EE115C Winter 2017 Digital Electronic Circuits. Lecture 3: MOS RC Model, CMOS Manufacturing

Size: px
Start display at page:

Download "EE115C Winter 2017 Digital Electronic Circuits. Lecture 3: MOS RC Model, CMOS Manufacturing"

Transcription

1 EE115C Winter 2017 Digital Electronic Circuits Lecture 3: MOS RC Model, CMOS Manufacturing

2 Agenda MOS Transistor: RC Model (pp ) S R on D CMOS Manufacturing Process (pp ) S S C GS G G C GD D D C SB C GB C DB B EE115C Winter

3 Switch Model of CMOS Transistor V GS G NMOS: V GS > 0 PMOS: V GS < 0 S D S R on D S V GS < V T V GS > V T D EE115C Winter

4 The Transistor as a Switch MOS can be treated as equivalent resistance Calculating MOS resistance: S V GS V T R on D I D R mid V GS = V DD R 0 good approximation (I-V linear) V DD /2 V DD V DS This model will be used for delay analysis EE115C Winter

5 Computing Equivalent Resistance (1/2) Method 1 ( exact ): by integration EE115C Winter

6 Computing Equivalent Resistance (2/2) Method 2: simple averaging The averaging works because of approximately linear dependence of I DS on V DS (recall the CLM model) Use this formula for hand analysis EE115C Winter

7 R eq (Ohm) R on vs. V DD (Simulation Result) R on increases rapidly as V DD approaches V T 7 x W/L=1, L=0.25 m V DD (V) EE115C Winter

8 MOS Capacitances G C GS C GD S D C SB C GB C DB B EE115C Winter

9 The Gate Capacitance Polysilicon gate Source n + x d x d W Drain n + L d Top view Gate-bulk overlap C gate t ox ox WL Gate oxide t ox n + L n + Cross section EE115C Winter

10 Capacitance Components #1: Gate-Channel Capacitance #2: Gate Overlap Capacitance #3: Junction/Diffusion Capacitance EE115C Winter

11 #1: Gate-Channel Capacitance G G G S C GC C GC C GC D S D S D Cut-off Resistive Saturation C GCB C GCS C GCD Textbook: page 109 Most important regions in digital design: saturation and cut-off EE115C Winter

12 A Close Look at Gate-Channel Capacitance C GC WLC ox WLC ox C GC WLC ox 2 C GCB C GCS =C GCD WLC ox 2 C GCS C GCD 2WLC ox 3 V GS 0 1 V DS / (V GS V T ) C gate as a function of V GS (with V DS = 0) C gate as a function of the degree of saturation EE115C Winter

13 Summary: #1: Gate-Channel Capacitance G G G C GC C GC C GC S D S D S D Cut-off Resistive Saturation C GCB C GCS C GCD Textbook: page 109 Off/Lin C gate = C ox W L eff ox Cox Sat C gate = (2/3) C ox W L eff tox EE115C Winter

14 Source #2: Gate Overlap Capacitance n + x d x d W Drain n + Polysilicon gate L d Top view Gate-bulk overlap Gate oxide Source n + x d L d Top view x d W Drain n + Gate-bulk overlap t ox n + L n + Cross section C O C ox x d Gate oxide t ox n + L n + Off/Lin/Sat C GSO = C GDO = C O W Cross section EE115C Winter

15 Capacitance (F) Measuring the Gate Cap Transient analysis 10 9 x V GS 7 I Gate Capacitance (F) V GS (V) EE115C Winter

16 Finding Equivalent Capacitance Delay Curve fitting approach to find a number that works for hand analysis of the gate delay Understand the limitations: the model will depend on signal rise times, voltage, temperature, process parameter variation t p1 t p2 c gate Experiment: find C gate to match propagation delays t p1 = t p2 C gate is equivalent cap of the green gate EE115C Winter

17 #3: Diffusion Capacitance Channel-stop implant N A + W Bottom Side wall Source N D x j Side wall L S Channel Substrate N A C diff = C bottom + C sw = C j AREA + C jsw PERIMETER = C j L S W + C jsw (2L S + W) EE115C Winter

18 #3: Diffusion Capacitance Channel-stop implant N A + W Bottom Side wall Source N D x j Side wall L S Channel Substrate N A C diff = C bottom + C sw = C j AREA + C jsw PERIMETER Off/Lin/Sat C diff = C j L S W + C jsw (2L S +W) EE115C Winter

19 Junction Capacitance is Bias-dependent C j C j0 (1 V ) D 0 m m = 0.5: abrupt junction m = 0.33: linear junction EE115C Winter

20 #3 Diffusion Capacitance: Summary of Equations Bottom-plate C Side-wall C m = 0.5: abrupt junction m = 0.33: linear junction EE115C Winter

21 Linearizing the Junction Cap Replace non-linear capacitance by large-signal equivalent linear capacitance, which displaces equal charge over voltage swing of interest Typical value for K eq around 0.5 EE115C Winter

22 Summary: Capacitive Device Model Gate-Channel Capacitance C GC = C ox W L eff (Off, Linear) C GC = (2/3) C ox W L eff (Saturation) Circuit design C gate Gate Overlap Capacitance C GSO = C GDO = C O W (Always) Junction/Diffusion Capacitance C diff = C j L S W + C jsw (2L S + W) (Always) C parasitic Zero-bias C diff > C gate MOS On C diff C gate EE115C Winter

