Lecture 27 ANNOUNCEMENTS. Regular office hours will end on Monday 12/10 Special office hours will be posted on the EE105 website

Size: px
Start display at page:

Download "Lecture 27 ANNOUNCEMENTS. Regular office hours will end on Monday 12/10 Special office hours will be posted on the EE105 website"

Transcription

1 Lecture 27 ANNOUNCEMENTS Regular office hours will end on Monday 12/10 Special office hours will be posted on the EE105 website Final Exam Review Session: Friday 12/14, 3PM, HP Auditorium Video will be posted online by Monday 12/17 Final Exam: Thursday 12/20, 12:30PM 3:30PM, 277 Cory Closed book; 6 pages of notes only Comprehensive in coverage: Material of MT#1 and MT#2, plus MOSFET amplifiers, MOSFET current sources, BJT and MOSFET differential amplifiers, feedback. Qualitative questions on state of the art device technology EE105 Fall 2007 Lecture 27, Slide 1 Prof. Liu, UC Berkeley

2 Outline IC technology advancement Q: How did we get here? Modern BJT technology Q: What is an HBT? Modern MOSFET technology Q: What are the challenges (and potential solutions) for continued MOSFET scaling? EE105 Fall 2007 Lecture 27, Slide 2 Prof. Liu, UC Berkeley

3 The IC Market The semiconductor industry is approaching $300B/yr in sales Military 2% Communications 24% Computers 42% Industrial 8% Transportation 8% Consumer Electronics 16% EE105 Fall 2007 Lecture 27, Slide 3 Prof. Liu, UC Berkeley Courtesy of r. Bill Flounders, UC Berkeley Microlab

4 IC Technology Advancement Improvements in IC performance and cost have been enabled by the steady miniaturization of the transistor Investment Transistor Scaling SMIC s Fab 4 (Beijing, China) Photo by L.R. Huang, igitimes Better Performance/Cost m) LENGTH (n 100 Market Growth PITCH 10 International Technology Roadmap for Semiconductors YEAR: HALF-PITCH: 90nm 65nm 45nm 32nm 22nm GATE LOW POWER HIGH PERFORMANCE YEAR EE105 Fall 2007 Lecture 27, Slide 4 Prof. Liu, UC Berkeley

5 The Nanometer Size Scale MOSFET Carbon nanotube EE105 Fall 2007 Lecture 27, Slide 5 Prof. Liu, UC Berkeley

6 Nanogap NA etector Prof. Luke Lee, BioEngineering gept. Single-stranded NA ouble-stranded NA Polysilicon Poly-Si Poly-Si Poly-Si Poly-Si Insulator (Si 3 N 4 ) Insulator (Si 3 N 4 ) EE105 Fall 2007 Lecture 27, Slide 6 Prof. Liu, UC Berkeley

7 IC Fabrication Goal: Mass fabrication (i.e. simultaneous fabrication) of many IC chips on each wafer, each containing millions or billions of transistors Approach: Form thin films of semiconductors, metals, and insulators over an entire wafer, and pattern each layer with a process much like printing (lithography). Planar processing consists of a sequence of additive and subtractive steps with lateral patterning oxidation deposition ion implantation etching lithography EE105 Fall 2007 Lecture 27, Slide 7 Prof. Liu, UC Berkeley

8 Planar Processing (patented by Fairchild Semiconductor in 1959: J. A. Hoerni, US Patent 3,064,167) EPOSITION of a thin film LITHOGRAPHY Coat with a protective layer Selectively expose the protective layer evelop the protective layer ETCH to selectively remove the thin film Strip (etch) the protective layer EE105 Fall 2007 Lecture 27, Slide 8 Prof. Liu, UC Berkeley Courtesy of r. Bill Flounders, UC Berkeley Microlab

9 Overview of IC Process Steps Test Bare Silicon Wafer Epitaxy Processed Wafer Anneal eposition/growth Ion Implantation CMP Mask Pattern Generation C SEM Metrology efect etection Etch Lithography EE105 Fall 2007 Lecture 27, Slide 9 Prof. Liu, UC Berkeley Courtesy of r. Bill Flounders, UC Berkeley Microlab

10 Modern BJT Structure B E C P+polySi eep trench N+polySi p + p + P base N collector P+polySi N + subcollector Shallow trench N + eep trench Features: P substrate Narrow base n+ poly Si emitter Slf Self aligned li p+ poly Si base contacts t Lightly doped collector Heavily doped epitaxial subcollector Shallow trenches and deep trenches filled with SiO 2 for electrical isolation EE105 Fall 2007 Lecture 27, Slide 10 Prof. Liu, UC Berkeley

11 BJT Performance Parameters Common emitter current gain, β : A 2 B B ie E E E ib B ie E E B B ib B E B C W N n W N n n qa W N n qa I I = = β The cutoff frequency, f T, is the frequency at which β falls to 1. E E i W N It is correlated with the maximum frequency of oscillation, f max. Intrinsic gain T A C A T C o m V V I V V I r g = EE105 Fall 2007 Lecture 27, Slide 11 Prof. Liu, UC Berkeley

12 Heterojunction Bipolar Transistor (HBT) To improve β, we can increase n ib by using a base material (Si 1 x Ge x ) that has a smaller band gap energy for x = 0.2, E g of Si 1 x Ge x is 0.1eV smaller than for Si n 2 i β = E g exp kt B n 2 ib E n 2 ie N N E B W W E B Note that this allows a large β to be achieved with large N B (even >N E ), which is advantageous for increasing Early voltage (V A ) reducing base resistance EE105 Fall 2007 Lecture 27, Slide 12 Prof. Liu, UC Berkeley

13 Modern MOSFET Structures (Intel Penryn, from com) N-channel MOSFETs P-channel MOSFETs 45nm CMOS technology features: High permittivity gate dielectric and metal gate electrodes strained channel regions shallow trench isolation EE105 Fall 2007 Lecture 27, Slide 13 Prof. Liu, UC Berkeley

