Modeling of High Voltage AlGaN/GaN HEMT. Copyright 2008 Crosslight Software Inc.

Size: px
Start display at page:

Download "Modeling of High Voltage AlGaN/GaN HEMT. Copyright 2008 Crosslight Software Inc."

Transcription

1 Modelin of Hih Voltae AlGaN/GaN HEMT Copyriht 2008 Crossliht Software Inc. 1

2 Introduction 2 AlGaN/GaN HEMTs - potential to be operated at hih power and hih breakdown voltae not possible for silicon or GaAs based technoloies. Numerous efforts explored to enhance the breakdown voltae of GaN based HEMT devices. The field plate (FP) structure effective for the hih breakdown voltae AlGaN/GaN HEMT desin but the field distribution in the drift reion needs optimization to minimize the specific on-resistance. In this work, modelin and optimization performed with the demonstration of remarkably hih breakdown voltae (900 V) for AlGaN/GaN HEMT with a manesium dopin layer under the 2-DEG channel by usin Crossliht APSYS.

3 Device structure Cross-section view of AlGaN/GaN HEMT structure with a M dopin layer. Chare density of cm -2 caused by the piezo-electric & polarization dipole modeled alon the upper side of the AlGaN/GaN interface to determine the 2DEG sheet carrier concentration. 3 Traps with its maximum concentration cm -3, relative enery level of 1.1eV also defined to ensure an semi-insulatin substrate. The substrate semi-insulatin traps effective in suppressin substrate parasitic conduction. Ref: G. Xie et al, in Proceedins of The 22nd International Symposium on Power Semiconductor Devices & ICs, Hiroshima, Japan, June 6-10, 2010

4 Material parameters used 4

5 Surface potential distribution 5 Reverse characteristics, alon the AlGaN/GaN interface (line B) for different M dopin layer lenth L, V GS =-5 V, drain voltae increased till breakdown; breakdown voltae as hih as 900V achieved with L=1.5 mm while only 560V for the conventional device without the manesium layer.

6 Impact ionization & breakdown I-V 6 Cutline alon y=7.0 mm; zero from x-axis left Cutline alon x=5.5 mm; zero from bottom I-V curve showin breakdown ~ 720 V; M dopin layer L~ 3.2 mm

7 Electric field distribution 7 Reverse characteristics, alon the AlGaN/GaN interface (line B) for different M dopin layer lenth L, V GS =-5 V. With a M layer, the electric field is spread between the drain and the ate. Without the M layer, the field peaks near the ede of the ate electrode.

8 Electric field 2D contours 8 The proposed AlGaN/GaN HEMT device with V GS = 5, V DS -breakdown= 900 V, L=1.5 mm Conventional HEMT structure of the same device dimension but without the M dopin layer showin breakdown only around 560 V

9 Breakdown vs M dopin layer 9 Breakdown voltaes as a function of the M layer s dopin concentration and width(lenth) at V GS = 5V. Breakdown voltae reaches its hihest value with a M dopin concentration of cm -3 for L=1.5, 2.5 and 3.5 mm.

10 2D current vectors reverse 10 Reverse characteristics, 2D current vectors the proposed HEMT after breakdown, showin majority of current flow throuh the substrate,v DS - breakdown= 900 V, V GS = 5 V

11 2D current vectors forward 11 Forward characteristics with applied V DS = 5 V, V GS = 0 V, the electron current flows throuh the quantum well.

12 Forward IV characteristics 12 The transistor exhibits ood pinch-off characteristics and a maximum drain current density of around 230A/m (per unit channel width) at a ate voltae of 0V.

13 Comparison of breakdown voltae versus specific on-resistance 13 Another important technique, device area manaement, can be used to improve the specific on-resistance and the breakdown voltae trade off. Ron-sp can be reduced by shrinkin excess areas such as contacts, ate-source offset and channel reions, dependin on the process.

14 Conslusion 14 Hih breakdown voltae AlGaN/GaN HEMT with the manesium layer structure simulated. Breakdown voltae of 900V is obtained by optimizin the manesium layer s lenth and its dopin concentration. The specific on resistance was 4 mw cm 2 with a breakdown voltae of 900 V usin a manesium layer lenth of 1.5 mm; its dopin concentration is cm -3 and the drift reion lenth is 10 μm. The manesium layer is deemed to be an effective mean to enhance the breakdown voltae of AlGaN/GaN devices.