23 Outline MOS Transistor: RC Model (pp ) CMOS Manufacturing Process (pp ) EE115C Winter

24 Photo-Lithographic Process oxidation optical mask photoresist removal (ashing) photoresist coating stepper exposure process step Typical operations in a single photolithographic cycle (from [Fullman]). spin, rinse, dry acid etch photoresist development EE115C Winter

25 Patterning of SiO 2 Si-substrate (a) Silicon base material Si-substrate (b) After oxidation and deposition of negative photoresist Si-substrate (c) Stepper exposure Photoresist SiO 2 UV-light Patterned optical mask Exposed resist Si-substrate Si-substrate Si-substrate Hardened resist SiO 2 (d) After development and etching of resist, chemical or plasma etch of SiO 2 (e) After etching Chemical or plasma etch Hardened resist SiO 2 SiO 2 (f) Final result after removal of resist EE115C Winter

26 CMOS Process at a Glance Define active areas Etch and fill trenches Implant well regions Deposit and pattern polysilicon layer Implant source and drain regions and substrate contacts Create contact and via windows Deposit and pattern metal layers EE115C Winter

27 CMOS Process Walk-Through p-epi p+ (a) Base material: p+ substrate with p-epi layer p-epi p+ SiN 3 4 SiO 2 (b) After deposition of gate-oxide and sacrificial nitride (acts as a buffer layer) p+ (c) After plasma etch of insulating trenches using the inverse of the active area mask EE115C Winter

28 CMOS Process Walk-Through SiO 2 (d) After trench filling, CMP planarization, and removal of sacrificial nitride n (e) After n-well and V TP adjust implants p (f) After p-well and V TN adjust implants EE115C Winter

29 CMOS Process Walk-Through poly(silicon) (g) After polysilicon deposition and etch n+ p+ (h) After n+ source/drain and p+ source/drain implants. These steps also dope the polysilicon. SiO 2 (i) After deposition of SiO 2 insulator and contact hole etch. EE115C Winter

30 CMOS Process Walk-Through Al (j) After deposition and patterning of first Al layer. Al SiO 2 (k) After deposition of SiO 2 insulator, etching of via s, deposition and patterning of second layer of Al. EE115C Winter

31 Advanced Metalization EE115C Winter

EE141- Spring 2003 Lecture 3. Last Lecture

EE141- Spring 2003 Lecture 3. Last Lecture - Spring 003 Lecture 3 IC Manufacturing 1 Last Lecture Design Metrics (part 1) Today Design metrics (wrap-up) IC manufacturing 1 Administrivia Discussion sessions start this week. Only one this week (Dejan

More information

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

The Devices. Digital Integrated Circuits A Design Perspective. Jan M. Rabaey Anantha Chandrakasan Borivoje Nikolic. July 30, 2002 Digital Integrated Circuits A Design Perspective Jan M. Rabaey Anantha Chandrakasan Borivoje Nikolic The Devices July 30, 2002 Goal of this chapter Present intuitive understanding of device operation Introduction

More information

Check course home page periodically for announcements. Homework 2 is due TODAY by 5pm In 240 Cory

Check course home page periodically for announcements. Homework 2 is due TODAY by 5pm In 240 Cory EE141 Fall 005 Lecture 6 MOS Capacitances, Propagation elay Important! Check course home page periodically for announcements Homework is due TOAY by 5pm In 40 Cory Homework 3 will be posted TOAY ue Thursday

More information

MOSFET: Introduction

MOSFET: Introduction E&CE 437 Integrated VLSI Systems MOS Transistor 1 of 30 MOSFET: Introduction Metal oxide semiconductor field effect transistor (MOSFET) or MOS is widely used for implementing digital designs Its major

More information

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

EEC 116 Lecture #3: CMOS Inverters MOS Scaling. Rajeevan Amirtharajah University of California, Davis Jeff Parkhurst Intel Corporation EEC 116 Lecture #3: CMOS Inverters MOS Scaling Rajeevan Amirtharajah University of California, Davis Jeff Parhurst Intel Corporation Outline Review: Inverter Transfer Characteristics Lecture 3: Noise Margins,

More information

VLSI Design and Simulation

VLSI Design and Simulation VLSI Design and Simulation Performance Characterization Topics Performance Characterization Resistance Estimation Capacitance Estimation Inductance Estimation Performance Characterization Inverter Voltage

More information

Lecture 3: CMOS Transistor Theory

Lecture 3: CMOS Transistor Theory Lecture 3: CMOS Transistor Theory Outline Introduction MOS Capacitor nmos I-V Characteristics pmos I-V Characteristics Gate and Diffusion Capacitance 2 Introduction So far, we have treated transistors

More information

Lecture 4: CMOS Transistor Theory

Lecture 4: CMOS Transistor Theory Introduction to CMOS VLSI Design Lecture 4: CMOS Transistor Theory David Harris, Harvey Mudd College Kartik Mohanram and Steven Levitan University of Pittsburgh Outline q Introduction q MOS Capacitor q

More information

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

EEC 118 Lecture #2: MOSFET Structure and Basic Operation. Rajeevan Amirtharajah University of California, Davis Jeff Parkhurst Intel Corporation EEC 118 Lecture #2: MOSFET Structure and Basic Operation Rajeevan Amirtharajah University of California, Davis Jeff Parkhurst Intel Corporation Announcements Lab 1 this week, report due next week Bring

More information

ESE 570: Digital Integrated Circuits and VLSI Fundamentals

ESE 570: Digital Integrated Circuits and VLSI Fundamentals ESE 570: Digital Integrated Circuits and VLSI Fundamentals Lec 7: February 4, 2016 MOS SPICE Models, MOS Parasitic Details Lecture Outline! MOS Capacitances " Extrinsic " Intrinsic! Lumped Capacitance

More information

! MOS Capacitances. " Extrinsic. " Intrinsic. ! Lumped Capacitance Model. ! First Order Capacitor Summary. ! Capacitance Implications

! MOS Capacitances.  Extrinsic.  Intrinsic. ! Lumped Capacitance Model. ! First Order Capacitor Summary. ! Capacitance Implications ESE 570: Digital Integrated Circuits and VLSI Fundamentals Lec 7: February, 07 MOS SPICE Models, MOS Parasitic Details Lecture Outline! MOS Capacitances " Extrinsic " Intrinsic! Lumped Capacitance Model!