14 MOSFET Performance Parameters Transconductance (short channel MOSFET): I gm = vwcox = V V GS TH The average carrier velocity v isdependent on the velocity at which carriers are injected from the source into the channel, which is dependent on the carrier mobility The cutoff frequency of a MOSFET is given by 2πf = T g C m GS Intrinsic gain: I 1 1 g mro = = V V λ I λ ( V VTH ) GS TH GS EE105 Fall 2007 Lecture 27, Slide 14 Prof. Liu, UC Berkeley

15 MOSFET Scaling Challenges Suppression of short channel effects Gain in I ON is incommensurate withl L g scaling Variability in performance Sub wavelength lithography: (Costly resolution enhancement techniques are needed) Random variations: Photoresist line edge edge roughness photoresist esign Mask Wafer 250nm SiO 2 MOSFET: Source Substrate 180nm OPC Gate L g Gate L eff X j rain N sub 90nm and Below PSM OPC T ox Statistical dopant fluctuations A. Asenov, Source Symp. VLSI Tech. ig., pp. rain 86-87, A. Brown et al., IEEE Trans. Nanotechnology, p. 195, 2002 EE105 Fall 2007 Lecture 27, Slide 15 Prof. Liu, UC Berkeley

16 V TH Roll Off V TH decreases with L g Effect is exacerbated by high values of V S M. Okuno et al., 2005 IEM p. 52 Qualitative explanation: The source & drain p n junctions assist in depleting the Si underneath the gate. The smaller the L g, the greater the percentage of charge balanced by the S/ p n junctions: n+ V G p n+ x j depletion region Large L g : S Small L g : S EE105 Fall 2007 Lecture 27, Slide 16 Prof. Liu, UC Berkeley

17 Why New Transistor Structures? Leakage must be suppressed in order to reduce L g Note that V TH reduction due to IBL, the root cause for λ > 0, is also TH the cause for increased MOSFET leakage (I >0 for V GS = 0V) with MOSFET miniaturization Leakage occurs in region far from channel surface Let s get rid of it! L g Thin-Body MOSFET Gate Gate Source rain Silicon-on- Buried Oxide Insulator (SOI) Substrate Wafer EE105 Fall 2007 Lecture 27, Slide 17 Prof. Liu, UC Berkeley

18 Thin Body MOSFETs Leakage is suppressed by using a thin body (T Si < L g ) Channel doping is not needed dd higher h carrier mobility ouble gate structure is more scalable (to L g <10nm) Ultra-Thin Body (UTB) L L g ouble-gate (G) Gate Gate Source rain T Si Source rain T Si Gate Buried Oxide Substrate EE105 Fall 2007 Lecture 27, Slide 18 Prof. Liu, UC Berkeley

19 ouble Gate FinFET Planar G-FET FinFET L g L g Gate rain T Si Source Gate Gate rain Fin Height H FIN = W/2 Source. Hisamoto et al. (UC Berkeley), IEM Technical igest, pp , 1998 N. Lindert et al. (UC Berkeley), IEEE Electron evice Letters, pp , Fin Width = T Si 15nm L g FinFET: GATE 20 nm 10 nm RAIN Y.-K. Choi et al. (UC Berkeley), IEM Technical igest, pp , 2001 SOURCE EE105 Fall 2007 Lecture 27, Slide 19 Prof. Liu, UC Berkeley

20 15 nm L g FinFETs Y.-K. Choi et al. (UC Berkeley), IEM Technical igest, pp , T Si = 10 nm; T ox = 2.1 nm rain Curren nt, I d [A/u um] Transfer Characteristics V P+Si 0.4 Ge =-1.0 V 0.6 V d =1.0 V d Gate V d =-0.05 V N-body= 2x10 18 cm -3 PMOS V d =0.05 V NMOS Gate Voltage, V g [V] t, I d [ua/ /um] Curren rain Output Characteristics V =1 NMOS 500 PMOS V g -V t =1.2V Voltage step :0.2V rain Voltage, V d [V] EE105 Fall 2007 Lecture 27, Slide 20 Prof. Liu, UC Berkeley

21 10 nm L g FinFETs B. Yu et al. (AM & UC Berkeley), IEM Technical igest, pp , Gate rain Source Poly-Si NiSi 220Å SiO2 cap Si Fin BOX Lg=10nm EE105 Fall 2007 Lecture 27, Slide 21 Prof. Liu, UC Berkeley

22 MOSFET Scaling Scenario Advanced structures will enable Si MOSFET scaling to L g <10 nm metallic gate high-κ gate dielectric L g (nm): S G Si strained Si classic al forward body biasing multi-gate S G Si G EE105 Fall 2007 Lecture 27, Slide 22 Prof. Liu, UC Berkeley

23 The End is Not the Limit! Innovations in process technology, materials, and device design will sustain the Si revolution R SA ALES($)/Y Mainframes (>1 persons per computer) PCs (1 person/computer) UbiComp (>1 computers per person) Acknowledgement: Mark Weiser TIME Sensatex today Investment Technology, evice & Circuit Innovations, Heterogeneous Integration Market Growth Lower Power, Lower Cost Information technology will for better quality-of-life pervasive embedded human-centered solving societalscale problems Energy Health care Environment isaster response Philips Transportation EE105 Fall 2007 Lecture 27, Slide 23 Prof. Liu, UC Berkeley

24 EECS 105 in the Grand Scheme Example electronic system: cell phone EE105 Fall 2007 Lecture 27, Slide 24 Prof. Liu, UC Berkeley

EECS130 Integrated Circuit Devices

EECS130 Integrated Circuit Devices EECS130 Integrated Circuit Devices Professor Ali Javey 11/6/2007 MOSFETs Lecture 6 BJTs- Lecture 1 Reading Assignment: Chapter 10 More Scalable Device Structures Vertical Scaling is important. For example,

More information

FinFET-based Design for Robust Nanoscale SRAM

FinFET-based Design for Robust Nanoscale SRAM FinFET-based Design for Robust Nanoscale SRAM Prof. Tsu-Jae King Liu Dept. of Electrical Engineering and Computer Sciences University of California at Berkeley Acknowledgements Prof. Bora Nikoli Zheng

