MOS Capacitor 9/25/2013 Microelectronics Circuit Analysis and Design Donald A. Neamen Chapter 3 The Field Effect Transistor In this chapter, we will: Study and understand the operation and characteristics of the various types

More information

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

ECE520 VLSI Design. Lecture 5: Basic CMOS Inverter. Payman Zarkesh-Ha ECE520 VLSI Design Lecture 5: Basic CMOS Inverter Payman Zarkesh-Ha Office: ECE Bldg. 230B Office hours: Wednesday 2:00-3:00PM or by appointment E-mail: pzarkesh@unm.edu Slide: 1 Review of Last Lecture

More information

NAME: Last First Signature

NAME: Last First Signature UNIVERSITY OF CALIFORNIA, BERKELEY College of Engineering Department of Electrical Engineering and Computer Sciences EE 130: IC Devices Spring 2003 FINAL EXAMINATION NAME: Last First Signature STUDENT

More information

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

MOSFET Terminals. The voltage applied to the GATE terminal determines whether current can flow between the SOURCE & DRAIN terminals. MOSFET Terminals The voltage applied to the GATE terminal determines whether current can flow between the SOURCE & DRAIN terminals. For an n-channel MOSFET, the SOURCE is biased at a lower potential (often

More information

Gechstudentszone.wordpress.com

Gechstudentszone.wordpress.com UNIT 4: Small Signal Analysis of Amplifiers 4.1 Basic FET Amplifiers In the last chapter, we described the operation of the FET, in particular the MOSFET, and analyzed and designed the dc response of circuits

More information

8. Combinational MOS Logic Circuits

8. Combinational MOS Logic Circuits 8. Combinational MOS Introduction Combinational logic circuits, or gates, witch perform Boolean operations on multiple input variables and determine the output as Boolean functions of the inputs, are the

More information

Electronic Circuits for Mechatronics ELCT 609 Lecture 6: MOS-FET Transistor

Electronic Circuits for Mechatronics ELCT 609 Lecture 6: MOS-FET Transistor Electronic Circuits for Mechatronics ELCT 609 Lecture 6: MOS-FET Transistor Assistant Professor Office: C3.315 E-mail: eman.azab@guc.edu.eg 1 Introduction Why we call it Transistor? The name came as an

More information

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

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

More information

Microelectronics Circuit Analysis and Design

Microelectronics Circuit Analysis and Design Microelectronics Circuit Analysis and Design Donald A. Neamen Chapter 3 The Field Effect Transistor Neamen Microelectronics, 4e Chapter 3-1 In this chapter, we will: Study and understand the operation

More information

Metal Oxide Semiconductor Field-Effect Transistors (MOSFETs)

Metal Oxide Semiconductor Field-Effect Transistors (MOSFETs) Metal Oxide Semiconductor Field-Effect Transistors (MOSFETs) Device Structure N-Channel MOSFET Providing electrons Pulling electrons (makes current flow) + + + Apply positive voltage to gate: Drives away

More information

Shorthand Notation for NMOS and PMOS Transistors

Shorthand Notation for NMOS and PMOS Transistors Shorthand Notation for NMOS and PMOS Transistors Terminal Voltages Mode of operation depends on V g, V d, V s V gs = V g V s V gd = V g V d V ds = V d V s = V gs - V gd Source and drain are symmetric diffusion

More information

EECE 481. MOS Basics Lecture 2

EECE 481. MOS Basics Lecture 2 EECE 481 MOS Basics Lecture 2 Reza Molavi Dept. of ECE University of British Columbia reza@ece.ubc.ca Slides Courtesy : Dr. Res Saleh (UBC), Dr. D. Sengupta (AMD), Dr. B. Razavi (UCLA) 1 PN Junction and

More information

8. Characteristics of Field Effect Transistor (MOSFET)

8. Characteristics of Field Effect Transistor (MOSFET) 1 8. Characteristics of Field Effect Transistor (MOSFET) 8.1. Objectives The purpose of this experiment is to measure input and output characteristics of n-channel and p- channel field effect transistors

More information

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

Lecture 16: MOS Transistor models: Linear models, SPICE models. Context. In the last lecture, we discussed the MOS transistor, and Lecture 16: MOS Transistor models: Linear models, SPICE models Context In the last lecture, we discussed the MOS transistor, and added a correction due to the changing depletion region, called the body