CHARACTERIZATION, MODELING, AND SIMULATION OF In 0.12 Al 0.88 N/GaN HEMTs

CHARACTERIZATION, MODELING, AND SIMULATION OF In 0.12 Al 0.88 N/GaN HEMTs CHARACTERIZATION, MODELING, AND SIMULATION OF In 0.12 Al 0.88 N/GaN HEMTs Marián Molnár 1,2, Gesualdo Donnarumma 1,Vassil Palankovski 1, Ján Kuzmík 1,3, Daniel Donoval 2, Jaroslav Kováč 2, and Siefried

More information

Spring Semester 2012 Final Exam

Spring Semester 2012 Final Exam Spring Semester 2012 Final Exam Note: Show your work, underline results, and always show units. Official exam time: 2.0 hours; an extension of at least 1.0 hour will be granted to anyone. Materials parameters

More information

Mixed-Signal IC Design Notes set 1: Quick Summary of Device Models

Mixed-Signal IC Design Notes set 1: Quick Summary of Device Models ECE194J /594J notes, M. Rodwell, copyrihted 2011 Mixed-Sinal IC Desin Notes set 1: Quick Summary of Device Models Mark Rodwell University of California, Santa Barbara rodwell@ece.ucsb.edu 805-893-3244,

More information

Device and Monte Carlo Simulation of GaN material and devices. Presenter: Ziyang Xiao Advisor: Prof. Neil Goldsman University of Maryland

Device and Monte Carlo Simulation of GaN material and devices. Presenter: Ziyang Xiao Advisor: Prof. Neil Goldsman University of Maryland Device and Monte Carlo Simulation of GaN material and devices Presenter: Ziyang Xiao Advisor: Prof. Neil Goldsman University of Maryland 2/23 OUTLINE - GaN Introduction and Background Device Simulation

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION Hihly efficient ate-tunable photocurrent eneration in vertical heterostructures of layered materials Woo Jon Yu, Yuan Liu, Hailon Zhou, Anxian Yin, Zhen Li, Yu Huan, and Xianfen Duan. Schematic illustration

More information

Normally-Off GaN Field Effect Power Transistors: Device Design and Process Technology Development

Normally-Off GaN Field Effect Power Transistors: Device Design and Process Technology Development Center for High Performance Power Electronics Normally-Off GaN Field Effect Power Transistors: Device Design and Process Technology Development Dr. Wu Lu (614-292-3462, lu.173@osu.edu) Dr. Siddharth Rajan

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

R. Ludwig and G. Bogdanov RF Circuit Design: Theory and Applications 2 nd edition. Figures for Chapter 6

R. Ludwig and G. Bogdanov RF Circuit Design: Theory and Applications 2 nd edition. Figures for Chapter 6 R. Ludwig and G. Bogdanov RF Circuit Design: Theory and Applications 2 nd edition Figures for Chapter 6 Free electron Conduction band Hole W g W C Forbidden Band or Bandgap W V Electron energy Hole Valence

More information

Lecture #27. The Short Channel Effect (SCE)

Lecture #27. The Short Channel Effect (SCE) Lecture #27 ANNOUNCEMENTS Design Project: Your BJT design should meet the performance specifications to within 10% at both 300K and 360K. ( β dc > 45, f T > 18 GHz, V A > 9 V and V punchthrough > 9 V )

More information

Chapter 6: Field-Effect Transistors

Chapter 6: Field-Effect Transistors Chapter 6: Field-Effect Transistors slamic University of Gaza Dr. Talal Skaik FETs vs. BJTs Similarities: Amplifiers Switching devices mpedance matching circuits Differences: FETs are voltage controlled

More information

ASM-HEMT Model for GaN RF and Power Electronic Applications: Overview and Extraction

ASM-HEMT Model for GaN RF and Power Electronic Applications: Overview and Extraction ASM-HEMT Model for GaN RF and Power Electronic Applications: Overview and Extraction June 27, 2016 Sheikh Aamir Ahsan Sudip Ghosh Yogesh Singh Chauhan IIT Kanpur Sourabh Khandelwal UC Berkeley MA Long

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

Avalanche breakdown. Impact ionization causes an avalanche of current. Occurs at low doping

Avalanche breakdown. Impact ionization causes an avalanche of current. Occurs at low doping Avalanche breakdown Impact ionization causes an avalanche of current Occurs at low doping Zener tunneling Electrons tunnel from valence band to conduction band Occurs at high doping Tunneling wave decays

More information

Analytical Evaluation of Energy and Electron Concentrations in Quantum Wells of the High Electron Mobility Transistors.