More information

Final Exam Topics. IC Technology Advancement. Microelectronics Technology in the 21 st Century. Intel s 90 nm CMOS Technology. 14 nm CMOS Transistors

Final Exam Topics. IC Technology Advancement. Microelectronics Technology in the 21 st Century. Intel s 90 nm CMOS Technology. 14 nm CMOS Transistors ANNOUNCEMENTS Final Exam: When: Wednesday 12/10 12:30-3:30PM Where: 10 Evans (last names beginning A-R) 60 Evans (last names beginning S-Z) Comprehensive coverage of course material Closed book; 3 sheets

More information

Fin-Shaped Field Effect Transistor (FinFET) Min Ku Kim 03/07/2018

Fin-Shaped Field Effect Transistor (FinFET) Min Ku Kim 03/07/2018 Fin-Shaped Field Effect Transistor (FinFET) Min Ku Kim 03/07/2018 ECE 658 Sp 2018 Semiconductor Materials and Device Characterizations OUTLINE Background FinFET Future Roadmap Keeping up w/ Moore s Law

More information

ECE 5745 Complex Digital ASIC Design Topic 2: CMOS Devices

ECE 5745 Complex Digital ASIC Design Topic 2: CMOS Devices ECE 5745 Complex Digital ASIC Design Topic 2: CMOS Devices Christopher Batten School of Electrical and Computer Engineering Cornell University http://www.csl.cornell.edu/courses/ece5950 Simple Transistor

More information

EECS130 Integrated Circuit Devices

EECS130 Integrated Circuit Devices EECS130 Integrated Circuit Devices Professor Ali Javey 11/01/2007 MOSFETs Lecture 5 Announcements HW7 set is due now HW8 is assigned, but will not be collected/graded. MOSFET Technology Scaling Technology

More information

EE 5611 Introduction to Microelectronic Technologies Fall Thursday, September 04, 2014 Lecture 02

EE 5611 Introduction to Microelectronic Technologies Fall Thursday, September 04, 2014 Lecture 02 EE 5611 Introduction to Microelectronic Technologies Fall 2014 Thursday, September 04, 2014 Lecture 02 1 Lecture Outline Review on semiconductor materials Review on microelectronic devices Example of microelectronic

More information

Advanced Digital Integrated Circuits. Lecture 2: Scaling Trends. Announcements. No office hour next Monday. Extra office hour Tuesday 2-3pm

Advanced Digital Integrated Circuits. Lecture 2: Scaling Trends. Announcements. No office hour next Monday. Extra office hour Tuesday 2-3pm EE241 - Spring 20 Advanced Digital Integrated Circuits Lecture 2: Scaling Trends and Features of Modern Technologies Announcements No office hour next Monday Extra office hour Tuesday 2-3pm 2 1 Outline

More information

Chapter 3: Basics Semiconductor Devices and Processing 2006/9/27 1. Topics

Chapter 3: Basics Semiconductor Devices and Processing 2006/9/27 1. Topics Chapter 3: Basics Semiconductor Devices and Processing 2006/9/27 1 Topics What is semiconductor Basic semiconductor devices Basics of IC processing CMOS technologies 2006/9/27 2 1 What is Semiconductor

More information

Chapter 3 Basics Semiconductor Devices and Processing

Chapter 3 Basics Semiconductor Devices and Processing Chapter 3 Basics Semiconductor Devices and Processing 1 Objectives Identify at least two semiconductor materials from the periodic table of elements List n-type and p-type dopants Describe a diode and

More information

FABRICATION OF CMOS INTEGRATED CIRCUITS. Dr. Mohammed M. Farag

FABRICATION OF CMOS INTEGRATED CIRCUITS. Dr. Mohammed M. Farag FABRICATION OF CMOS INTEGRATED CIRCUITS Dr. Mohammed M. Farag Outline Overview of CMOS Fabrication Processes The CMOS Fabrication Process Flow Design Rules Reference: Uyemura, John P. "Introduction to

More information

ADVANCED MATERIALS AND PROCESSES FOR NANOMETER-SCALE FINFETS

ADVANCED MATERIALS AND PROCESSES FOR NANOMETER-SCALE FINFETS ADVANCED MATERIALS AND PROCESSES FOR NANOMETER-SCALE FINFETS Tsu-Jae King, Yang-Kyu Choi, Pushkar Ranade^ and Leland Chang Electrical Engineering and Computer Sciences Dept., ^Materials Science and Engineering

More information

ITRS MOSFET Scaling Trends, Challenges, and Key Technology Innovations

ITRS MOSFET Scaling Trends, Challenges, and Key Technology Innovations Workshop on Frontiers of Extreme Computing Santa Cruz, CA October 24, 2005 ITRS MOSFET Scaling Trends, Challenges, and Key Technology Innovations Peter M. Zeitzoff Outline Introduction MOSFET scaling and

More information

EE4800 CMOS Digital IC Design & Analysis. Lecture 1 Introduction Zhuo Feng

EE4800 CMOS Digital IC Design & Analysis. Lecture 1 Introduction Zhuo Feng EE4800 CMOS Digital IC Design & Analysis Lecture 1 Introduction Zhuo Feng 1.1 Prof. Zhuo Feng Office: EERC 730 Phone: 487-3116 Email: zhuofeng@mtu.edu Class Website http://www.ece.mtu.edu/~zhuofeng/ee4800fall2010.html

More information

Lecture 0: Introduction

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

More information

CMOS Digital Integrated Circuits Lec 2 Fabrication of MOSFETs

CMOS Digital Integrated Circuits Lec 2 Fabrication of MOSFETs CMOS Digital Integrated Circuits Lec 2 Fabrication of MOSFETs 1 CMOS Digital Integrated Circuits 3 rd Edition Categories of Materials Materials can be categorized into three main groups regarding their

More information

The 3 D Tri Gate transistor is a variant of the FinFET developed at UC Berkeley, and is being used in Intel s 22nmgeneration. microprocessors.