More information

Chapter 6 DIFFERENT TYPES OF LOGIC GATES

Chapter 6 DIFFERENT TYPES OF LOGIC GATES Chapter 6 DIFFERENT TYPES OF LOGIC GATES Lesson 8 NMOS gates Ch06L8-"Digital Principles and Design", Raj Kamal, Pearson Education, 2006 2 Outline NMOS (n-channel based MOSFETs based circuit) NMOS Features

More information

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

EEC 118 Lecture #11: CMOS Design Guidelines Alternative Static Logic Families EEC 118 Lecture #11: CMOS Design Guidelines Alternative Static Logic Families Rajeevan Amirtharajah University of California, Davis Jeff Parkhurst Intel Corporation Announcements Homework 5 this week Lab

More information

problem grade total

problem grade total Fall 2005 6.012 Microelectronic Devices and Circuits Prof. J. A. del Alamo Name: Recitation: November 16, 2005 Quiz #2 problem grade 1 2 3 4 total General guidelines (please read carefully before starting):

More information

Chapter 6 DIFFERENT TYPES OF LOGIC GATES

Chapter 6 DIFFERENT TYPES OF LOGIC GATES Chapter 6 DIFFERENT TYPES OF LOGIC GATES Lesson 9 CMOS gates Ch06L9-"Digital Principles and Design", Raj Kamal, Pearson Education, 2006 2 Outline CMOS (n-channel based MOSFETs based circuit) CMOS Features

More information

CHAPTER 3 PERFORMANCE OF A TWO INPUT NAND GATE USING SUBTHRESHOLD LEAKAGE CONTROL TECHNIQUES

CHAPTER 3 PERFORMANCE OF A TWO INPUT NAND GATE USING SUBTHRESHOLD LEAKAGE CONTROL TECHNIQUES CHAPTER 3 PERFORMANCE OF A TWO INPUT NAND GATE USING SUBTHRESHOLD LEAKAGE CONTROL TECHNIQUES 41 In this chapter, performance characteristics of a two input NAND gate using existing subthreshold leakage

More information

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

MOSFET & IC Basics - GATE Problems (Part - I) MOSFET & IC Basics - GATE Problems (Part - I) 1. Channel current is reduced on application of a more positive voltage to the GATE of the depletion mode n channel MOSFET. (True/False) [GATE 1994: 1 Mark]

More information

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

Depletion-mode operation ( 공핍형 ): Using an input gate voltage to effectively decrease the channel size of an FET Ch. 13 MOSFET Metal-Oxide-Semiconductor Field-Effect Transistor : I D D-mode E-mode V g The gate oxide is made of dielectric SiO 2 with e = 3.9 Depletion-mode operation ( 공핍형 ): Using an input gate voltage

More information

Field Effect Transistors (FET s) University of Connecticut 136

Field Effect Transistors (FET s) University of Connecticut 136 Field Effect Transistors (FET s) University of Connecticut 136 Field Effect Transistors (FET s) FET s are classified three ways: by conduction type n-channel - conduction by electrons p-channel - conduction

More information

Design cycle for MEMS

Design cycle for MEMS Design cycle for MEMS Design cycle for ICs IC Process Selection nmos CMOS BiCMOS ECL for logic for I/O and driver circuit for critical high speed parts of the system The Real Estate of a Wafer MOS Transistor

More information

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

6.976 High Speed Communication Circuits and Systems Lecture 5 High Speed, Broadband Amplifiers 6.976 High Speed Communication Circuits and Systems Lecture 5 High Speed, Broadband Amplifiers Michael Perrott Massachusetts Institute of Technology Copyright 2003 by Michael H. Perrott Broadband Communication

More information

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

Introduction to MOSFET MOSFET (Metal Oxide Semiconductor Field Effect Transistor) Microelectronic Circuits Introduction to MOSFET MOSFET (Metal Oxide Semiconductor Field Effect Transistor) Slide 1 MOSFET Construction MOSFET (Metal Oxide Semiconductor Field Effect Transistor) Slide 2

More information

MOS Capacitance and Introduction to MOSFETs

MOS Capacitance and Introduction to MOSFETs ECE-305: Fall 2016 MOS Capacitance and Introduction to MOSFETs Professor Peter Bermel Electrical and Computer Engineering Purdue University, West Lafayette, IN USA pbermel@purdue.edu 11/4/2016 Pierret,

More information

Week 9a OUTLINE. MOSFET I D vs. V GS characteristic Circuit models for the MOSFET. Reading. resistive switch model small-signal model