More information

Device Models (PN Diode, MOSFET )

Device Models (PN Diode, MOSFET ) Device Models (PN Diode, MOSFET ) Instructor: Steven P. Levitan steve@ece.pitt.edu TA: Gayatri Mehta, José Martínez Book: Digital Integrated Circuits: A Design Perspective; Jan Rabaey Lab Notes: Handed

More information

MOS Transistor I-V Characteristics and Parasitics

MOS Transistor I-V Characteristics and Parasitics ECEN454 Digital Integrated Circuit Design MOS Transistor I-V Characteristics and Parasitics ECEN 454 Facts about Transistors So far, we have treated transistors as ideal switches An ON transistor passes

More information

The Devices. Devices

The Devices. Devices The The MOS Transistor Gate Oxyde Gate Source n+ Polysilicon Drain n+ Field-Oxyde (SiO 2 ) p-substrate p+ stopper Bulk Contact CROSS-SECTION of NMOS Transistor Cross-Section of CMOS Technology MOS transistors

More information

Device Models (PN Diode, MOSFET )

Device Models (PN Diode, MOSFET ) Device Models (PN Diode, MOSFET ) Instructor: Steven P. Levitan steve@ece.pitt.edu TA: Gayatri Mehta, José Martínez Book: Digital Integrated Circuits: A Design Perspective; Jan Rabaey Lab Notes: Handed

More information

The Devices: MOS Transistors

The Devices: MOS Transistors The Devices: MOS Transistors References: Semiconductor Device Fundamentals, R. F. Pierret, Addison-Wesley Digital Integrated Circuits: A Design Perspective, J. Rabaey et.al. Prentice Hall NMOS Transistor

More information

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

University of Pennsylvania Department of Electrical Engineering. ESE 570 Midterm Exam March 14, 2013 FORMULAS AND DATA University of Pennsylvania Department of Electrical Engineering ESE 570 Midterm Exam March 4, 03 FORMULAS AND DATA. PHYSICAL CONSTANTS: n i = intrinsic concentration undoped) silicon =.45 x 0 0 cm -3 @

More information

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

The Devices. Digital Integrated Circuits A Design Perspective. Jan M. Rabaey Anantha Chandrakasan Borivoje Nikolic. July 30, 2002 igital Integrated Circuits A esign Perspective Jan M. Rabaey Anantha Chandrakasan Borivoje Nikolic The evices July 30, 2002 Goal of this chapter Present intuitive understanding of device operation Introduction

More information

MOS Transistor Properties Review

MOS Transistor Properties Review MOS Transistor Properties Review 1 VLSI Chip Manufacturing Process Photolithography: transfer of mask patterns to the chip Diffusion or ion implantation: selective doping of Si substrate Oxidation: SiO

More information

Chapter 4 Field-Effect Transistors

Chapter 4 Field-Effect Transistors Chapter 4 Field-Effect Transistors Microelectronic Circuit Design Richard C. Jaeger Travis N. Blalock 5/5/11 Chap 4-1 Chapter Goals Describe operation of MOSFETs. Define FET characteristics in operation

More information

The Devices. Jan M. Rabaey

The Devices. Jan M. Rabaey The Devices Jan M. Rabaey Goal of this chapter Present intuitive understanding of device operation Introduction of basic device equations Introduction of models for manual analysis Introduction of models

More information

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

EE105 Fall 2014 Microelectronic Devices and Circuits. NMOS Transistor Capacitances: Saturation Region EE105 Fall 014 Microelectronic Devices and Circuits Prof. Ming C. Wu wu@eecs.berkeley.edu 511 Sutardja Dai Hall (SDH) 1 NMOS Transistor Capacitances: Saturation Region Drain no longer connected to channel

More information

ECE321 Electronics I

ECE321 Electronics I EE31 Electronics I Lecture 8: MOSET Threshold Voltage and Parasitic apacitances Payman Zarkesh-Ha Office: EE Bldg. 3B Office hours: Tuesday :-3:PM or by appointment E-mail: payman@ece.unm.edu Slide: 1

More information

MOS Transistor Theory

MOS Transistor Theory MOS Transistor Theory So far, we have viewed a MOS transistor as an ideal switch (digital operation) Reality: less than ideal EE 261 Krish Chakrabarty 1 Introduction So far, we have treated transistors

More information

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

Introduction to CMOS VLSI. Chapter 2: CMOS Transistor Theory. Harris, 2004 Updated by Li Chen, Outline Introduction to MOS VLSI Design hapter : MOS Transistor Theory copyright@david Harris, 004 Updated by Li hen, 010 Outline Introduction MOS apacitor nmos IV haracteristics pmos IV haracteristics Gate and

More information

Practice 3: Semiconductors

Practice 3: Semiconductors Practice 3: Semiconductors Digital Electronic Circuits Semester A 2012 VLSI Fabrication Process VLSI Very Large Scale Integration The ability to fabricate many devices on a single substrate within a given