The 3 D Tri Gate transistor is a variant of the FinFET developed at UC Berkeley, and is being used in Intel s 22nmgeneration. microprocessors. On May 4, 2011, Intel Corporation announced what it called the most radical shift in semiconductor technology in 50 years. A new 3 dimensional transistor design will enable the production of integrated

More information

45nm Bulk CMOS Within-Die Variations. Courtesy of C. Spanos (UC Berkeley) Lecture 11. Process-induced Variability I: Random

45nm Bulk CMOS Within-Die Variations. Courtesy of C. Spanos (UC Berkeley) Lecture 11. Process-induced Variability I: Random 45nm Bulk CMOS Within-Die Variations. Courtesy of C. Spanos (UC Berkeley) Lecture 11 Process-induced Variability I: Random Random Variability Sources and Characterization Comparisons of Different MOSFET

More information

420 Intro to VLSI Design

420 Intro to VLSI Design Dept of Electrical and Computer Engineering 420 Intro to VLSI Design Lecture 0: Course Introduction and Overview Valencia M. Joyner Spring 2005 Getting Started Syllabus About the Instructor Labs, Problem

More information

EECS 151/251A Spring 2019 Digital Design and Integrated Circuits. Instructors: Wawrzynek. Lecture 8 EE141

EECS 151/251A Spring 2019 Digital Design and Integrated Circuits. Instructors: Wawrzynek. Lecture 8 EE141 EECS 151/251A Spring 2019 Digital Design and Integrated Circuits Instructors: Wawrzynek Lecture 8 EE141 From the Bottom Up IC processing CMOS Circuits (next lecture) EE141 2 Overview of Physical Implementations

More information

Lecture 020 ECE4430 Review II (1/5/04) Page 020-1

Lecture 020 ECE4430 Review II (1/5/04) Page 020-1 Lecture 020 ECE4430 Review II (1/5/04) Page 020-1 LECTURE 020 ECE 4430 REVIEW II (READING: GHLM - Chap. 2) Objective The objective of this presentation is: 1.) Identify the prerequisite material as taught

More information

Alternatives to standard MOSFETs. What problems are we really trying to solve?

Alternatives to standard MOSFETs. What problems are we really trying to solve? Alternatives to standard MOSFETs A number of alternative FET schemes have been proposed, with an eye toward scaling up to the 10 nm node. Modifications to the standard MOSFET include: Silicon-in-insulator

More information

Lecture 020 ECE4430 Review II (1/5/04) Page 020-1

Lecture 020 ECE4430 Review II (1/5/04) Page 020-1 Lecture 020 ECE4430 Review II (1/5/04) Page 020-1 LECTURE 020 ECE 4430 REVIEW II (READING: GHLM - Chap. 2) Objective The objective of this presentation is: 1.) Identify the prerequisite material as taught

More information

VLSI Design. Introduction

VLSI Design. Introduction VLSI Design Introduction Outline Introduction Silicon, pn-junctions and transistors A Brief History Operation of MOS Transistors CMOS circuits Fabrication steps for CMOS circuits Introduction Integrated

More information

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

Integrated diodes. The forward voltage drop only slightly depends on the forward current. ELEKTRONIKOS ĮTAISAI 1 Integrated diodes pn junctions of transistor structures can be used as integrated diodes. The choice of the junction is limited by the considerations of switching speed and breakdown voltage. The forward

More information

Parameter Optimization Of GAA Nano Wire FET Using Taguchi Method

Parameter Optimization Of GAA Nano Wire FET Using Taguchi Method Parameter Optimization Of GAA Nano Wire FET Using Taguchi Method S.P. Venu Madhava Rao E.V.L.N Rangacharyulu K.Lal Kishore Professor, SNIST Professor, PSMCET Registrar, JNTUH Abstract As the process technology

More information

Lecture 33 - The Short Metal-Oxide-Semiconductor Field-Effect Transistor (cont.) April 30, 2007

Lecture 33 - The Short Metal-Oxide-Semiconductor Field-Effect Transistor (cont.) April 30, 2007 6.720J/3.43J - Integrated Microelectronic Devices - Spring 2007 Lecture 33-1 Lecture 33 - The Short Metal-Oxide-Semiconductor Field-Effect Transistor (cont.) April 30, 2007 Contents: 1. MOSFET scaling

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

Session 3: Solid State Devices. Silicon on Insulator

Session 3: Solid State Devices. Silicon on Insulator Session 3: Solid State Devices Silicon on Insulator 1 Outline A B C D E F G H I J 2 Outline Ref: Taurand Ning 3 SOI Technology SOl materials: SIMOX, BESOl, and Smart Cut SIMOX : Synthesis by IMplanted

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

Chapter 2 : Semiconductor Materials & Devices (II) Feb

Chapter 2 : Semiconductor Materials & Devices (II) Feb Chapter 2 : Semiconductor Materials & Devices (II) 1 Reference 1. SemiconductorManufacturing Technology: Michael Quirk and Julian Serda (2001) 3. Microelectronic Circuits (5/e): Sedra & Smith (2004) 4.