Analytical Evaluation of Energy and Electron Concentrations in Quantum Wells of the High Electron Mobility Transistors. Analytical Evaluation of Energy Electron Concentrations in Quantum Wells of the High Electron Mobility Transistors Salih SAYGI Department of Physics, Faculty of Arts Sciences, Gaziosmanpasa University,

More information

AlGaN/GaN-based HEMT on SiC substrate for microwave characteristics using different passivation layers

AlGaN/GaN-based HEMT on SiC substrate for microwave characteristics using different passivation layers PRAMANA c Indian Academy of Sciences Vol. 79, No. 1 journal of July 2012 physics pp. 151 163 AlGaN/GaN-based HEMT on SiC substrate for microwave characteristics using different passivation layers T R LENKA

More information

Quantum Phenomena & Nanotechnology (4B5)

Quantum Phenomena & Nanotechnology (4B5) Quantum Phenomena & Nanotechnology (4B5) The 2-dimensional electron gas (2DEG), Resonant Tunneling diodes, Hot electron transistors Lecture 11 In this lecture, we are going to look at 2-dimensional electron

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

Classification of Solids

Classification of Solids Classification of Solids Classification by conductivity, which is related to the band structure: (Filled bands are shown dark; D(E) = Density of states) Class Electron Density Density of States D(E) Examples

More information

Impact of sidewall spacer on gate leakage behavior of nano-scale MOSFETs

Impact of sidewall spacer on gate leakage behavior of nano-scale MOSFETs PACS 85.0.Tv Impact of sidewall spacer on ate leakae behavior of nano-scale MOSFETs Ashwani K. Rana 1, Narottam Chand, Vinod Kapoor 1 1 Department of Electronics and Communication, National Institute of

More information

Lecture 11: J-FET and MOSFET

Lecture 11: J-FET and MOSFET ENE 311 Lecture 11: J-FET and MOSFET FETs vs. BJTs Similarities: Amplifiers Switching devices Impedance matching circuits Differences: FETs are voltage controlled devices. BJTs are current controlled devices.

More information

JFET Operating Characteristics: V GS = 0 V 14. JFET Operating Characteristics: V GS = 0 V 15

JFET Operating Characteristics: V GS = 0 V 14. JFET Operating Characteristics: V GS = 0 V 15 J Operating Characteristics: V GS = 0 V 14 V GS = 0 and V DS increases from 0 to a more positive voltage: Gate and Source terminals: at the same potential Drain: at positive potential => reverse biased

More information

1 Name: Student number: DEPARTMENT OF PHYSICS AND PHYSICAL OCEANOGRAPHY MEMORIAL UNIVERSITY OF NEWFOUNDLAND. Fall :00-11:00

1 Name: Student number: DEPARTMENT OF PHYSICS AND PHYSICAL OCEANOGRAPHY MEMORIAL UNIVERSITY OF NEWFOUNDLAND. Fall :00-11:00 1 Name: DEPARTMENT OF PHYSICS AND PHYSICAL OCEANOGRAPHY MEMORIAL UNIVERSITY OF NEWFOUNDLAND Final Exam Physics 3000 December 11, 2012 Fall 2012 9:00-11:00 INSTRUCTIONS: 1. Answer all seven (7) questions.

More information

Analysis and Design of Analog Integrated Circuits Lecture 7. Differential Amplifiers

Analysis and Design of Analog Integrated Circuits Lecture 7. Differential Amplifiers Analysis and Desin of Analo Interated Circuits ecture 7 Differential Amplifiers Michael H. Perrott February 1, 01 Copyriht 01 by Michael H. Perrott All rihts reserved. Review Proposed Thevenin CMOS Transistor

More information

Dynamic On-resistance and Tunneling Based De-trapping in GaN HEMT

Dynamic On-resistance and Tunneling Based De-trapping in GaN HEMT MITSUBISHI ELECTRIC RESEARCH LABORATORIES http://www.merl.com Dynamic On-resistance and Tunneling Based De-trapping in GaN HEMT Zhu, L.; Teo, K.H.; Gao, Q. TR2015-047 June 2015 Abstract GaN HEMT dynamic

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: ircuitlevel Modeling, Design, and Optimization for Digital Systems Lec 7: September 20, 2017 MOS Transistor Operating Regions Part 1 Today! PN Junction! MOS Transistor Topology! Threshold! Operating

More information

Impact of oxide thickness on gate capacitance Modelling and comparative analysis of GaN-based MOSHEMTs

Impact of oxide thickness on gate capacitance Modelling and comparative analysis of GaN-based MOSHEMTs PRAMANA c Indian Academy of Sciences Vol. 85, No. 6 journal of December 2015 physics pp. 1221 1232 Impact of oxide thickness on gate capacitance Modelling and comparative analysis of GaN-based MOSHEMTs

More information

Lecture 12: MOSFET Devices

Lecture 12: MOSFET Devices Lecture 12: MOSFET Devices Gu-Yeon Wei Division of Engineering and Applied Sciences Harvard University guyeon@eecs.harvard.edu Wei 1 Overview Reading S&S: Chapter 5.1~5.4 Supplemental Reading Background

More information

High Voltage GaN Devices for Photovoltaics and High Frequency Switched Power Supplies

High Voltage GaN Devices for Photovoltaics and High Frequency Switched Power Supplies HIPER Lab Harris Integrative Photonics and Electronics Research Laboratory High Voltage GaN Devices for Photovoltaics and High Frequency Switched Power Supplies H. Rusty Harris Texas A&M University Depts.