More information

EE 560 MOS TRANSISTOR THEORY PART 2. Kenneth R. Laker, University of Pennsylvania

EE 560 MOS TRANSISTOR THEORY PART 2. Kenneth R. Laker, University of Pennsylvania 1 EE 560 MOS TRANSISTOR THEORY PART nmos TRANSISTOR IN LINEAR REGION V S = 0 V G > V T0 channel SiO V D = small 4 C GC C BC substrate depletion region or bulk B p nmos TRANSISTOR AT EDGE OF SATURATION

More information

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

P. R. Nelson 1 ECE418 - VLSI. Midterm Exam. Solutions P. R. Nelson 1 ECE418 - VLSI Midterm Exam Solutions 1. (8 points) Draw the cross-section view for A-A. The cross-section view is as shown below.. ( points) Can you tell which of the metal1 regions is the

More information

Digital Integrated Circuits EECS 312

Digital Integrated Circuits EECS 312 14 12 10 8 6 Fujitsu VP2000 IBM 3090S Pulsar 4 IBM 3090 IBM RY6 CDC Cyber 205 IBM 4381 IBM RY4 2 IBM 3081 Apache Fujitsu M380 IBM 370 Merced IBM 360 IBM 3033 Vacuum Pentium II(DSIP) 0 1950 1960 1970 1980

More information

EE5311- Digital IC Design

EE5311- Digital IC Design EE5311- Digital IC Design Module 1 - The Transistor Janakiraman V Assistant Professor Department of Electrical Engineering Indian Institute of Technology Madras Chennai October 28, 2017 Janakiraman, IITM

More information

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

Chapter 2 CMOS Transistor Theory. Jin-Fu Li Department of Electrical Engineering National Central University Jungli, Taiwan Chapter 2 CMOS Transistor Theory Jin-Fu Li Department of Electrical Engineering National Central University Jungli, Taiwan Outline Introduction MOS Device Design Equation Pass Transistor Jin-Fu Li, EE,

More information

CMPEN 411 VLSI Digital Circuits. Lecture 03: MOS Transistor

CMPEN 411 VLSI Digital Circuits. Lecture 03: MOS Transistor CMPEN 411 VLSI Digital Circuits Lecture 03: MOS Transistor Kyusun Choi [Adapted from Rabaey s Digital Integrated Circuits, Second Edition, 2003 J. Rabaey, A. Chandrakasan, B. Nikolic] CMPEN 411 L03 S.1

More information

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

HW 5 posted due in two weeks Lab this week Midterm graded Project to be launched in week 7 HW 5 posted due in two weeks Lab this week Midterm graded Project to be launched in week 7 2 What do digital IC designers need to know? 5 EE4 EECS4 6 3 0< V GS - V T < V DS Pinch-off 7 For (V GS V T )

More information

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

CMOS INVERTER. Last Lecture. Metrics for qualifying digital circuits. »Cost» Reliability» Speed (delay)»performance CMOS INVERTER Last Lecture Metrics for qualifying digital circuits»cost» Reliability» Speed (delay)»performance 1 Today s lecture The CMOS inverter at a glance An MOS transistor model for manual analysis

More information

VLSI Design The MOS Transistor

VLSI Design The MOS Transistor VLSI Design The MOS Transistor Frank Sill Torres Universidade Federal de Minas Gerais (UFMG), Brazil VLSI Design: CMOS Technology 1 Outline Introduction MOS Capacitor nmos I-V Characteristics pmos I-V

More information

MOS Transistor Theory

MOS Transistor Theory CHAPTER 3 MOS Transistor Theory Outline 2 1. Introduction 2. Ideal I-V Characteristics 3. Nonideal I-V Effects 4. C-V Characteristics 5. DC Transfer Characteristics 6. Switch-level RC Delay Models MOS

More information

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

CMPEN 411 VLSI Digital Circuits. Lecture 04: CMOS Inverter (static view) CMPEN 411 VLSI Digital Circuits Lecture 04: CMOS Inverter (static view) Kyusun Choi [Adapted from Rabaey s Digital Integrated Circuits, Second Edition, 2003 J. Rabaey, A. Chandrakasan, B. Nikolic] CMPEN

More information

Lecture 5: CMOS Transistor Theory

Lecture 5: CMOS Transistor Theory Lecture 5: CMOS Transistor Theory Slides courtesy of Deming Chen Slides based on the initial set from David Harris CMOS VLSI Design Outline q q q q q q q Introduction MOS Capacitor nmos I-V Characteristics

More information

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

Today s lecture. EE141- Spring 2003 Lecture 4. Design Rules CMOS Inverter MOS Transistor Model - Spring 003 Lecture 4 Design Rules CMOS Inverter MOS Transistor Model Today s lecture Design Rules The CMOS inverter at a glance An MOS transistor model for manual analysis Important! Labs start next

More information

ECE 497 JS Lecture - 12 Device Technologies

ECE 497 JS Lecture - 12 Device Technologies ECE 497 JS Lecture - 12 Device Technologies Spring 2004 Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois jose@emlab.uiuc.edu 1 NMOS Transistor 2 ρ Source channel charge density

More information

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

Fig. 1 CMOS Transistor Circuits (a) Inverter Out = NOT In, (b) NOR-gate C = NOT (A or B) 1 Introduction to Transistor-Level Logic Circuits 1 By Prawat Nagvajara At the transistor level of logic circuits, transistors operate as switches with the logic variables controlling the open or closed

More information

CMOS Inverter (static view)