More information

VLSI Design. Introduction

VLSI Design. Introduction Tassadaq Hussain VLSI Design Introduction Outcome of this course Problem Aims Objectives Outcomes Data Collection Theoretical Model Mathematical Model Validate Development Analysis and Observation Pseudo

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

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

Transistor was first invented by William.B.Shockley, Walter Brattain and John Bardeen of Bell Labratories. In 1961, first IC was introduced. Unit 1 Basic MOS Technology Transistor was first invented by William.B.Shockley, Walter Brattain and John Bardeen of Bell Labratories. In 1961, first IC was introduced. Levels of Integration:- i) SSI:-

More information

Lecture #29. Moore s Law

Lecture #29. Moore s Law Lecture #29 ANNOUNCEMENTS HW#15 will be for extra credit Quiz #6 (Thursday 5/8) will include MOSFET C-V No late Projects will be accepted after Thursday 5/8 The last Coffee Hour will be held this Thursday

More information

Sustaining the Si Revolution: From 3D Transistors to 3D Integration

Sustaining the Si Revolution: From 3D Transistors to 3D Integration Sustaining the Si Revolution: From 3D Transistors to 3D Integration Tsu Jae King Liu Department of Electrical Engineering and Computer Sciences University of California, Berkeley, CA USA February 23, 2015

More information

Topic 3. CMOS Fabrication Process

Topic 3. CMOS Fabrication Process Topic 3 CMOS Fabrication Process Peter Cheung Department of Electrical & Electronic Engineering Imperial College London URL: www.ee.ic.ac.uk/pcheung/ E-mail: p.cheung@ic.ac.uk Lecture 3-1 Layout of a Inverter

More information

Key Questions. ECE 340 Lecture 39 : Introduction to the BJT-II 4/28/14. Class Outline: Fabrication of BJTs BJT Operation

Key Questions. ECE 340 Lecture 39 : Introduction to the BJT-II 4/28/14. Class Outline: Fabrication of BJTs BJT Operation Things you should know when you leave ECE 340 Lecture 39 : Introduction to the BJT-II Fabrication of BJTs Class Outline: Key Questions What elements make up the base current? What do the carrier distributions

More information

Record I on (0.50 ma/μm at V DD = 0.5 V and I off = 100 na/μm) 25 nm-gate-length ZrO 2 /InAs/InAlAs MOSFETs

Record I on (0.50 ma/μm at V DD = 0.5 V and I off = 100 na/μm) 25 nm-gate-length ZrO 2 /InAs/InAlAs MOSFETs Record I on (0.50 ma/μm at V DD = 0.5 V and I off = 100 na/μm) 25 nm-gate-length ZrO 2 /InAs/InAlAs MOSFETs Sanghoon Lee 1*, V. Chobpattana 2,C.-Y. Huang 1, B. J. Thibeault 1, W. Mitchell 1, S. Stemmer

More information

VLSI Technology Dr. Nandita Dasgupta Department of Electrical Engineering Indian Institute of Technology, Madras

VLSI Technology Dr. Nandita Dasgupta Department of Electrical Engineering Indian Institute of Technology, Madras VLSI Technology Dr. Nandita Dasgupta Department of Electrical Engineering Indian Institute of Technology, Madras Lecture - 40 BICMOS technology So, today we are going to have the last class on this VLSI

More information

Enabling Breakthroughs In Technology

Enabling Breakthroughs In Technology Enabling Breakthroughs In Technology Mike Mayberry Director of Components Research VP, Technology and Manufacturing Group Intel Corporation June 2011 Defined To be defined Enabling a Steady Technology

More information

In this lecture we will begin a new topic namely the Metal-Oxide-Semiconductor Field Effect Transistor.

In this lecture we will begin a new topic namely the Metal-Oxide-Semiconductor Field Effect Transistor. Solid State Devices Dr. S. Karmalkar Department of Electronics and Communication Engineering Indian Institute of Technology, Madras Lecture - 38 MOS Field Effect Transistor In this lecture we will begin

More information

FinFET Devices and Technologies

FinFET Devices and Technologies FinFET Devices and Technologies Jack C. Lee The University of Texas at Austin NCCAVS PAG Seminar 9/25/14 Material Opportunities for Semiconductors 1 Why FinFETs? Planar MOSFETs cannot scale beyond 22nm

More information

Record Extrinsic Transconductance (2.45 ms/μm at V DS = 0.5 V) InAs/In 0.53 Ga 0.47 As Channel MOSFETs Using MOCVD Source-Drain Regrowth

Record Extrinsic Transconductance (2.45 ms/μm at V DS = 0.5 V) InAs/In 0.53 Ga 0.47 As Channel MOSFETs Using MOCVD Source-Drain Regrowth Record Extrinsic Transconductance (2.45 ms/μm at = 0.5 V) InAs/In 0.53 Ga 7 As Channel MOSFETs Using MOCVD Source-Drain Regrowth Sanghoon Lee 1*, C.-Y. Huang 1, A. D. Carter 1, D. C. Elias 1, J. J. M.

More information

Performance investigations of novel dual-material gate (DMG) MOSFET with dielectric pockets (DP)

Performance investigations of novel dual-material gate (DMG) MOSFET with dielectric pockets (DP) Science in China Series E: Technological Sciences 2009 SCIENCE IN CHINA PRESS www.scichina.com tech.scichina.com Performance investigations of novel dual-material gate (DMG) MOSFET with dielectric pockets

More information

Newer process technology (since 1999) includes :

Newer process technology (since 1999) includes : Newer process technology (since 1999) includes : copper metalization hi-k dielectrics for gate insulators si on insulator strained silicon lo-k dielectrics for interconnects Immersion lithography for masks

More information

Bridging the Gap between Dreams and Nano-Scale Reality

Bridging the Gap between Dreams and Nano-Scale Reality Bridging the Gap between Dreams and Nano-Scale Reality Ban P. Wong Design Methodology, Chartered Semiconductor wongb@charteredsemi.com 28 July 2006 Outline Deficiencies in Boolean-based Design Rules in

More information

SRM INSTITUTE OF SCIENCE AND TECHNOLOGY (DEEMED UNIVERSITY)

SRM INSTITUTE OF SCIENCE AND TECHNOLOGY (DEEMED UNIVERSITY) SRM INSTITUTE OF SCIENCE AND TECHNOLOGY (DEEMED UNIVERSITY) QUESTION BANK I YEAR B.Tech (II Semester) ELECTRONIC DEVICES (COMMON FOR EC102, EE104, IC108, BM106) UNIT-I PART-A 1. What are intrinsic and

More information

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

Semiconductor Memory: DRAM and SRAM. Department of Electrical and Computer Engineering, National University of Singapore Semiconductor Memory: DRAM and SRAM Outline Introduction Random Access Memory (RAM) DRAM SRAM Non-volatile memory UV EPROM EEPROM Flash memory SONOS memory QD memory Introduction Slow memories Magnetic