More information

Nanoelectronics. Topics

Nanoelectronics. Topics Nanoelectronics Topics Moore s Law Inorganic nanoelectronic devices Resonant tunneling Quantum dots Single electron transistors Motivation for molecular electronics The review article Overview of Nanoelectronic

More information

Lecture 04 Review of MOSFET

Lecture 04 Review of MOSFET ECE 541/ME 541 Microelectronic Fabrication Techniques Lecture 04 Review of MOSFET Zheng Yang (ERF 3017, email: yangzhen@uic.edu) What is a Transistor? A Switch! An MOS Transistor V GS V T V GS S Ron D

More information

A Compact Gate Tunnel Current Model for Nano Scale MOSFET with Sub 1nm Gate Oxide

A Compact Gate Tunnel Current Model for Nano Scale MOSFET with Sub 1nm Gate Oxide A Compact Gate Tunnel Current Model for Nano Scale MOSFT with Sub 1nm Gate Oxide Ashwani Kumar 1, Narottam Chand 2,Vinod Kapoor 1 Department of lectronics and Communication nineerin Department of Computer

More information

Electrical Degradation of InAlAs/InGaAs Metamorphic High-Electron Mobility Transistors

Electrical Degradation of InAlAs/InGaAs Metamorphic High-Electron Mobility Transistors Electrical Degradation of InAlAs/InGaAs Metamorphic High-Electron Mobility Transistors S. D. Mertens and J.A. del Alamo Massachusetts Institute of Technology Sponsor: Agilent Technologies Outline Introduction

More information

Performance Analysis of. doped and undoped AlGaN/GaN HEMTs

Performance Analysis of. doped and undoped AlGaN/GaN HEMTs Performance Analysis of doped and undoped AlGaN/GaN HEMTs Smitha G S 1, Meghana V 2, Narayan T. Deshpande 3 1 M. Tech Student, ECE, BMS College of Engineering, Bengaluru, Karnataka, India 2B.E. Student,

More information

Overview of Modeling and Simulation TCAD - FLOOPS / FLOODS

Overview of Modeling and Simulation TCAD - FLOOPS / FLOODS Overview of Modeling and Simulation TCAD - FLOOPS / FLOODS Modeling Overview Strain Effects Thermal Modeling TCAD Modeling Outline FLOOPS / FLOODS Introduction Progress on GaN Devices Prospects for Reliability

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

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

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

Anomalous Source-side Degradation of InAlN/GaN HEMTs under ON-state Stress

Anomalous Source-side Degradation of InAlN/GaN HEMTs under ON-state Stress Anomalous Source-side Degradation of InAlN/GaN HEMTs under ON-state Stress Yufei Wu, Jesús A. del Alamo Microsystems Technology Laboratories, Massachusetts Institute of Technology October 04, 2016 Sponsor:

More information

ECE 305 Exam 5 SOLUTIONS: Spring 2015 April 17, 2015 Mark Lundstrom Purdue University

ECE 305 Exam 5 SOLUTIONS: Spring 2015 April 17, 2015 Mark Lundstrom Purdue University NAME: PUID: : ECE 305 Exam 5 SOLUTIONS: April 17, 2015 Mark Lundstrom Purdue University This is a closed book exam. You may use a calculator and the formula sheet at the end of this exam. Following the

More information

8. Schottky contacts / JFETs

8. Schottky contacts / JFETs Technische Universität Graz Institute of Solid State Physics 8. Schottky contacts / JFETs Nov. 21, 2018 Technische Universität Graz Institute of Solid State Physics metal - semiconductor contacts Photoelectric

More information

OFF-state TDDB in High-Voltage GaN MIS-HEMTs

OFF-state TDDB in High-Voltage GaN MIS-HEMTs OFF-state TDDB in High-Voltage GaN MIS-HEMTs Shireen Warnock and Jesús A. del Alamo Microsystems Technology Laboratories (MTL) Massachusetts Institute of Technology (MIT) Purpose Further understanding

More information

Schottky diodes. JFETs - MESFETs - MODFETs

Schottky diodes. JFETs - MESFETs - MODFETs Technische Universität Graz Institute of Solid State Physics Schottky diodes JFETs - MESFETs - MODFETs Quasi Fermi level When the charge carriers are not in equilibrium the Fermi energy can be different

More information

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

Operation and Modeling of. The MOS Transistor. Second Edition. Yannis Tsividis Columbia University. New York Oxford OXFORD UNIVERSITY PRESS Operation and Modeling of The MOS Transistor Second Edition Yannis Tsividis Columbia University New York Oxford OXFORD UNIVERSITY PRESS CONTENTS Chapter 1 l.l 1.2 1.3 1.4 1.5 1.6 1.7 Chapter 2 2.1 2.2