CMOS Inverter (static view) Review: Design Abstraction Levels SYSTEM CMOS Inverter (static view) + MODULE GATE [Adapted from Chapter 5. 5.3 CIRCUIT of G DEVICE Rabaey s Digital Integrated Circuits,, J. Rabaey et al.] S D Review:

More information

Discussions start next week Labs start in week 3 Homework #1 is due next Friday

Discussions start next week Labs start in week 3 Homework #1 is due next Friday EECS141 1 Discussions start next week Labs start in week 3 Homework #1 is due next Friday Everyone should have an EECS instructional account Use cory, quasar, pulsar EECS141 2 1 CMOS LEAKAGE CHARACTERIZATION

More information

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

Digital Integrated Circuits A Design Perspective. Jan M. Rabaey Anantha Chandrakasan Borivoje Nikolic. The Devices. July 30, Devices. Digital Integrated Circuits A Design Perspective Jan M. Rabaey Anantha Chandrakasan Borivoje Nikolic The July 30, 2002 1 Goal of this chapter Present intuitive understanding of device operation Introduction

More information

ECE 342 Electronic Circuits. Lecture 6 MOS Transistors

ECE 342 Electronic Circuits. Lecture 6 MOS Transistors ECE 342 Electronic Circuits Lecture 6 MOS Transistors Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois jesa@illinois.edu 1 NMOS Transistor Typically L = 0.1 to 3 m, W = 0.2

More information

Digital Microelectronic Circuits ( )

Digital Microelectronic Circuits ( ) Digital Microelectronic ircuits (361-1-3021 ) Presented by: Dr. Alex Fish Lecture 5: Parasitic apacitance and Driving a Load 1 Motivation Thus far, we have learned how to model our essential building block,

More information

Lecture 11: MOS Transistor

Lecture 11: MOS Transistor Lecture 11: MOS Transistor Prof. Niknejad Lecture Outline Review: MOS Capacitors Regions MOS Capacitors (3.8 3.9) CV Curve Threshold Voltage MOS Transistors (4.1 4.3): Overview Cross-section and layout

More information

EE 5211 Analog Integrated Circuit Design. Hua Tang Fall 2012

EE 5211 Analog Integrated Circuit Design. Hua Tang Fall 2012 EE 5211 Analog Integrated Circuit Design Hua Tang Fall 2012 Today s topic: 1. Introduction to Analog IC 2. IC Manufacturing (Chapter 2) Introduction What is Integrated Circuit (IC) vs discrete circuits?

More information

EE 560 MOS TRANSISTOR THEORY

EE 560 MOS TRANSISTOR THEORY 1 EE 560 MOS TRANSISTOR THEORY PART 1 TWO TERMINAL MOS STRUCTURE V G (GATE VOLTAGE) 2 GATE OXIDE SiO 2 SUBSTRATE p-type doped Si (N A = 10 15 to 10 16 cm -3 ) t ox V B (SUBSTRATE VOLTAGE) EQUILIBRIUM:

More information

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

EE 330 Lecture 16. MOS Device Modeling p-channel n-channel comparisons Model consistency and relationships CMOS Process Flow EE 330 Lecture 16 MOS Device Modeling p-channel n-channel comparisons Model consistency and relationships CMOS Process Flow Review from Last Time Operation Regions by Applications Id I D 300 250 200 150

More information

Step 1. Finding V M. Goal: Þnd V M = input voltage for the output = V M both transistors are saturated at V IN = V M since

Step 1. Finding V M. Goal: Þnd V M = input voltage for the output = V M both transistors are saturated at V IN = V M since Step 1. Finding V M Goal: Þnd V M = input voltage for the output = V M both transistors are saturated at V IN = V M since V DSn = V M - 0 > V M - V Tn V SDp = V DD - V M = (V DD - V M ) V Tp Equate drain

More information

EE 435. Lecture 37. Parasitic Capacitances in MOS Devices. String DAC Parasitic Capacitances

EE 435. Lecture 37. Parasitic Capacitances in MOS Devices. String DAC Parasitic Capacitances EE 435 Lecture 37 Parasitic Capacitances in MOS Devices String DAC Parasitic Capacitances Parasitic Capacitors in MOSFET (will initially consider two) Parasitic Capacitors in MOSFET C GCH Parasitic Capacitors

More information

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

ENGR890 Digital VLSI Design Fall Lecture 4: CMOS Inverter (static view) ENGR89 Digital VLSI Design Fall 5 Lecture 4: CMOS Inverter (static view) [Adapted from Chapter 5 of Digital Integrated Circuits, 3, J. Rabaey et al.] [Also borrowed from Vijay Narayanan and Mary Jane Irwin]

More information

ESE 570: Digital Integrated Circuits and VLSI Fundamentals

ESE 570: Digital Integrated Circuits and VLSI Fundamentals ESE 570: Digital Integrated Circuits and VLSI Fundamentals Lec 4: January 23, 2018 MOS Transistor Theory, MOS Model Penn ESE 570 Spring 2018 Khanna Lecture Outline! CMOS Process Enhancements! Semiconductor

More information

EE382M-14 CMOS Analog Integrated Circuit Design

EE382M-14 CMOS Analog Integrated Circuit Design EE382M-14 CMOS Analog Integrated Circuit Design Lecture 3, MOS Capacitances, Passive Components, and Layout of Analog Integrated Circuits MOS Capacitances Type of MOS transistor capacitors Depletion capacitance

More information

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

ECE 438: Digital Integrated Circuits Assignment #4 Solution The Inverter ECE 438: Digital Integrated Circuits Assignment #4 The Inverter Text: Chapter 5, Digital Integrated Circuits 2 nd Ed, Rabaey 1) Consider the CMOS inverter circuit in Figure P1 with the following parameters.