Week 9a OUTLINE. MOSFET I D vs. V GS characteristic Circuit models for the MOSFET. Reading. resistive switch model small-signal model Week 9a OUTLINE MOSFET I vs. V GS characteristic Circuit models for the MOSFET resistive switch model small-signal model Reading Rabaey et al.: Chapter 3.3.2 Hambley: Chapter 12 (through 12.5); Section

More information

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

Field-Effect Transistor (FET) is one of the two major transistors; FET derives its name from its working mechanism; Chapter 3 Field-Effect Transistors (FETs) 3.1 Introduction Field-Effect Transistor (FET) is one of the two major transistors; FET derives its name from its working mechanism; The concept has been known

More information

Lecture-45. MOS Field-Effect-Transistors Threshold voltage

Lecture-45. MOS Field-Effect-Transistors Threshold voltage Lecture-45 MOS Field-Effect-Transistors 7.4. Threshold voltage In this section we summarize the calculation of the threshold voltage and discuss the dependence of the threshold voltage on the bias applied

More information

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

ECE520 VLSI Design. Lecture 2: Basic MOS Physics. Payman Zarkesh-Ha ECE520 VLSI Design Lecture 2: Basic MOS Physics Payman Zarkesh-Ha Office: ECE Bldg. 230B Office hours: Wednesday 2:00-3:00PM or by appointment E-mail: pzarkesh@unm.edu Slide: 1 Review of Last Lecture Semiconductor

More information

Lecture 4. The CMOS Inverter. DC Transfer Curve: Load line. DC Operation: Voltage Transfer Characteristic. Noise in Digital Integrated Circuits

Lecture 4. The CMOS Inverter. DC Transfer Curve: Load line. DC Operation: Voltage Transfer Characteristic. Noise in Digital Integrated Circuits Noise in Digital Integrated Circuits Lecture 4 The CMOS Inverter i(t) v(t) V DD Peter Cheung Department of Electrical & Electronic Engineering Imperial College London URL: www.ee.ic.ac.uk/pcheung/ E-mail:

More information

Prof. Paolo Colantonio a.a

Prof. Paolo Colantonio a.a Prof. Paolo Colantonio a.a. 20 2 Field effect transistors (FETs) are probably the simplest form of transistor, widely used in both analogue and digital applications They are characterised by a very high

More information

IENGINEERS-CONSULTANTS QUESTION BANK SERIES ELECTRONICS ENGINEERING 1 YEAR UPTU ELECTRONICS ENGINEERING EC 101 UNIT 3 (JFET AND MOSFET)

IENGINEERS-CONSULTANTS QUESTION BANK SERIES ELECTRONICS ENGINEERING 1 YEAR UPTU ELECTRONICS ENGINEERING EC 101 UNIT 3 (JFET AND MOSFET) ELECTRONICS ENGINEERING EC 101 UNIT 3 (JFET AND MOSFET) LONG QUESTIONS (10 MARKS) 1. Draw the construction diagram and explain the working of P-Channel JFET. Also draw the characteristics curve and transfer

More information

EE5320: Analog IC Design

EE5320: Analog IC Design EE5320: Analog IC Design Handout 3: MOSFETs Saurabh Saxena & Qadeer Khan Indian Institute of Technology Madras Copyright 2018 by EE6:Integrated Circuits & Systems roup @ IIT Madras Overview Transistors

More information

ENEE 307 Laboratory#2 (n-mosfet, p-mosfet, and a single n-mosfet amplifier in the common source configuration)

ENEE 307 Laboratory#2 (n-mosfet, p-mosfet, and a single n-mosfet amplifier in the common source configuration) Revised 2/16/2007 ENEE 307 Laboratory#2 (n-mosfet, p-mosfet, and a single n-mosfet amplifier in the common source configuration) *NOTE: The text mentioned below refers to the Sedra/Smith, 5th edition.

More information

ELEC 2210 EXPERIMENT 12 NMOS Logic

ELEC 2210 EXPERIMENT 12 NMOS Logic ELEC 2210 EXPERIMENT 12 NMOS Logic Objectives: The experiments in this laboratory exercise will provide an introduction to NMOS logic. You will use the Bit Bucket breadboarding system to build and test

More information

Semiconductor Physics and Devices

Semiconductor Physics and Devices Metal-Semiconductor and Semiconductor Heterojunctions The Metal-Oxide-Semiconductor Field-Effect Transistor (MOSFET) is one of two major types of transistors. The MOSFET is used in digital circuit, because

More information

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

! PN Junction. ! MOS Transistor Topology. ! Threshold. ! Operating Regions.  Resistive.  Saturation.  Subthreshold (next class) ESE370: ircuit-level Modeling, Design, and Optimization for Digital Systems Today! PN Junction! MOS Transistor Topology! Threshold Lec 7: September 16, 2015 MOS Transistor Operating Regions Part 1! Operating

More information

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

Metal-Oxide-Silicon (MOS) devices PMOS. n-type Metal-Oxide-Silicon (MOS devices Principle of MOS Field Effect Transistor transistor operation Metal (poly gate on oxide between source and drain Source and drain implants of opposite type to substrate.