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

Semi-insulating SiC substrates for high frequency devices

Semi-insulating SiC substrates for high frequency devices Klausurtagung Silberbach, 19. - 21. Feb. 2002 Institut für Werkstoffwissenschaften - WW 6 Semi-insulating SiC substrates for high frequency devices Vortrag von Matthias Bickermann Semi-insulating SiC substrates

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

Temperature accelerated Degradation of GaN HEMTs under High power Stress: Activation Energy of Drain Current Degradation

Temperature accelerated Degradation of GaN HEMTs under High power Stress: Activation Energy of Drain Current Degradation Temperature accelerated Degradation of GaN HEMTs under High power Stress: Activation Energy of Drain Current Degradation Yufei Wu, Chia Yu Chen and Jesús A. del Alamo Microsystems Technology Laboratory

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

Quantum and Non-local Transport Models in Crosslight Device Simulators. Copyright 2008 Crosslight Software Inc.

Quantum and Non-local Transport Models in Crosslight Device Simulators. Copyright 2008 Crosslight Software Inc. Quantum and Non-local Transport Models in Crosslight Device Simulators Copyright 2008 Crosslight Software Inc. 1 Introduction Quantization effects Content Self-consistent charge-potential profile. Space

More information

MSE 310/ECE 340: Electrical Properties of Materials Fall 2014 Department of Materials Science and Engineering Boise State University

MSE 310/ECE 340: Electrical Properties of Materials Fall 2014 Department of Materials Science and Engineering Boise State University MSE 310/ECE 340: Electrical Properties of Materials Fall 2014 Department of Materials Science and Engineering Boise State University Practice Final Exam 1 Read the questions carefully Label all figures

More information

Polytech Montpellier MEA4 M2 EEA Systèmes Microélectroniques. Analog IC Design

Polytech Montpellier MEA4 M2 EEA Systèmes Microélectroniques. Analog IC Design Analo C Desin - Academic year 05/06 - Session 3 04/0/5 Polytech Montellier MEA4 M EEA Systèmes Microélectroniques Analo C Desin From transistor in to current sources Pascal Nouet 05/06 - nouet@lirmm.fr

More information

Modelling of capacitance and threshold voltage for ultrathin normally-off AlGaN/GaN MOSHEMT

Modelling of capacitance and threshold voltage for ultrathin normally-off AlGaN/GaN MOSHEMT Pramana J. Phys. (07) 88: 3 DOI 0.007/s043-06-30-y c Indian Academy of Sciences Modelling of capacitance and threshold voltage for ultrathin normally-off AlGaN/GaN MOSHEMT R SWAIN, K JENA and T R LENKA

More information

Modeling of the Substrate Current and Characterization of Traps in MOSFETs under Sub-Bandgap Photonic Excitation

Modeling of the Substrate Current and Characterization of Traps in MOSFETs under Sub-Bandgap Photonic Excitation Journal of the Korean Physical Society, Vol. 45, No. 5, November 2004, pp. 1283 1287 Modeling of the Substrate Current and Characterization of Traps in MOSFETs under Sub-Bandgap Photonic Excitation I.

More information

Is quantum capacitance in graphene a potential hurdle for device scaling?

Is quantum capacitance in graphene a potential hurdle for device scaling? Electronic Supplementary Material Is quantum capacitance in raphene a potential hurdle for device scalin? Jaeho Lee 1,,, Hyun-Jon hun 1,3, (), David H. Seo 1, Jaehon Lee,4, Hyuncheol Shin, Sunae Seo 1,5,

More information

Computer Aided Design of GaN Light-Emitting Diodes. Copyright 2006 Crosslight Software Inc.

Computer Aided Design of GaN Light-Emitting Diodes. Copyright 2006 Crosslight Software Inc. Computer Aided Design of GaN Light-Emitting Diodes Copyright 2006 Crosslight Software Inc. www.crosslight.com 1 2 Contents Available tools and modules. Simulation of IQE droop. Design of superlattice.

More information

UNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences. EECS 130 Professor Ali Javey Fall 2006

UNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences. EECS 130 Professor Ali Javey Fall 2006 UNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences EECS 130 Professor Ali Javey Fall 2006 Midterm 2 Name: SID: Closed book. Two sheets of notes are

More information

Dual-metal-gate Structure of AlGaN/GaN MIS HEMTs Analysis and Design

Dual-metal-gate Structure of AlGaN/GaN MIS HEMTs Analysis and Design Dual-metal-gate Structure of AlGaN/GaN MIS HEMTs Analysis and Design Mr. Gaurav Phulwari 1, Mr. Manish Kumar 2 Electronics & Communication Engineering 1, 2, Bhagwant University, Ajmer 1,2 M.Tech Scholar

More information

Device 3D. 3D Device Simulator. Nano Scale Devices. Fin FET

Device 3D. 3D Device Simulator. Nano Scale Devices. Fin FET Device 3D 3D Device Simulator Device 3D is a physics based 3D device simulator for any device type and includes material properties for the commonly used semiconductor materials in use today. The physical