More information

Lecture 10 MOSFET (III) MOSFET Equivalent Circuit Models

Lecture 10 MOSFET (III) MOSFET Equivalent Circuit Models Lecture 10 MOSFET (III) MOSFET Equivalent Circuit Models Outline Lowfrequency smallsignal equivalent circuit model Highfrequency smallsignal equivalent circuit model Reading Assignment: Howe and Sodini;

More information

MOSFET Capacitance Model

MOSFET Capacitance Model MOSFET Capacitance Model So far we discussed the MOSFET DC models. In real circuit operation, the device operates under time varying terminal voltages and the device operation can be described by: 1 small

More information

Announcements. EE141- Fall 2002 Lecture 7. MOS Capacitances Inverter Delay Power

Announcements. EE141- Fall 2002 Lecture 7. MOS Capacitances Inverter Delay Power - Fall 2002 Lecture 7 MOS Capacitances Inverter Delay Power Announcements Wednesday 12-3pm lab cancelled Lab 4 this week Homework 2 due today at 5pm Homework 3 posted tonight Today s lecture MOS capacitances

More information

Lecture 150 Basic IC Processes (10/10/01) Page ECE Analog Integrated Circuits and Systems P.E. Allen

Lecture 150 Basic IC Processes (10/10/01) Page ECE Analog Integrated Circuits and Systems P.E. Allen Lecture 150 Basic IC Processes (10/10/01) Page 1501 LECTURE 150 BASIC IC PROCESSES (READING: TextSec. 2.2) INTRODUCTION Objective The objective of this presentation is: 1.) Introduce the fabrication of

More information

EECS 141: FALL 05 MIDTERM 1

EECS 141: FALL 05 MIDTERM 1 University of California College of Engineering Department of Electrical Engineering and Computer Sciences D. Markovic TuTh 11-1:3 Thursday, October 6, 6:3-8:pm EECS 141: FALL 5 MIDTERM 1 NAME Last SOLUTION

More information

Lecture 210 Physical Aspects of ICs (12/15/01) Page 210-1

Lecture 210 Physical Aspects of ICs (12/15/01) Page 210-1 Lecture 210 Physical Aspects of ICs (12/15/01) Page 210-1 LECTURE 210 PHYSICAL ASPECTS OF ICs (READING: Text-Sec. 2.5, 2.6, 2.8) INTRODUCTION Objective Illustrate the physical aspects of integrated circuits

More information

The Physical Structure (NMOS)

The Physical Structure (NMOS) The Physical Structure (NMOS) Al SiO2 Field Oxide Gate oxide S n+ Polysilicon Gate Al SiO2 SiO2 D n+ L channel P Substrate Field Oxide contact Metal (S) n+ (G) L W n+ (D) Poly 1 Transistor Resistance Two

More information

The Inverter. Digital Integrated Circuits A Design Perspective. Jan M. Rabaey Anantha Chandrakasan Borivoje Nikolic

The Inverter. Digital Integrated Circuits A Design Perspective. Jan M. Rabaey Anantha Chandrakasan Borivoje Nikolic Digital Integrated Circuits A Design Perspective Jan M. Rabaey Anantha Chandrakasan Borivoje Nikolic The Inverter Revised from Digital Integrated Circuits, Jan M. Rabaey el, 2003 Propagation Delay CMOS

More information

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

and V DS V GS V T (the saturation region) I DS = k 2 (V GS V T )2 (1+ V DS ) ECE 4420 Spring 2005 Page 1 FINAL EXAMINATION NAME SCORE /100 Problem 1O 2 3 4 5 6 7 Sum Points INSTRUCTIONS: This exam is closed book. You are permitted four sheets of notes (three of which are your sheets

More information

EE 466/586 VLSI Design. Partha Pande School of EECS Washington State University

EE 466/586 VLSI Design. Partha Pande School of EECS Washington State University EE 466/586 VLSI Design Partha Pande School of EECS Washington State University pande@eecs.wsu.edu Lecture 9 Propagation delay Power and delay Tradeoffs Follow board notes Propagation Delay Switching Time

More information

II III IV V VI B C N. Al Si P S. Zn Ga Ge As Se Cd In Sn Sb Te. Silicon (Si) the dominating material in IC manufacturing

II III IV V VI B C N. Al Si P S. Zn Ga Ge As Se Cd In Sn Sb Te. Silicon (Si) the dominating material in IC manufacturing II III IV V VI B N Al Si P S Zn Ga Ge As Se d In Sn Sb Te Silicon (Si) the dominating material in I manufacturing ompound semiconductors III - V group: GaAs GaN GaSb GaP InAs InP InSb... The Energy Band

More information

Lecture 0: Introduction

Lecture 0: Introduction Lecture 0: Introduction Introduction q Integrated circuits: many transistors on one chip q Very Large Scale Integration (VLSI): bucketloads! q Complementary Metal Oxide Semiconductor Fast, cheap, low power

More information

MOS Transistor Theory MOSFET Symbols Current Characteristics of MOSFET. MOS Symbols and Characteristics. nmos Enhancement Transistor

MOS Transistor Theory MOSFET Symbols Current Characteristics of MOSFET. MOS Symbols and Characteristics. nmos Enhancement Transistor MOS Transistor Theory MOSFET Symbols Current Characteristics of MOSFET Calculation of t and Important 2 nd Order Effects SmallSignal Signal MOSFET Model Summary Material from: CMOS LSI Design By Weste

More information

EE105 - Fall 2006 Microelectronic Devices and Circuits

EE105 - Fall 2006 Microelectronic Devices and Circuits EE105 - Fall 2006 Microelectronic Devices and Circuits Prof. Jan M. Rabaey (jan@eecs) Lecture 7: MOS Transistor Some Administrative Issues Lab 2 this week Hw 2 due on We Hw 3 will be posted same day MIDTERM

More information

B.Supmonchai June 26, q Introduction of device basic equations. q Introduction of models for manual analysis.