More information

Transistor Scaling in the Innovation Era. Mark Bohr Intel Senior Fellow Logic Technology Development August 15, 2011

Transistor Scaling in the Innovation Era. Mark Bohr Intel Senior Fellow Logic Technology Development August 15, 2011 Transistor Scaling in the Innovation Era Mark Bohr Intel Senior Fellow Logic Technology Development August 15, 2011 MOSFET Scaling Device or Circuit Parameter Scaling Factor Device dimension tox, L, W

More information

EE301 Electronics I , Fall

EE301 Electronics I , Fall EE301 Electronics I 2018-2019, Fall 1. Introduction to Microelectronics (1 Week/3 Hrs.) Introduction, Historical Background, Basic Consepts 2. Rewiev of Semiconductors (1 Week/3 Hrs.) Semiconductor materials

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

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

+1 (479)

+1 (479) Introduction to VLSI Design http://csce.uark.edu +1 (479) 575-6043 yrpeng@uark.edu Invention of the Transistor Vacuum tubes ruled in first half of 20th century Large, expensive, power-hungry, unreliable

More information

IH2655 Design and Characterisation of Nano- and Microdevices. Lecture 1 Introduction and technology roadmap

IH2655 Design and Characterisation of Nano- and Microdevices. Lecture 1 Introduction and technology roadmap IH2655 Design and Characterisation of Nano- and Microdevices Lecture 1 Introduction and technology roadmap IH2655 Design and Characterisation of Nano- and Microdevices Introduction to IH2655 Brief historic

More information

EE241 - Spring 2013 Advanced Digital Integrated Circuits. Announcements. Sign up for Piazza if you haven t already

EE241 - Spring 2013 Advanced Digital Integrated Circuits. Announcements. Sign up for Piazza if you haven t already EE241 - Spring 2013 Advanced Digital Integrated Circuits Lecture 2: Scaling Trends and Features of Modern Technologies Announcements Sign up for Piazza if you haven t already 2 1 Assigned Reading R.H.

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

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

UNIT-VI FIELD EFFECT TRANSISTOR. 1. Explain about the Field Effect Transistor and also mention types of FET s. UNIT-I FIELD EFFECT TRANSISTOR 1. Explain about the Field Effect Transistor and also mention types of FET s. The Field Effect Transistor, or simply FET however, uses the voltage that is applied to their

More information

AE53/AC53/AT53/AE103 ELECT. DEVICES & CIRCUITS DEC 2015

AE53/AC53/AT53/AE103 ELECT. DEVICES & CIRCUITS DEC 2015 Q.2 a. By using Norton s theorem, find the current in the load resistor R L for the circuit shown in Fig.1. (8) Fig.1 IETE 1 b. Explain Z parameters and also draw an equivalent circuit of the Z parameter

More information

A New SiGe Base Lateral PNM Schottky Collector. Bipolar Transistor on SOI for Non Saturating. VLSI Logic Design

A New SiGe Base Lateral PNM Schottky Collector. Bipolar Transistor on SOI for Non Saturating. VLSI Logic Design A ew SiGe Base Lateral PM Schottky Collector Bipolar Transistor on SOI for on Saturating VLSI Logic Design Abstract A novel bipolar transistor structure, namely, SiGe base lateral PM Schottky collector

More information

Notes. (Subject Code: 7EC5)

Notes. (Subject Code: 7EC5) COMPUCOM INSTITUTE OF TECHNOLOGY & MANAGEMENT, JAIPUR (DEPARTMENT OF ELECTRONICS & COMMUNICATION) Notes VLSI DESIGN NOTES (Subject Code: 7EC5) Prepared By: MANVENDRA SINGH Class: B. Tech. IV Year, VII

More information

Active Technology for Communication Circuits

Active Technology for Communication Circuits EECS 242: Active Technology for Communication Circuits UC Berkeley EECS 242 Copyright Prof. Ali M Niknejad Outline Comparison of technology choices for communication circuits Si npn, Si NMOS, SiGe HBT,

More information

Solid State Devices- Part- II. Module- IV

Solid State Devices- Part- II. Module- IV Solid State Devices- Part- II Module- IV MOS Capacitor Two terminal MOS device MOS = Metal- Oxide- Semiconductor MOS capacitor - the heart of the MOSFET The MOS capacitor is used to induce charge at the

More information

Semiconductor Devices

Semiconductor Devices Semiconductor Devices - 2014 Lecture Course Part of SS Module PY4P03 Dr. P. Stamenov School of Physics and CRANN, Trinity College, Dublin 2, Ireland Hilary Term, TCD 3 th of Feb 14 MOSFET Unmodified Channel

More information

EE 410: Integrated Circuit Fabrication Laboratory

EE 410: Integrated Circuit Fabrication Laboratory EE 410: Integrated Circuit Fabrication Laboratory 1 EE 410: Integrated Circuit Fabrication Laboratory Web Site: Instructor: http://www.stanford.edu/class/ee410 https://ccnet.stanford.edu/ee410/ (on CCNET)

More information

VLSI Technology Dr. Nandita Dasgupta Department of Electrical Engineering Indian Institute of Technology, Madras

VLSI Technology Dr. Nandita Dasgupta Department of Electrical Engineering Indian Institute of Technology, Madras VLSI Technology Dr. Nandita Dasgupta Department of Electrical Engineering Indian Institute of Technology, Madras Lecture - 39 Latch up in CMOS We have been discussing about the problems in CMOS, basic

More information

ECSE-6300 IC Fabrication Laboratory Lecture 9 MOSFETs. Lecture Outline

ECSE-6300 IC Fabrication Laboratory Lecture 9 MOSFETs. Lecture Outline ECSE-6300 IC Fabrication Laboratory Lecture 9 MOSFETs Prof. Rensselaer Polytechnic Institute Troy, NY 12180 Office: CII-6229 Tel.: (518) 276-2909 e-mails: luj@rpi.edu http://www.ecse.rpi.edu/courses/s18/ecse

More information

Layout of a Inverter. Topic 3. CMOS Fabrication Process. The CMOS Process - photolithography (2) The CMOS Process - photolithography (1) v o.

