Ge Semiconductor Devices for Cryogenic Power Electronics - V

Slides:



Advertisements
Similar presentations
POWER ELECTRONICS Instructor: Eng.Moayed N. EL Mobaied The Islamic University of Gaza Faculty of Engineering Electrical Engineering Department بسم الله.
Advertisements

Power Semiconductor Systems I
Instructor Name: (Your Name)
Justin Chow Jacob Huang Daniel Soledad ME 4447/6405 Student Lecture.
Transistors These are three terminal devices, where the current or voltage at one terminal, the input terminal, controls the flow of current between the.
Basic Electronics Ninth Edition Basic Electronics Ninth Edition ©2002 The McGraw-Hill Companies Grob Schultz.
MOSFETs Monday 19 th September. MOSFETs Monday 19 th September In this presentation we will look at the following: State the main differences between.
For the exclusive use of adopters of the book Introduction to Microelectronic Fabrication, Second Edition by Richard C. Jaeger. ISBN © 2002.
Power Diodes for Cryogenic Operation PESC 2003 Acapulco, Mexico, June 2003.
Chap. 5 Field-effect transistors (FET) Importance for LSI/VLSI –Low fabrication cost –Small size –Low power consumption Applications –Microprocessors –Memories.
Semiconductor circuit elements and dependent sources
Principles & Applications
Basic Bipolar Process Description Bipolar Process Flow –Vertical npn –Lateral pnp –JFET –Prepared by Randy Geiger, September 2001.
BJT Processing 1. Implantation of the buried n + layer 2. Growth of the epitaxial layer 3. p + isolation diffusion 4. Base p-type diffusion 5. Emitter.
Chapter 28 Basic Transistor Theory. 2 Transistor Construction Bipolar Junction Transistor (BJT) –3 layers of doped semiconductor –2 p-n junctions –Layers.
Power Electronics Lecture-9 Power Transistors & GTO Dr. Imtiaz Hussain
1 Bipolar Junction Transistor Models Professor K.N.Bhat Center for Excellence in Nanoelectronics ECE Department Indian Institute of Science Bangalore-560.
09/16/2010© 2010 NTUST Today Course overview and information.
Transistors Three-terminal devices with three doped silicon regions and two P-N junctions versus a diode with two doped regions and one P-N junction Two.
Field-Effect Transistor
Module 2 Bipolar Junction Transistor. Learning Outcomes 1.The 3 terminals or regions of a BJT. 2.Construction and symbol of NPN and PNP types 3.Low power.
Junction Field Effect Transistor
Field-Effect Transistors
Digital Integrated Circuits© Prentice Hall 1995 Introduction The Devices.
Chapter 5: Field–Effect Transistors
Principles & Applications
Power Semiconductor Devices for Low-Temperature Environments Space Power Workshop April 2004, Manhattan Beach, California.
Principles & Applications
Power Semiconductor Devices for Low-Temperature Environments - II Space Power Workshop April 2005, Manhattan Beach, California.
Chapter 5: Field Effect Transistor
© 2013 The McGraw-Hill Companies, Inc. All rights reserved. McGraw-Hill 5-1 Electronics Principles & Applications Eighth Edition Chapter 5 Transistors.
TRANSISTOR.  A transistor is a semiconductor device used to amplify and switch electronic signals and electrical power.  The transistor is the fundamental.
BJTs. Transistor The transistor is the main building block “element” of electronics. A transistor is a semiconductor device used to amplify and switch.
Novel SiGe Semiconductor Devices for Cryogenic Power Electronics ICMC/CEC August-September 2005 Keystone, Colorado.
Field Effect Transistor. What is FET FET is abbreviation of Field Effect Transistor. This is a transistor in which current is controlled by voltage only.
SiGe Semiconductor Devices for Cryogenic Power Electronics
Field Effect Transistors
NEPP - April/May 2002 Semiconductor Device Options for Low-Temperature Electronics R. K. Kirschman, R. R. Ward and W. J. Dawson GPD Optoelectronics Corp.,
ISAT 436 Micro-/Nanofabrication and Applications Transistors David J. Lawrence Spring 2004.
Introduction to Transistors
Electronics The ninth and tenth lectures Ninth week 5 - 8/ 1/ 1437 هـ أ / سمر السلمي.
McGraw-Hill 5-1 © 2013 The McGraw-Hill Companies, Inc. All rights reserved. Electronics Principles & Applications Eighth Edition Chapter 5 Transistors.
Power Semiconductor Devices Power Diodes Cross-sectional view of a pn- junction diode intended for power applications. I-V characteristics of a pn- junction.
Electronics The Fourteenth Fifteenth Lectures Twelfth week / 1/ 1437 هـ أ / سمر السلمي.
Full-Wave (Bridge) Rectifier
Electronics The Twelfth and Thirteenth Lectures Eleventh week / 1/ 1437 هـ أ / سمر السلمي.
Junction Field Effect Transistor
 A transistor: a three-terminal semiconductor device that can perform two functions: amplification and switching.  Amplification consists of magnifying.
1 Other Transistor Topologies 30 March and 1 April 2015 The two gate terminals are tied together to form single gate connection; the source terminal is.
SMV ELECTRIC TUTORIALS Aditya Kuroodi 2016 Relevant Course(s): EE121B, EE115A.
AMATEUR RADIO OPERATOR INTRODUCTION January 2013 Active Devices Diodes, Transistors, and Tubes.
Development of Ge JFETs for Deep-Cryogenic Preamplifiers SPIE - Astronomical Telescopes and Instrumentation Hawai’i, August 2002.
Field Effect Transistors
COURSE NAME: SEMICONDUCTORS Course Code: PHYS 473 Week No. 8.
TRANSISTORS AND THYRISTORS
SILVER OAK COLLEGE OF ENGG. & TECHNOLOGY  SUB – Electronics devices & Circuits  Topic- JFET  Student name – Kirmani Sehrish  Enroll. No
BJT transistors FET ( Field Effect Transistor) 1. Unipolar device i. e. operation depends on only one type of charge carriers (h or e) 2. Voltage controlled.
Transistors Different types and sizes BJT (PNP) Electrical Diagram First Transistor Modern Electronics FET and BJT Transistor.
Power Electronics Prof. Mohammed Zeki Khedher
Different Types of Transistors and Their Functions
SiC Power Devices Vaibhav Ostwal
Instrumentation & Power Electronic Systems
Chapter 2 Overview of Power Semiconductor Devices
IGBT.
Power Semiconductor Systems I
UNIT 2 POWER TRANSISTORS
Bipolar Processes Description
ECE 442 Power Electronics Text:
Introduction Dr. Kakade K.P.
9 Transistor Fundamentals.
Presentation transcript:

Ge Semiconductor Devices for Cryogenic Power Electronics - V WOLTE 6 Ge Semiconductor Devices for Cryogenic Power Electronics - V ESA/ESTEC, Noordwijk, June 2004

Supported by NASA Glenn Research Center R. R. Ward, W. J. Dawson, L. Zhu, R. K. Kirschman GPD Optoelectronics Corp., Salem, New Hampshire O. Mueller, M. J. Hennessy, E. K. Mueller MTECH Laboratories, Ballston Spa, New York R. L. Patterson, J. E. Dickman NASA Glenn Research Center, Cleveland, Ohio A. Hammoud QSS Group Inc., Cleveland, Ohio Supported by NASA Glenn Research Center

“Very Little of the Solar System (or the Universe) Is at Room Temperature.”

Temperatures for Spacecraft

Solar System Exploration Fly-by, orbiters, landers, rovers, probes, penetrators Using conventional electronics in cold environments - Heating - Wake/sleep (where possible)

“Traditional” Spacecraft COLD ENVIRONMENT CONVENTIONAL ELECTRONICS HEATING/COOLING SYSTEM TEMPERATURE CONTROL THERMAL INSULATION (HEAT STORAGE)

“Cold” Spacecraft CRYOGENIC ELECTRONICS COLD ENVIRONMENT

“Cold” Spacecraft Benefits Eliminate heating, thermal control, isolation Reduce power, weight, size, cost, complexity Improve overall reliability Reduce disruption of environment Increase mission duration & capability

Development Program

Cryogenic Power Electronics Active semiconductor devices for power circuits For spacecraft power management & actuator control Parameters Power ~10 W Temperature range 300 K to ~20 K Device types Diodes (P--N, 10 A, 300 V) JFETs (lateral, vertical) MISFETs (lateral, vertical) BJTs (vertical implanted) Based on Ge

Why Use Ge?