More information

EE105 Fall 2015 Microelectronic Devices and Circuits

EE105 Fall 2015 Microelectronic Devices and Circuits EE105 Fall 2015 Microelectronic Devices and Circuits Prof. Ming C. Wu wu@eecs.berkeley.edu 511 Sutardja Dai Hall (SDH) 11-1 Transistor Operating Mode in Amplifiers Transistors are biased in flat part of

More information

Introduction to Electronic Devices

Introduction to Electronic Devices Introduction to Electronic Devices (Course Number 300331) Fall 2006 Dr. Dietmar Knipp Assistant Professor of Electrical Engineering Information: http://www.faculty.iubremen.de/dknipp/ Source: Apple Ref.:

More information

Chapter 4 Single-stage MOS amplifiers

Chapter 4 Single-stage MOS amplifiers Chapter 4 Single-stage MOS amplifiers ELEC-H402/CH4: Single-stage MOS amplifiers 1 Single-stage MOS amplifiers NMOS as an amplifier: example of common-source circuit NMOS amplifier example Introduction

More information

Field Effect Transistors

Field Effect Transistors Field Effect Transistors LECTURE NO. - 41 Field Effect Transistors www.mycsvtunotes.in JFET MOSFET CMOS Field Effect transistors - FETs First, why are we using still another transistor? BJTs had a small

More information

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

Lecture 16. Complementary metal oxide semiconductor (CMOS) CMOS 1-1 Lecture 16 Complementary metal oxide semiconductor (CMOS) CMOS 1-1 Outline Complementary metal oxide semiconductor (CMOS) Inverting circuit Properties Operating points Propagation delay Power dissipation

More information

Lecture # 16 Logic with a State Dependent Device. Logic Gates How are they built in practice?

Lecture # 16 Logic with a State Dependent Device. Logic Gates How are they built in practice? EECS 42 Introduction to Digital Electronics Andrew R. Neureuther These viewgraphs will be handed out in class 1/21/ Lecture # 16 Logic with a State Dependent Device S&O pp. 9-9, 4-6 (read for graphs and

More information

COMPARISON OF THE MOSFET AND THE BJT:

COMPARISON OF THE MOSFET AND THE BJT: COMPARISON OF THE MOSFET AND THE BJT: In this section we present a comparison of the characteristics of the two major electronic devices: the MOSFET and the BJT. To facilitate this comparison, typical

More information

EE105 Fall 2015 Microelectronic Devices and Circuits: MOSFET Prof. Ming C. Wu 511 Sutardja Dai Hall (SDH)

EE105 Fall 2015 Microelectronic Devices and Circuits: MOSFET Prof. Ming C. Wu 511 Sutardja Dai Hall (SDH) EE105 Fall 2015 Microelectronic Devices and Circuits: MOSFET Prof. Ming C. Wu wu@eecs.berkeley.edu 511 Sutardja Dai Hall (SDH) 7-1 Simplest Model of MOSFET (from EE16B) 7-2 CMOS Inverter 7-3 CMOS NAND

More information

ECEN325: Electronics Summer 2018

ECEN325: Electronics Summer 2018 ECEN325: Electronics Summer 2018 Metal-Oxide-Semiconductor Field Effect Transistor (MOSFET) Sam Palermo Analog & Mixed-Signal Center Texas A&M University Announcements & Reading H5 due today Exam 2 on

More information

CPE/EE 427, CPE 527 VLSI Design I CMOS Inverter. CMOS Inverter: A First Look

CPE/EE 427, CPE 527 VLSI Design I CMOS Inverter. CMOS Inverter: A First Look CPE/EE 427, CPE 527 VLSI Design I CMOS Inverter Department of Electrical and Computer Engineering University of Alabama in Huntsville Aleksandar Milenkovic CMOS Inverter: A First Look C L 9/11/26 VLSI