More information

Schottky Rectifiers Zheng Yang (ERF 3017,

Schottky Rectifiers Zheng Yang (ERF 3017, ECE442 Power Semiconductor Devices and Integrated Circuits Schottky Rectifiers Zheng Yang (ERF 3017, email: yangzhen@uic.edu) Power Schottky Rectifier Structure 2 Metal-Semiconductor Contact The work function

More information

ANALYSIS AND MODELING OF 1/f NOISE IN IGZO TFTS

ANALYSIS AND MODELING OF 1/f NOISE IN IGZO TFTS ANALYSIS AND MODELING OF 1/f NOISE IN IGZO TFTS Gerard Uriarte, Wondwosen E. Muhea, Benjamin Iñiguez Dep. of Electronic Engineering, University Rovira i Virgili, Tarragona (Spain) Thomas Gneiting AdMOS

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

Investigation of the Thermal Noise of MOS Transistors under Analog and RF Operating Conditions

Investigation of the Thermal Noise of MOS Transistors under Analog and RF Operating Conditions Investigation of the Thermal Noise of MOS Transistors under Analog and RF Operating Conditions Ralf Brederlow 1, Georg Wenig 2, and Roland Thewes 1 1 Infineon Technologies, Corporate Research, 2 Technical

More information

Application II: The Ballistic Field-E ect Transistor

Application II: The Ballistic Field-E ect Transistor Chapter 1 Application II: The Ballistic Field-E ect Transistor 1.1 Introduction In this chapter, we apply the formalism we have developed for charge currents to understand the output characteristics of

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

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

Field-Effect (FET) transistors

Field-Effect (FET) transistors Field-Effect (FET) transistors References: Barbow (Chapter 8), Rizzoni (chapters 8 & 9) In a field-effect transistor (FET), the width of a conducting channel in a semiconductor and, therefore, its current-carrying

More information

ANALYSIS OF POWER EFFICIENCY FOR FOUR-PHASE POSITIVE CHARGE PUMPS

ANALYSIS OF POWER EFFICIENCY FOR FOUR-PHASE POSITIVE CHARGE PUMPS ANALYSS OF POWER EFFCENCY FOR FOUR-PHASE POSTVE CHARGE PUMPS Chien-pin Hsu and Honchin Lin Department of Electrical Enineerin National Chun-Hsin University, Taichun, Taiwan e-mail:hclin@draon.nchu.edu.tw

More information

Current mechanisms Exam January 27, 2012

Current mechanisms Exam January 27, 2012 Current mechanisms Exam January 27, 2012 There are four mechanisms that typically cause currents to flow: thermionic emission, diffusion, drift, and tunneling. Explain briefly which kind of current mechanisms

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

Final Examination EE 130 December 16, 1997 Time allotted: 180 minutes

Final Examination EE 130 December 16, 1997 Time allotted: 180 minutes Final Examination EE 130 December 16, 1997 Time allotted: 180 minutes Problem 1: Semiconductor Fundamentals [30 points] A uniformly doped silicon sample of length 100µm and cross-sectional area 100µm 2

More information

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

SECTION: Circle one: Alam Lundstrom. ECE 305 Exam 5 SOLUTIONS: Spring 2016 April 18, 2016 M. A. Alam and M.S. Lundstrom Purdue University NAME: PUID: SECTION: Circle one: Alam Lundstrom ECE 305 Exam 5 SOLUTIONS: April 18, 2016 M A Alam and MS Lundstrom Purdue University This is a closed book exam You may use a calculator and the formula

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 Bond Model of Electrons and Holes Si Si Si Si Si Si Si Si Si Silicon

More information

Field effect = Induction of an electronic charge due to an electric field Example: Planar capacitor

Field effect = Induction of an electronic charge due to an electric field Example: Planar capacitor JFETs AND MESFETs Introduction Field effect = Induction of an electronic charge due to an electric field Example: Planar capacitor Why would an FET made of a planar capacitor with two metal plates, as

More information

3D Simulation of SiC MESFET

3D Simulation of SiC MESFET Lighting Up Semiconductor World 3D Simulation of SiC MESFET Crosslight Software, Inc., Vancouver, BC, Canada, (604)320-1704, www.crosslight.com Introduction Introduction to Simulation Flow 3D simulation

More information

Traps in MOCVD n-gan Studied by Deep Level Transient Spectroscopy and Minority Carrier Transient Spectroscopy

Traps in MOCVD n-gan Studied by Deep Level Transient Spectroscopy and Minority Carrier Transient Spectroscopy Traps in MOCVD n-gan Studied by Deep Level Transient Spectroscopy and Minority Carrier Transient Spectroscopy Yutaka Tokuda Department of Electrical and Electronics Engineering, Aichi Institute of Technology,