B.Supmonchai June 26, q Introduction of device basic equations. q Introduction of models for manual analysis. June 26, 2004 oal of this chapter Chapter 2 MO Transistor Theory oonchuay upmonchai Integrated esign Application Research (IAR) Laboratory June 16th, 2004; Revised June 16th, 2005 q Present intuitive understanding

More information

ESE570 Spring University of Pennsylvania Department of Electrical and System Engineering Digital Integrated Cicruits AND VLSI Fundamentals

ESE570 Spring University of Pennsylvania Department of Electrical and System Engineering Digital Integrated Cicruits AND VLSI Fundamentals University of Pennsylvania Department of Electrical and System Engineering Digital Integrated Cicruits AND VLSI Fundamentals ESE570, Spring 2018 Final Monday, Apr 0 5 Problems with point weightings shown.

More information

Lecture 12: MOS Capacitors, transistors. Context

Lecture 12: MOS Capacitors, transistors. Context Lecture 12: MOS Capacitors, transistors Context In the last lecture, we discussed PN diodes, and the depletion layer into semiconductor surfaces. Small signal models In this lecture, we will apply those

More information

EE105 - Fall 2005 Microelectronic Devices and Circuits

EE105 - Fall 2005 Microelectronic Devices and Circuits EE105 - Fall 005 Microelectronic Devices and Circuits ecture 7 MOS Transistor Announcements Homework 3, due today Homework 4 due next week ab this week Reading: Chapter 4 1 ecture Material ast lecture

More information

Practice 7: CMOS Capacitance

Practice 7: CMOS Capacitance Practice 7: CMOS Capacitance Digital Electronic Circuits Semester A 2012 MOSFET Capacitances MOSFET Capacitance Components 3 Gate to Channel Capacitance In general, the gate capacitance is similar to a

More information

ECE 342 Electronic Circuits. 3. MOS Transistors

ECE 342 Electronic Circuits. 3. MOS Transistors 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

More information

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

Important! EE141- Fall 2002 Lecture 5. CMOS Inverter MOS Transistor Model - Fall 00 Lecture 5 CMO Inverter MO Transistor Model Important! Lab 3 this week You must show up in one of the lab sessions this week If you don t show up you will be dropped from the class» Unless you

More information

Introduction and Background

Introduction and Background Analog CMOS Integrated Circuit Design Introduction and Background Dr. Jawdat Abu-Taha Department of Electrical and Computer Engineering Islamic University of Gaza jtaha@iugaza.edu.ps 1 Marking Assignments

More information

ESE 570: Digital Integrated Circuits and VLSI Fundamentals

ESE 570: Digital Integrated Circuits and VLSI Fundamentals ESE 570: Digital Integrated Circuits and VLSI Fundamentals Lec 4: January 29, 2019 MOS Transistor Theory, MOS Model Penn ESE 570 Spring 2019 Khanna Lecture Outline! CMOS Process Enhancements! Semiconductor

More information

Integrated Circuits & Systems

Integrated Circuits & Systems Federal University of Santa Catarina Center for Technology Computer Science & Electronics Engineering Integrated Circuits & Systems INE 5442 Lecture 10 MOSFET part 1 guntzel@inf.ufsc.br ual-well Trench-Isolated

More information

ECE 546 Lecture 10 MOS Transistors

ECE 546 Lecture 10 MOS Transistors ECE 546 Lecture 10 MOS Transistors Spring 2018 Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois jesa@illinois.edu NMOS Transistor NMOS Transistor N-Channel MOSFET Built on p-type

More information

EE 330 Lecture 16. MOSFET Modeling CMOS Process Flow

EE 330 Lecture 16. MOSFET Modeling CMOS Process Flow EE 330 Lecture 16 MOSFET Modeling CMOS Process Flow Model Extensions 300 Id 250 200 150 100 50 300 0 0 1 2 3 4 5 Vds Existing Model 250 200 Id 150 100 50 Slope is not 0 0 0 1 2 3 4 Actual Device Vds Model

More information

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

MOS Transistors. Prof. Krishna Saraswat. Department of Electrical Engineering Stanford University Stanford, CA MOS Transistors Prof. Krishna Saraswat Department of Electrical Engineering S Stanford, CA 94305 saraswat@stanford.edu 1 1930: Patent on the Field-Effect Transistor! Julius Lilienfeld filed a patent describing

More information

ESE570 Spring University of Pennsylvania Department of Electrical and System Engineering Digital Integrated Cicruits AND VLSI Fundamentals

ESE570 Spring University of Pennsylvania Department of Electrical and System Engineering Digital Integrated Cicruits AND VLSI Fundamentals University of Pennsylvania Department of Electrical and System Engineering Digital Integrated Cicruits AND VLSI Fundamentals ESE570, Spring 2016 Final Friday, May 6 5 Problems with point weightings shown.