More information

INTRODUCTION TO ELECTRONICS EHB 222E

INTRODUCTION TO ELECTRONICS EHB 222E INTRODUCTION TO ELECTRONICS EHB 222E MOS Field Effect Transistors (MOSFETS II) MOSFETS 1/ INTRODUCTION TO ELECTRONICS 1 MOSFETS Amplifiers Cut off when v GS < V t v DS decreases starting point A, once

More information

Digital Integrated Circuits - Logic Families (Part II)

Digital Integrated Circuits - Logic Families (Part II) Digital Integrated Circuits - Logic Families (Part II) MOSFET Logic Circuits MOSFETs are unipolar devices. They are simple, small in size, inexpensive to fabricate and consume less power. MOS fabrication

More information

MOS TRANSISTOR THEORY

MOS TRANSISTOR THEORY MOS TRANSISTOR THEORY Introduction A MOS transistor is a majority-carrier device, in which the current in a conducting channel between the source and the drain is modulated by a voltage applied to the

More information

Lecture 11 Circuits numériques (I) L'inverseur

Lecture 11 Circuits numériques (I) L'inverseur Lecture 11 Circuits numériques (I) L'inverseur Outline Introduction to digital circuits The inverter NMOS inverter with resistor pull-up 6.12 Spring 24 Lecture 11 1 1. Introduction to digital circuits:

More information

Electronic CAD Practical work. Week 1: Introduction to transistor models. curve tracing of NMOS transfer characteristics

Electronic CAD Practical work. Week 1: Introduction to transistor models. curve tracing of NMOS transfer characteristics Electronic CAD Practical work Dr. Martin John Burbidge Lancashire UK Tel: +44 (0)1524 825064 Email: martin@mjb-rfelectronics-synthesis.com Martin Burbidge 2006 Week 1: Introduction to transistor models

More information

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

CMOS Digital Logic Design with Verilog. Chapter1 Digital IC Design &Technology CMOS Digital Logic Design with Verilog Chapter1 Digital IC Design &Technology Chapter Overview: In this chapter we study the concept of digital hardware design & technology. This chapter deals the standard

More information

Power dissipation in CMOS

Power dissipation in CMOS DC Current in For V IN < V TN, N O is cut off and I DD = 0. For V TN < V IN < V DD /2, N O is saturated. For V DD /2 < V IN < V DD +V TP, P O is saturated. For V IN > V DD + V TP, P O is cut off and I

More information

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

ECEN 474/704 Lab 5: Frequency Response of Inverting Amplifiers ECEN 474/704 Lab 5: Frequency Response of Inverting Amplifiers Objective Design, simulate and layout various inverting amplifiers. Introduction Inverting amplifiers are fundamental building blocks of electronic

More information

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

D n ox GS THN DS GS THN DS GS THN. D n ox GS THN DS GS THN DS GS THN Name: EXAM #3 Closed book, closed notes. Calculators may be used for numeric computations only. All work is to be your own - show your work for maximum partial credit. Data: Use the following data in all

More information

Department of Electrical Engineering IIT Madras

Department of Electrical Engineering IIT Madras Department of Electrical Engineering IIT Madras Sample Questions on Semiconductor Devices EE3 applicants who are interested to pursue their research in microelectronics devices area (fabrication and/or

More information

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

ECE 340 Lecture 37 : Metal- Insulator-Semiconductor FET Class Outline: ECE 340 Lecture 37 : Metal- Insulator-Semiconductor FET Class Outline: Metal-Semiconductor Junctions MOSFET Basic Operation MOS Capacitor Things you should know when you leave Key Questions What is the

More information

Field Effect Transistors (npn)

Field Effect Transistors (npn) Field Effect Transistors (npn) gate drain source FET 3 terminal device channel e - current from source to drain controlled by the electric field generated by the gate base collector emitter BJT 3 terminal

More information

DIGITAL VLSI LAB ASSIGNMENT 1

DIGITAL VLSI LAB ASSIGNMENT 1 DIGITAL VLSI LAB ASSIGNMENT 1 Problem 1: NMOS and PMOS plots using Cadence. In this exercise, you are required to generate both NMOS and PMOS I-V device characteristics (I/P and O/P) using Cadence (Use

More information

CHAPTER 8 FIELD EFFECT TRANSISTOR (FETs)

CHAPTER 8 FIELD EFFECT TRANSISTOR (FETs) CHAPTER 8 FIELD EFFECT TRANSISTOR (FETs) INTRODUCTION - FETs are voltage controlled devices as opposed to BJT which are current controlled. - There are two types of FETs. o Junction FET (JFET) o Metal