More information

Investigation of Buffer Traps in AlGaN/GaN Heterostructure Field-Effect Transistors Using a Simple Test Structure

Investigation of Buffer Traps in AlGaN/GaN Heterostructure Field-Effect Transistors Using a Simple Test Structure http://dx.doi.org/10.5573/jsts.2014.14.4.478 JOURNAL OF SEMICONDUCTOR TECHNOLOGY AND SCIENCE, VOL.14, NO.4, AUGUST, 2014 Investigation of Buffer Traps in AlGaN/GaN Heterostructure Field-Effect Transistors

More information

Typical example of the FET: MEtal Semiconductor FET (MESFET)

Typical example of the FET: MEtal Semiconductor FET (MESFET) Typical example of the FET: MEtal Semiconductor FET (MESFET) Conducting channel (RED) is made of highly doped material. The electron concentration in the channel n = the donor impurity concentration N

More information

EE 446/646 Photovoltaic Devices I. Y. Baghzouz

EE 446/646 Photovoltaic Devices I. Y. Baghzouz EE 446/646 Photovoltaic Devices I Y. Baghzouz What is Photovoltaics? First used in about 1890, the word has two parts: photo, derived from the Greek word for light, volt, relating to electricity pioneer

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

Complete Surface-Potential Modeling Approach Implemented in the HiSIM Compact Model Family for Any MOSFET Type

Complete Surface-Potential Modeling Approach Implemented in the HiSIM Compact Model Family for Any MOSFET Type Complete Surface-Potential Modeling Approach Implemented in the HiSIM Compact Model Family for Any MOSFET Type WCM in Boston 15. June, 2011 M. Miura-Mattausch, M. Miyake, H. Kikuchihara, U. Feldmann and

More information

Polarization Induced 2DEG in AlGaN/GaN HEMTs: On the origin, DC and transient characterization. Ramakrishna Vetury. Committee

Polarization Induced 2DEG in AlGaN/GaN HEMTs: On the origin, DC and transient characterization. Ramakrishna Vetury. Committee Polarization Induced 2DEG in AlGaN/GaN HEMTs: On the origin, DC and transient characterization by Ramakrishna Vetury Committee Dr. James Ibbetson Prof. Evelyn Hu Prof. Robert York Prof. Umesh Mishra Acknowledgements

More information

GaN based transistors

GaN based transistors GaN based transistors S FP FP dielectric G SiO 2 Al x Ga 1-x N barrier i-gan Buffer i-sic D Transistors "The Transistor was probably the most important invention of the 20th Century The American Institute

More information

Appendix 1: List of symbols

Appendix 1: List of symbols Appendix 1: List of symbols Symbol Description MKS Units a Acceleration m/s 2 a 0 Bohr radius m A Area m 2 A* Richardson constant m/s A C Collector area m 2 A E Emitter area m 2 b Bimolecular recombination

More information

OPTIMIZATION OF OFF-STATE BREAKDOWN VOLTAGE IN GAN HIGH ELECTRON MOBILITY TRANSISTORS

OPTIMIZATION OF OFF-STATE BREAKDOWN VOLTAGE IN GAN HIGH ELECTRON MOBILITY TRANSISTORS OPTIMIZATION OF OFF-STATE BREAKDOWN VOLTAGE IN GAN HIGH ELECTRON MOBILITY TRANSISTORS By Begum Kasap Senior Thesis in Electrical Engineering University of Illinois at Urbana-Champaign Advisor: Can Bayram

More information

Electronics Fets and Mosfets Prof D C Dube Department of Physics Indian Institute of Technology, Delhi

Electronics Fets and Mosfets Prof D C Dube Department of Physics Indian Institute of Technology, Delhi Electronics Fets and Mosfets Prof D C Dube Department of Physics Indian Institute of Technology, Delhi Module No. #05 Lecture No. #02 FETS and MOSFETS (contd.) In the previous lecture, we studied the working

More information

Self-heating simulation of GaN-based metal-oxide-semiconductor high-electron-mobility transistors including hot electron and quantum effects

Self-heating simulation of GaN-based metal-oxide-semiconductor high-electron-mobility transistors including hot electron and quantum effects JOURNAL OF APPLIED PHYSICS 100, 074501 2006 Self-heating simulation of GaN-based metal-oxide-semiconductor high-electron-mobility transistors including hot electron and quantum effects W. D. Hu, X. S.