Layout of a Inverter. Topic 3. CMOS Fabrication Process. The CMOS Process - photolithography (2) The CMOS Process - photolithography (1) v o. Layout of a Inverter Topic 3 CMOS Fabrication Process V DD Q p Peter Cheung Department of Electrical & Electronic Engineering Imperial College London v i v o Q n URL: www.ee.ic.ac.uk/pcheung/ E-mail: p.cheung@ic.ac.uk

More information

Basic Fabrication Steps

Basic Fabrication Steps Basic Fabrication Steps and Layout Somayyeh Koohi Department of Computer Engineering Adapted with modifications from lecture notes prepared by author Outline Fabrication steps Transistor structures Transistor

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 3: January 24, 2019 MOS Fabrication pt. 2: Design Rules and Layout Penn ESE 570 Spring 2019 Khanna Jack Keil Wolf Lecture http://www.ese.upenn.edu/about-ese/events/wolf.php

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

EE 330 Lecture 21. Bipolar Process Flow

EE 330 Lecture 21. Bipolar Process Flow EE 330 Lecture 21 Bipolar Process Flow Exam 2 Friday March 9 Exam 3 Friday April 13 Review from Last Lecture Simplified Multi-Region Model I C βi B JSA IB β V 1 V E e V CE BE V t AF V BE >0.4V V BC

More information

Sub-micron technology IC fabrication process trends SOI technology. Development of CMOS technology. Technology problems due to scaling

Sub-micron technology IC fabrication process trends SOI technology. Development of CMOS technology. Technology problems due to scaling Goodbye Microelectronics Welcome Nanoelectronics Sub-micron technology IC fabrication process trends SOI technology SiGe Tranzistor in 50nm process Virus The thickness of gate oxide= 1.2 nm!!! Today we

More information

EE 330 Lecture 7. Design Rules. IC Fabrication Technology Part 1

EE 330 Lecture 7. Design Rules. IC Fabrication Technology Part 1 EE 330 Lecture 7 Design Rules IC Fabrication Technology Part 1 Review from Last Time Technology Files Provide Information About Process Process Flow (Fabrication Technology) Model Parameters Design Rules

More information

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

Jack Keil Wolf Lecture. ESE 570: Digital Integrated Circuits and VLSI Fundamentals. Lecture Outline. MOSFET N-Type, P-Type. ESE 570: Digital Integrated Circuits and VLSI Fundamentals Jack Keil Wolf Lecture Lec 3: January 24, 2019 MOS Fabrication pt. 2: Design Rules and Layout http://www.ese.upenn.edu/about-ese/events/wolf.php

More information

A Review of Low-Power VLSI Technology Developments

A Review of Low-Power VLSI Technology Developments A Review of Low-Power VLSI Technology Developments Nakka Ravi Kumar Abstract Ever since the invention of integrated circuits, there has been a continuous demand for high-performance, low-power, and low-area/low-cost

More information

Design Simulation and Analysis of NMOS Characteristics for Varying Oxide Thickness

Design Simulation and Analysis of NMOS Characteristics for Varying Oxide Thickness MIT International Journal of Electronics and Communication Engineering, Vol. 4, No. 2, August 2014, pp. 81 85 81 Design Simulation and Analysis of NMOS Characteristics for Varying Oxide Thickness Alpana

More information

Lecture Wrap up. December 13, 2005

Lecture Wrap up. December 13, 2005 6.012 Microelectronic Devices and Circuits Fall 2005 Lecture 26 1 Lecture 26 6.012 Wrap up December 13, 2005 Contents: 1. 6.012 wrap up Announcements: Final exam TA review session: December 16, 7:30 9:30

More information

State-of-the-art device fabrication techniques

State-of-the-art device fabrication techniques State-of-the-art device fabrication techniques! Standard Photo-lithography and e-beam lithography! Advanced lithography techniques used in semiconductor industry Deposition: Thermal evaporation, e-gun

More information

Chapter 15 Summary and Future Trends

Chapter 15 Summary and Future Trends Chapter 15 Summary and Future Trends Hong Xiao, Ph. D. hxiao89@hotmail.com www2.austin.cc.tx.us/hongxiao/book.htm Hong Xiao, Ph. D. www2.austin.cc.tx.us/hongxiao/book.htm 1 The 1960s First IC product Bipolar

More information

3-D Modelling of the Novel Nanoscale Screen-Grid Field Effect Transistor (SGFET)

3-D Modelling of the Novel Nanoscale Screen-Grid Field Effect Transistor (SGFET) 3-D Modelling of the Novel Nanoscale Screen-Grid Field Effect Transistor (SGFET) Pei W. Ding, Kristel Fobelets Department of Electrical Engineering, Imperial College London, U.K. J. E. Velazquez-Perez

More information

Photolithography I ( Part 1 )

Photolithography I ( Part 1 ) 1 Photolithography I ( Part 1 ) Chapter 13 : Semiconductor Manufacturing Technology by M. Quirk & J. Serda Bjørn-Ove Fimland, Department of Electronics and Telecommunication, Norwegian University of Science

More information

High-Performance Si Nanowire FET with a Semi Gate-Around Structure Suitable for Integration

High-Performance Si Nanowire FET with a Semi Gate-Around Structure Suitable for Integration High-Performance Si Nanowire FET with a Semi Gate-Around Structure Suitable for Integration Soshi Sato 1, Hideyuki Kamimura 1, Hideaki Arai 1, Kuniyuki Kakushima 2, Parhat Ahmet 1, Kenji Ohmori 3, Keisaku

More information

FinFET vs. FD-SOI Key Advantages & Disadvantages

FinFET vs. FD-SOI Key Advantages & Disadvantages FinFET vs. FD-SOI Key Advantages & Disadvantages Amiad Conley Technical Marketing Manager Process Diagnostics & Control, Applied Materials ChipEx-2014, Apr 2014 1 Moore s Law The number of transistors

More information

V A ( ) 2 = A. For Vbe = 0.4V: Ic = 7.34 * 10-8 A. For Vbe = 0.5V: Ic = 3.49 * 10-6 A. For Vbe = 0.6V: Ic = 1.