More information

Session 10: Solid State Physics MOSFET

Session 10: Solid State Physics MOSFET Session 10: Solid State Physics MOSFET 1 Outline A B C D E F G H I J 2 MOSCap MOSFET Metal-Oxide-Semiconductor Field-Effect Transistor: Al (metal) SiO2 (oxide) High k ~0.1 ~5 A SiO2 A n+ n+ p-type Si (bulk)

More information

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

Lecture 13. Biasing and Loading Single Stage FET Amplifiers. The Building Blocks of Analog Circuits - III Lecture 3 Biasing and Loading Single Stage FET Amplifiers The Building Blocks of Analog Circuits III In this lecture you will learn: Current biasing of circuits Current sources and sinks for CS, CG, and

More information

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

UNIT-1 Bipolar Junction Transistors. Text Book:, Microelectronic Circuits 6 ed., by Sedra and Smith, Oxford Press UNIT-1 Bipolar Junction Transistors Text Book:, Microelectronic Circuits 6 ed., by Sedra and Smith, Oxford Press Figure 6.1 A simplified structure of the npn transistor. Microelectronic Circuits, Sixth

More information

BJT Amplifier. Superposition principle (linear amplifier)

BJT Amplifier. Superposition principle (linear amplifier) BJT Amplifier Two types analysis DC analysis Applied DC voltage source AC analysis Time varying signal source Superposition principle (linear amplifier) The response of a linear amplifier circuit excited

More information

Lecture 11 Digital Circuits (I) THE INVERTER

Lecture 11 Digital Circuits (I) THE INVERTER Lecture 11 Digital Circuits (I) THE INVERTER Outline Introduction to digital circuits The inverter NMOS inverter with resistor pull-up Reading Assignment: Howe and Sodini; Chapter 5, Sections 5.1-5.3 6.12

More information

ECE 3110: Engineering Electronics II Fall Final Exam. Dec. 16, 8:00-10:00am. Name: (78 points total)

ECE 3110: Engineering Electronics II Fall Final Exam. Dec. 16, 8:00-10:00am. Name: (78 points total) Final Exam Dec. 16, 8:00-10:00am Name: (78 points total) Problem 1: Consider the emitter follower in Fig. 7, which is being used as an output stage. For Q 1, assume β = and initally assume that V BE =

More information

ECE/CoE 0132: FETs and Gates

ECE/CoE 0132: FETs and Gates ECE/CoE 0132: FETs and Gates Kartik Mohanram September 6, 2017 1 Physical properties of gates Over the next 2 lectures, we will discuss some of the physical characteristics of integrated circuits. We will

More information

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

EE 42/100 Lecture 23: CMOS Transistors and Logic Gates. Rev A 4/15/2012 (10:39 AM) Prof. Ali M. Niknejad A. M. Niknejad University of California, Berkeley EE 100 / 42 Lecture 23 p. 1/16 EE 42/100 Lecture 23: CMOS Transistors and Logic Gates ELECTRONICS Rev A 4/15/2012 (10:39 AM) Prof. Ali M. Niknejad University

More information

MEASUREMENT AND INSTRUMENTATION STUDY NOTES UNIT-I

MEASUREMENT AND INSTRUMENTATION STUDY NOTES UNIT-I MEASUREMENT AND INSTRUMENTATION STUDY NOTES The MOSFET The MOSFET Metal Oxide FET UNIT-I As well as the Junction Field Effect Transistor (JFET), there is another type of Field Effect Transistor available

More information

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

UNIVERSITY OF CALIFORNIA AT BERKELEY College of Engineering Department of Electrical Engineering and Computer Sciences. UNIVERSITY OF CALIFORNIA AT BERKELEY College of Engineering Department of Electrical Engineering and Computer Sciences Discussion #9 EE 05 Spring 2008 Prof. u MOSFETs The standard MOSFET structure is shown

More information

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

Improved Inverter: Current-Source Pull-Up. MOS Inverter with Current-Source Pull-Up. What else could be connected between the drain and V DD? Improved Inverter: Current-Source Pull-Up MOS Inverter with Current-Source Pull-Up What else could be connected between the drain and? Replace resistor with current source I SUP roc i D v IN v OUT Find

More information

University of Pittsburgh

University of Pittsburgh University of Pittsburgh Experiment #4 Lab Report MOSFET Amplifiers and Current Mirrors Submission Date: 07/03/2018 Instructors: Dr. Ahmed Dallal Shangqian Gao Submitted By: Nick Haver & Alex Williams

More information

3.CMOS Inverter-homework

3.CMOS Inverter-homework 3.CMOS Inverter-homework 1. for a CMOS inverter, when the pmos and nmos are long-channel devices,or when the supply voltage is low, velocity does not occur, under these circumstances,vm(vin=vout)=? 2.