More information

Chapter 3 Basics Semiconductor Devices and Processing

Chapter 3 Basics Semiconductor Devices and Processing Chapter 3 Basics Semiconductor Devices and Processing Hong Xiao, Ph. D. www2.austin.cc.tx.us/hongxiao/book.htm Hong Xiao, Ph. D. www2.austin.cc.tx.us/hongxiao/book.htm 1 Objectives Identify at least two

More information

Section 12: Intro to Devices

Section 12: Intro to Devices Section 12: Intro to Devices Extensive reading materials on reserve, including Robert F. Pierret, Semiconductor Device Fundamentals EE143 Ali Javey Bond Model of Electrons and Holes Si Si Si Si Si Si Si

More information

Chapter 2. Design and Fabrication of VLSI Devices

Chapter 2. Design and Fabrication of VLSI Devices Chapter 2 Design and Fabrication of VLSI Devices Jason Cong 1 Design and Fabrication of VLSI Devices Objectives: To study the materials used in fabrication of VLSI devices. To study the structure of devices

More information

EEC 118 Lecture #5: CMOS Inverter AC Characteristics. Rajeevan Amirtharajah University of California, Davis Jeff Parkhurst Intel Corporation

EEC 118 Lecture #5: CMOS Inverter AC Characteristics. Rajeevan Amirtharajah University of California, Davis Jeff Parkhurst Intel Corporation EEC 8 Lecture #5: CMOS Inverter AC Characteristics Rajeevan Amirtharajah University of California, Davis Jeff Parkhurst Intel Corporation Acknowledgments Slides due to Rajit Manohar from ECE 547 Advanced

More information

Lecture 12 CMOS Delay & Transient Response

Lecture 12 CMOS Delay & Transient Response EE 471: Transport Phenomena in Solid State Devices Spring 2018 Lecture 12 CMOS Delay & Transient Response Bryan Ackland Department of Electrical and Computer Engineering Stevens Institute of Technology

More information

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

Lecture 15: MOS Transistor models: Body effects, SPICE models. Context. In the last lecture, we discussed the modes of operation of a MOS FET: Lecture 15: MOS Transistor models: Body effects, SPICE models Context In the last lecture, we discussed the modes of operation of a MOS FET: oltage controlled resistor model I- curve (Square-Law Model)

More information

ECEN474/704: (Analog) VLSI Circuit Design Spring 2018

ECEN474/704: (Analog) VLSI Circuit Design Spring 2018 ECEN474/704: (Analog) SI Circuit Design Spring 2018 ecture 2: MOS ransistor Modeling Sam Palermo Analog & Mixed-Signal Center exas A&M University Announcements If you haven t already, turn in your 0.18um

More information

nmos IC Design Report Module: EEE 112

nmos IC Design Report Module: EEE 112 nmos IC Design Report Author: 1302509 Zhao Ruimin Module: EEE 112 Lecturer: Date: Dr.Zhao Ce Zhou June/5/2015 Abstract This lab intended to train the experimental skills of the layout designing of the

More information

EE 330 Lecture 17. MOSFET Modeling CMOS Process Flow

EE 330 Lecture 17. MOSFET Modeling CMOS Process Flow EE 330 Lecture 17 MOSFET Modeling CMOS Process Flow Review from Last Lecture Limitations of Existing Models V DD V OUT V OUT V DD?? V IN V OUT V IN V IN V DD Switch-Level Models V DD Simple square-law

More information

LECTURE 3 MOSFETS II. MOS SCALING What is Scaling?

LECTURE 3 MOSFETS II. MOS SCALING What is Scaling? LECTURE 3 MOSFETS II Lecture 3 Goals* * Understand constant field and constant voltage scaling and their effects. Understand small geometry effects for MOS transistors and their implications modeling and

More information

ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems

ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems Lec 6: September 18, 2017 MOS Model You are Here: Transistor Edition! Previously: simple models (0 and 1 st order) " Comfortable

More information

EE 330 Lecture 18. Small-signal Model (very preliminary) Bulk CMOS Process Flow

EE 330 Lecture 18. Small-signal Model (very preliminary) Bulk CMOS Process Flow EE 330 Lecture 18 Small-signal Model (very preliminary) Bulk CMOS Process Flow Review from Last Lecture How many models of the MOSFET do we have? Switch-level model (2) Square-law model Square-law model

More information

ESE 570: Digital Integrated Circuits and VLSI Fundamentals

ESE 570: Digital Integrated Circuits and VLSI Fundamentals ESE 570: Digital Integrated Circuits and VLSI Fundamentals Lec 4: January 24, 2017 MOS Transistor Theory, MOS Model Penn ESE 570 Spring 2017 Khanna Lecture Outline! Semiconductor Physics " Band gaps "

More information

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

ELEC 3908, Physical Electronics, Lecture 26. MOSFET Small Signal Modelling ELEC 3908, Physical Electronics, Lecture 26 MOSFET Small Signal Modelling Lecture Outline MOSFET small signal behavior will be considered in the same way as for the diode and BJT Capacitances will be considered

More information

ELEN0037 Microelectronic IC Design. Prof. Dr. Michael Kraft

ELEN0037 Microelectronic IC Design. Prof. Dr. Michael Kraft ELEN0037 Microelectronic IC Design Prof. Dr. Michael Kraft Lecture 2: Technological Aspects Technology Passive components Active components CMOS Process Basic Layout Scaling CMOS Technology Integrated

More information

ESE 570: Digital Integrated Circuits and VLSI Fundamentals

ESE 570: Digital Integrated Circuits and VLSI Fundamentals ESE 570: Digital Integrated Circuits and VLSI Fundamentals Lec 5: January 25, 2018 MOS Operating Regions, pt. 1 Lecture Outline! 3 Regions of operation for MOSFET " Subthreshold " Linear " Saturation!

More information