V A ( ) 2 = A. For Vbe = 0.4V: Ic = 7.34 * 10-8 A. For Vbe = 0.5V: Ic = 3.49 * 10-6 A. For Vbe = 0.6V: Ic = 1. 1. A BJT has the structure and parameters below. a. Base Width = 0.5mu b. Electron lifetime in base is 1x10-7 sec c. Base doping is NA=10 17 /cm 3 d. Emitter Doping is ND=2 x10 19 /cm 3. Collector Doping

More information

New Devices for Ultra Low Energy Information Processing

New Devices for Ultra Low Energy Information Processing Beyond Transistor Scaling: New Devices for Ultra Low Energy Information Processing Prof. Tsu Jae King Liu Department of Electrical Engineering and Computer Sciences University it of California, i Berkeley,

More information

PAPER SOLUTION_DECEMBER_2014_VLSI_DESIGN_ETRX_SEM_VII Prepared by Girish Gidaye

PAPER SOLUTION_DECEMBER_2014_VLSI_DESIGN_ETRX_SEM_VII Prepared by Girish Gidaye Q1a) The MOS System under External Bias Depending on the polarity and the magnitude of V G, three different operating regions can be observed for the MOS system: 1) Accumulation 2) Depletion 3) Inversion

More information

Semiconductor Devices

Semiconductor Devices Semiconductor Devices Modelling and Technology Source Electrons Gate Holes Drain Insulator Nandita DasGupta Amitava DasGupta SEMICONDUCTOR DEVICES Modelling and Technology NANDITA DASGUPTA Professor Department

More information

INTRODUCTION TO MOS TECHNOLOGY

INTRODUCTION TO MOS TECHNOLOGY INTRODUCTION TO MOS TECHNOLOGY 1. The MOS transistor The most basic element in the design of a large scale integrated circuit is the transistor. For the processes we will discuss, the type of transistor

More information

ECEN474/704: (Analog) VLSI Circuit Design Fall 2016

ECEN474/704: (Analog) VLSI Circuit Design Fall 2016 ECEN474/704: (Analog) VLSI Circuit Design Fall 2016 Lecture 1: Introduction Sam Palermo Analog & Mixed-Signal Center Texas A&M University Announcements Turn in your 0.18um NDA form by Thursday Sep 1 No

More information

Integrated Circuit Technology (Course Code: EE662) Lecture 1: Introduction

Integrated Circuit Technology (Course Code: EE662) Lecture 1: Introduction Indian Institute of Technology Jodhpur, Year 2015 2016 Integrated Circuit Technology (Course Code: EE662) Lecture 1: Introduction Course Instructor: Shree Prakash Tiwari, Ph.D. Email: sptiwari@iitj.ac.in

More information

LSI ON GLASS SUBSTRATES

LSI ON GLASS SUBSTRATES LSI ON GLASS SUBSTRATES OUTLINE Introduction: Why System on Glass? MOSFET Technology Low-Temperature Poly-Si TFT Technology System-on-Glass Technology Issues Conclusion System on Glass CPU SRAM DRAM EEPROM

More information

INTRODUCTION: Basic operating principle of a MOSFET:

INTRODUCTION: Basic operating principle of a MOSFET: INTRODUCTION: Along with the Junction Field Effect Transistor (JFET), there is another type of Field Effect Transistor available whose Gate input is electrically insulated from the main current carrying

More information

MSE 410/ECE 340: Electrical Properties of Materials Fall 2016 Micron School of Materials Science and Engineering Boise State University

MSE 410/ECE 340: Electrical Properties of Materials Fall 2016 Micron School of Materials Science and Engineering Boise State University MSE 410/ECE 340: Electrical Properties of Materials Fall 2016 Micron School of Materials Science and Engineering Boise State University Practice Final Exam 1 Read the questions carefully Label all figures

More information

2.8 - CMOS TECHNOLOGY

2.8 - CMOS TECHNOLOGY CMOS Technology (6/7/00) Page 1 2.8 - CMOS TECHNOLOGY INTRODUCTION Objective The objective of this presentation is: 1.) Illustrate the fabrication sequence for a typical MOS transistor 2.) Show the physical

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 1, Introduction

Chapter 1, Introduction Introduction to Semiconductor Manufacturing Technology Chapter 1, Introduction hxiao89@hotmail.com 1 Objective After taking this course, you will able to Use common semiconductor terminology Describe a

More information

Improving CMOS Speed and Switching Energy with Vacuum-Gap Structures

Improving CMOS Speed and Switching Energy with Vacuum-Gap Structures Improving CMOS Speed and Switching Energy with Vacuum-Gap Structures Chenming Hu and Je Min Park Univ. of California, Berkeley -1- Outline Introduction Background and Motivation MOSFETs with Vacuum-Spacer

More information

International Journal of Scientific & Engineering Research, Volume 6, Issue 2, February-2015 ISSN

International Journal of Scientific & Engineering Research, Volume 6, Issue 2, February-2015 ISSN Performance Evaluation and Comparison of Ultra-thin Bulk (UTB), Partially Depleted and Fully Depleted SOI MOSFET using Silvaco TCAD Tool Seema Verma1, Pooja Srivastava2, Juhi Dave3, Mukta Jain4, Priya

More information

Power MOSFET Zheng Yang (ERF 3017,

Power MOSFET Zheng Yang (ERF 3017, ECE442 Power Semiconductor Devices and Integrated Circuits Power MOSFET Zheng Yang (ERF 3017, email: yangzhen@uic.edu) Evolution of low-voltage (

More information