More information

CMOS VLSI Design (A3425)

CMOS VLSI Design (A3425) CMOS VLSI Design (A3425) Unit III Static Logic Gates Introduction A static logic gate is one that has a well defined output once the inputs are stabilized and the switching transients have decayed away.

More information

MOSFET as a Switch. MOSFET Characteristics Curves

MOSFET as a Switch. MOSFET Characteristics Curves MOSFET as a Switch MOSFET s make very good electronic switches for controlling loads and in CMOS digital circuits as they operate between their cut-off and saturation regions. We saw previously, that the

More information

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

Digital Electronics. By: FARHAD FARADJI, Ph.D. Assistant Professor, Electrical and Computer Engineering, K. N. Toosi University of Technology K. N. Toosi University of Technology Chapter 7. Field-Effect Transistors By: FARHAD FARADJI, Ph.D. Assistant Professor, Electrical and Computer Engineering, K. N. Toosi University of Technology http://wp.kntu.ac.ir/faradji/digitalelectronics.htm

More information

Power and Energy. Courtesy of Dr. Daehyun Dr. Dr. Shmuel and Dr.

Power and Energy. Courtesy of Dr. Daehyun Dr. Dr. Shmuel and Dr. Power and Energy Courtesy of Dr. Daehyun Lim@WSU, Dr. Harris@HMC, Dr. Shmuel Wimer@BIU and Dr. Choi@PSU http://csce.uark.edu +1 (479) 575-6043 yrpeng@uark.edu The Chip is HOT Power consumption increases

More information

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

Conduction Characteristics of MOS Transistors (for fixed Vds)! Topic 2. Basic MOS theory & SPICE simulation. MOS Transistor Conduction Characteristics of MOS Transistors (for fixed Vds)! Topic 2 Basic MOS theory & SPICE simulation Peter Cheung Department of Electrical & Electronic Engineering Imperial College London (Weste&Harris,

More information

Topic 2. Basic MOS theory & SPICE simulation

Topic 2. Basic MOS theory & SPICE simulation Topic 2 Basic MOS theory & SPICE simulation Peter Cheung Department of Electrical & Electronic Engineering Imperial College London (Weste&Harris, Ch 2 & 5.1-5.3 Rabaey, Ch 3) URL: www.ee.ic.ac.uk/pcheung/

More information

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

Conduction Characteristics of MOS Transistors (for fixed Vds) Topic 2. Basic MOS theory & SPICE simulation. MOS Transistor Conduction Characteristics of MOS Transistors (for fixed Vds) Topic 2 Basic MOS theory & SPICE simulation Peter Cheung Department of Electrical & Electronic Engineering Imperial College London (Weste&Harris,

More information

Basic Electronics Prof. Dr. Chitralekha Mahanta Department of Electronics and Communication Engineering Indian Institute of Technology, Guwahati

Basic Electronics Prof. Dr. Chitralekha Mahanta Department of Electronics and Communication Engineering Indian Institute of Technology, Guwahati Basic Electronics Prof. Dr. Chitralekha Mahanta Department of Electronics and Communication Engineering Indian Institute of Technology, Guwahati Module: 3 Field Effect Transistors Lecture-3 MOSFET UNDER

More information

Session 2 MOS Transistor for RF Circuits

Session 2 MOS Transistor for RF Circuits Session 2 MOS Transistor for RF Circuits Session Speaker Chandramohan P. Session Contents MOS transistor basics MOS equivalent circuit Single stage amplifiers Opamp design Session objectives To understand

More information

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

Week 7: Common-Collector Amplifier, MOS Field Effect Transistor EE 2110A Electronic Circuits Week 7: Common-Collector Amplifier, MOS Field Effect Transistor ecture 07-1 Topics to coer Common-Collector Amplifier MOS Field Effect Transistor Physical Operation and I-V

More information

Contents 1 Introduction 2 MOS Fabrication Technology

Contents 1 Introduction 2 MOS Fabrication Technology Contents 1 Introduction... 1 1.1 Introduction... 1 1.2 Historical Background [1]... 2 1.3 Why Low Power? [2]... 7 1.4 Sources of Power Dissipations [3]... 9 1.4.1 Dynamic Power... 10 1.4.2 Static Power...