More information

Strain and Temperature Dependence of Defect Formation at AlGaN/GaN High Electron Mobility Transistors on a Nanometer Scale

Strain and Temperature Dependence of Defect Formation at AlGaN/GaN High Electron Mobility Transistors on a Nanometer Scale Strain and Temperature Dependence of Defect Formation at AlGaN/GaN High Electron Mobility Transistors on a Nanometer Scale Chung-Han Lin Department of Electrical & Computer Engineering, The Ohio State

More information

HOT-CARRIER RELIABILITY SIMULATION IN AGGRESSIVELY SCALED MOS TRANSISTORS. Manish P. Pagey. Dissertation. Submitted to the Faculty of the

HOT-CARRIER RELIABILITY SIMULATION IN AGGRESSIVELY SCALED MOS TRANSISTORS. Manish P. Pagey. Dissertation. Submitted to the Faculty of the HOT-CARRIER RELIABILITY SIMULATION IN AGGRESSIVELY SCALED MOS TRANSISTORS By Manish P. Pagey Dissertation Submitted to the Faculty of the Graduate School of Vanderbilt University in partial fulfillment

More information

CHAPTER 2 PHYSICS OF LEDS

CHAPTER 2 PHYSICS OF LEDS CHAPTER 2 PHYSICS OF LEDS 2.1 LIGHT EMITTING DIODE A light-emitting diode (LED) is simply a two terminal p-n junction diode, which emits light when forward bias is applied across the terminals. When an

More information

Planar View of Structural Degradation in GaN HEMT: Voltage, Time and Temperature Dependence

Planar View of Structural Degradation in GaN HEMT: Voltage, Time and Temperature Dependence Planar View of Structural Degradation in GaN HEMT: Voltage, Time and Temperature Dependence Jungwoo Joh 1, Prashanth Makaram 2 Carl V. Thompson 2 and Jesús A. del Alamo 1 1 Microsystems Technology Laboratories,

More information

Time Dependent Dielectric Breakdown in High Voltage GaN MIS HEMTs: The Role of Temperature

Time Dependent Dielectric Breakdown in High Voltage GaN MIS HEMTs: The Role of Temperature Time Dependent Dielectric Breakdown in High Voltage GaN MIS HEMTs: The Role of Temperature Shireen Warnock, Allison Lemus, and Jesús A. del Alamo Microsystems Technology Laboratories (MTL) Massachusetts

More information

Reliability and Instability of GaN MIS-HEMTs for Power Electronics

Reliability and Instability of GaN MIS-HEMTs for Power Electronics Reliability and Instability of GaN MIS-HEMTs for Power Electronics Jesús A. del Alamo, Alex Guo and Shireen Warnock Microsystems Technology Laboratories Massachusetts Institute of Technology 2016 Fall

More information

The physical process analysis of the capacitance voltage characteristics of AlGaN/AlN/GaN high electron mobility transistors

The physical process analysis of the capacitance voltage characteristics of AlGaN/AlN/GaN high electron mobility transistors Chin. Phys. B Vol. 9, No. 9 200 097302 The physical process analysis of the capacitance voltage characteristics of AlGaN/AlN/GaN high electron mobility transistors Wang Xin-Hua, Zhao Miao, Liu Xin-Yu,

More information

MOSFET Model with Simple Extraction Procedures, Suitable for Sensitive Analog Simulations

MOSFET Model with Simple Extraction Procedures, Suitable for Sensitive Analog Simulations ROMANIAN JOURNAL OF INFORMATION SCIENCE AND TECHNOLOGY Volume 10, Number 2, 2007, 189 197 MOSFET Model with Simple Extraction Procedures, Suitable for Sensitive Analog Simulations S. EFTIMIE 1, ALEX. RUSU

More information

Fundamentals of the Metal Oxide Semiconductor Field-Effect Transistor

Fundamentals of the Metal Oxide Semiconductor Field-Effect Transistor Triode Working FET Fundamentals of the Metal Oxide Semiconductor Field-Effect Transistor The characteristics of energy bands as a function of applied voltage. Surface inversion. The expression for the

More information

EE C245 - ME C218 Introduction to MEMS Design Fall Today s Lecture

EE C245 - ME C218 Introduction to MEMS Design Fall Today s Lecture EE C45 ME C18 Introduction to MEMS Desin all 3 Roer Howe and Thara Srinivasan Lecture 1 Electrostatic Actuators I Today s Lecture Enery in electromechanical systems define carefully Parallelplate electrostatic

More information

Low Switching Loss and Scalable V LDMOS Transistors with Low Specific On-Resistance

Low Switching Loss and Scalable V LDMOS Transistors with Low Specific On-Resistance International Conference on Technology and Social Science 218 (ICTSS 218) Invited Low Switching Loss and Scalable 2-4 V LDMOS Transistors with Low Specific On-Resistance Jun-ichi Matsuda, Jun-ya Kojima,

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

Performance Analysis of Ultra-Scaled InAs HEMTs

Performance Analysis of Ultra-Scaled InAs HEMTs Purdue University Purdue e-pubs Birck and NCN Publications Birck Nanotechnology Center 2009 Performance Analysis of Ultra-Scaled InAs HEMTs Neerav Kharche Birck Nanotechnology Center and Purdue University,

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