Why Ge Devices? Applications require operation to 30 – 40 K range Ge devices of all types can operate to low cryogenic temperatures (~20 K or lower) Diodes Field-effect transistors (JFETs, MISFETs) Bipolar transistors Performance advantages P-N junction voltages are low Mobility is high

Ge Cryo Power Diodes

Ge Cryo Power Diodes P- - N Bulk Design Metal P+ implant Guard ring(s) N– ( ) Metal N+ implant

Ge Diode - Forward I-V

Ge Diode - Forward I-V

Ge Diode - Forward I-V

Ge Diodes - Forward Voltage Si data from literature

Ge Diodes - Forward Voltage Si data from literature

Ge Diodes - Reverse Breakdown

Ge Diodes - Reverse Recovery

Ge Diodes - Reverse Recovery

Ge Diodes - Reverse Recovery

Ge Cryo Power Field-Effect Transistors

Ge Cryo Power JFET or MISFET ~1.3 mm G S D

Ge Cryo Power JFETs (Junction Field-Effect Transistors)

Ge JFET Cross-Section (n-channel) Back gate contact Source Front gate P+ implant P+ substrate N epitaxial layer N+ implant Drain

Ge JFET at 300 K (n-channel) ΔVGS = 1 V/step J42 2004-01 10 V

Ge JFET at 77 K (n-channel) ΔVGS = 1 V/step 10 V

Ge JFET at 4 K (n-channel) ΔVGS = 1 V/step 10 V

Ge JFET at 300 K (p-channel) ΔVGS = 1 V/step JL2-01B-Q01, Quad JFET 50 V

Ge JFET at 77 K (p-channel) ΔVGS = 1 V/step 50 V

Ge JFET at 4 K (p-channel) ΔVGS = 1 V/step 50 V

Ge JFET Cross-Section (p-channel) Back gate contact Source (N+ implant) N+ substrate P epitaxial layer P+ implant Drain Trench

Ge JFET at 300 K (p-channel) ΔVGS = 2 V/step JL2-01B-Q01, Quad JFET 20 V

Ge JFET at 77 K (p-channel) ΔVGS = 2 V/step 20 V

Ge JFET at 4 K (p-channel) ΔVGS = 2 V/step 20 V

Ge Cryo Power MISFETs (Metal-Insulator-Semiconductor Field-Effect Transistors)

Lateral Ge MISFET Design (n-channel) Substrate contact Source Gate (P+ implant) P substrate Gate dielectric N+ implant Drain

Ge MISFET at 300 K (n-channel) ΔVGS = 1 V/step M31 20 V

Ge MISFET at 77 K (n-channel) ΔVGS = 1 V/step 20 V

Ge MISFET at 4 K (n-channel) ΔVGS = 1 V/step 20 V

Ge MISFET Switching - 50 kHz ~30 W Load

Ge MISFET Switching - 5 MHz ~30 W Load

Ge MISFET at 300 K (p-channel) ΔVGS = 2 V/step M31 20 V

Ge MISFET at 77 K (p-channel) ΔVGS = 2 V/step 20 V

Ge MISFET at 4 K (p-channel) ΔVGS = 2 V/step 20 V

Vertical Ge MISFET Design (n-channel) Drain Source Gate P+ implant P– substrate Gate dielectric N epi

Ge Vertical MISFET at 77 K (n-channel) ΔVGS = 2 V/step 10 V

Ge Bipolar Junction Transistors

Ge Bipolar – Double-Implant, Vertical Emitter Base N+ implant P implant N– substrate Collector N+ implant

Ge BJT at 77 K (npn) ΔIB = 1 mA/step 0.1 A 10 V

Ge BJT at 77 K (pnp) ΔIB = 2 mA/step 0.05 A 100 V

Summary Cryogenic power electronics is needed for spacecraft going to cold environments and for space observatories Temperatures may be as low as ~30 - 40 K Used Ge Ge devices of all types can operate to deep cryogenic temperatures – to 20 K, as low as 4 K We developed Ge diodes, JFETs, MISFETs, BJTs specifically for cryogenic power applications Power to ~20 W

Continuing Development Now developing cryogenic power devices based on SiGe Flexibility, compatibility, easier dielectric Two separate programs: NASA (spacecraft) and DARPA (motors & generators using superconductors) Temperature ranges: to ~20 K (NASA, medium power) and ~55 K (DARPA, higher power) HBTs, MOSFETs, IGBTs (NASA); diodes, thyristors (DARPA) Simulation, fabrication, evaluation Demonstrations of SiGe devices in ~100 - 1000 W power converters at cryogenic temperatures