More information

ELEC 350L Electronics I Laboratory Fall 2012

ELEC 350L Electronics I Laboratory Fall 2012 ELEC 350L Electronics I Laboratory Fall 2012 Lab #9: NMOS and CMOS Inverter Circuits Introduction The inverter, or NOT gate, is the fundamental building block of most digital devices. The circuits used

More information

ECE 546 Lecture 12 Integrated Circuits

ECE 546 Lecture 12 Integrated Circuits ECE 546 Lecture 12 Integrated Circuits Spring 2018 Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois jesa@illinois.edu ECE 546 Jose Schutt Aine 1 Integrated Circuits IC Requirements

More information

Lecture 24 - The Si surface and the Metal-Oxide-Semiconductor Structure (cont.) The Long Metal-Oxide-Semiconductor Field-Effect Transistor

Lecture 24 - The Si surface and the Metal-Oxide-Semiconductor Structure (cont.) The Long Metal-Oxide-Semiconductor Field-Effect Transistor 6.720J/3.43J - Integrated Microelectronic Devices - Spring 2007 Lecture 24-1 Lecture 24 - The Si surface and the Metal-Oxide-Semiconductor Structure (cont.) The Long Metal-Oxide-Semiconductor Field-Effect

More information

MOS Field Effect Transistors

MOS Field Effect Transistors MOS Field Effect Transistors A gate contact gate interconnect n polysilicon gate source contacts W active area (thin oxide area) polysilicon gate contact metal interconnect drain contacts A bulk contact

More information

ECE 334: Electronic Circuits Lecture 10: Digital CMOS Circuits

ECE 334: Electronic Circuits Lecture 10: Digital CMOS Circuits Faculty of Engineering ECE 334: Electronic Circuits Lecture 10: Digital CMOS Circuits CMOS Technology Complementary MOS, or CMOS, needs both PMOS and NMOS FET devices for their logic gates to be realized

More information

MOS Field-Effect Transistors (MOSFETs)

MOS Field-Effect Transistors (MOSFETs) 6 MOS Field-Effect Transistors (MOSFETs) A three-terminal device that uses the voltages of the two terminals to control the current flowing in the third terminal. The basis for amplifier design. The basis

More information

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

Chapter 4. CMOS Cascode Amplifiers. 4.1 Introduction. 4.2 CMOS Cascode Amplifiers Chapter 4 CMOS Cascode Amplifiers 4.1 Introduction A single stage CMOS amplifier cannot give desired dc voltage gain, output resistance and transconductance. The voltage gain can be made to attain higher

More information

Designing Information Devices and Systems II Fall 2017 Note 1

Designing Information Devices and Systems II Fall 2017 Note 1 EECS 16B Designing Information Devices and Systems II Fall 2017 Note 1 1 Digital Information Processing Electrical circuits manipulate voltages (V ) and currents (I) in order to: 1. Process information

More information

EEC 118 Spring 2010 Lab #1: NMOS and PMOS Transistor Parameters

EEC 118 Spring 2010 Lab #1: NMOS and PMOS Transistor Parameters EEC 118 Spring 2010 Lab #1: NMOS and PMOS Transistor Parameters Dept. of Electrical and Computer Engineering University of California, Davis March 18, 2010 Reading: Rabaey Chapter 3 [1]. Reference: Kang

More information

Module 4 : Propagation Delays in MOS Lecture 19 : Analyzing Delay for various Logic Circuits

Module 4 : Propagation Delays in MOS Lecture 19 : Analyzing Delay for various Logic Circuits Module 4 : Propagation Delays in MOS Lecture 19 : Analyzing Delay for various Logic Circuits Objectives In this lecture you will learn the following Ratioed Logic Pass Transistor Logic Dynamic Logic Circuits

More information

Digital circuits. Bởi: Sy Hien Dinh

Digital circuits. Bởi: Sy Hien Dinh Digital circuits Bởi: Sy Hien Dinh This module presents the basic concepts of MOSFET digital logic circuits. We will examine NMOS logic circuits, which contain only n-channel transistors, and complementary

More information

Digital Electronics. Assign Ò1Ó and Ò0Ó to a range of voltage (or current), with a separation that minimizes a transition region.

Digital Electronics. Assign Ò1Ó and Ò0Ó to a range of voltage (or current), with a separation that minimizes a transition region. Digital Electronics Assign Ò1Ó and Ò0Ó to a range of voltage (or current), with a separation that minimizes a transition region Positive Logic Logic 1 Negative Logic Logic 0 Voltage Transition egion Transition

More information