Silicon Semiconductor Technology

Total Page:16

File Type:pdf, Size:1020Kb

Silicon Semiconductor Technology Runyan TEXAS INSTRUMENTS INCORPORATED Semiconductor·Components Division EXAS INSTRUMENTS INCORPORATED Silicon Semiconductor Technology W. R. Runyan Texas Instruments Electronics Series McGraw·HiII McGraw-Hili Beok Company 54276 Silicon Semiconductor Technology The Engineering Staff of Texas Instruments Incorporated • TRANSISTOR CIRCUIT DESIGN Runyan • SILICON SEMICONDUCTOR TECHNOLOGY Sevin • FIELD-EFFECT TRANSISTORS Silicon Semiconductor Technology w. R. Runyan Semiconductor Research and Development Laboratory Texas Instruments Incorporated McGRAW-HILL BOOK COMPANY New York San Francisco Toronto London Sydney SILICON SEMICONDUCTOR TECHNOLOGY Copyright © 1965 by Texas Instruments Incorporated. All Rights Reserved. Printed in the United States of America. This book, or parts thereof, may not be reproduced in any form without permission of Texas Instru­ ments Incorporated. Library of Congress Catalog Card Number 64-24607. Information contained in this book is believed to be accurate and reliable. However, responsibility is assumed neither for its use nor for any infringement of patents or rights of others which may result from its use. No license is granted by implication or otherwise under any patent or patent right of Texas Instruments or others. 54276 345678 9-MP-9 8 7 6 Preface The purposes of this book are to provide in a single reference the properties of silicon important to those who would use it as a semiconductor and to discuss at length several of the more important semiconductor technologies, such as crystal growing and diffusion. It had its beginning in a set of notes I began compiling shortly after starting work in the semiconductor industry. Since most of my activ­ ities were with silicon, these notes were restricted to information pertaining to that material. A few years later, while teaching a graduate course in semiconductor technology at Southern Methodist University, the notes were expanded from a col­ lection of data to a unified coverage of topics relating to semiconductor material technology and were used as an adjunct to a general text. However, because of my interest in silicon, after the semiconductor material technology was presented in some depth it was then applied specifically to silicon. This in no sense restricts the book's use to those interested only in silicon since the majority of each of those chapters not relating to specific silicon properties discusses each technology inde­ pendent of the material. While this book will be of most interest to device designers and those working as semiconductor technologists, it should also prove of considerable interest to those using devices, both circuit designers and systems engineers, in that it will supply background information and material properties helpful in understanding device performance. An attempt was made to cover all aspects of the technology except those relating to the surface itself. The complexity of surface behavior would warrant a separate volume and is beyond the scope of this book. In addition, where there are books covering some phase ofthe technology in great detail, e.g., Pfann's "Zone Melting," only a cursory treatment is given. -.J. The author would like to thank Harry L. Owens for his continued interest and support, Dr. Lyndon Taylor of the University of Texas and Dr. W. E. Phillips of Texas Technology College for a critical reading of the manuscript, John R. Miller for editorial advice, Virginia Belshaw for typing, Stacy B. Watelski for the photo­ micrographs, Earl W. Scott of Scott's Studio for the crystal photographs of Chap. 4, and the photographic staff of Texas Instruments Incorporated for all other photog­ raphy. In addition, the help of the many other members of the Semiconductor Research and Development Laboratory of Texas Instruments Incorporated is gratefully acknowledged. W R. Runyan v Foreword It is particularly timely for a book to appear on the subject of silicon semicon­ ductor technology. Until the past few years the semiconductor device industry was based largely on germanium technology, with silicon being restricted chiefly to military and power applications. During recent years silicon technology has been developed so that silicon now promises, along with germanium, to have broad usage. Integrated circuits have been developed almost exclusively around silicon technology. While these were developed first for military applications, they will be applied broadly to industrial and consumer markets. It is also evident that future generations of devices will be far more sophisticated than those now in use, and that a much better understand­ ing and blending of material properties with device functions will be required. Dr. Runyan has written a book which should prove to be a useful addition to the literature on semiconductor technology and an aid in this blending process. He is especially well qualified to author such a book since much of his professional career has been devoted to research and development on silicon materials and devices. At present he leads the materials research program in the Semiconductor Research and Development Laboratory at Texas Instruments. This book is a part of the new Texas Instruments Electronics Series, through which we hope to make readily available to the technical community important research findings which will further the progress of the electronics industry. Richard L. Petritz, DIRECTOR SEMICONDUCTOR RESEARCH AND DEVELOPMENT LABORATORY vi Contents Preface............................ ...... .............. ......... v Foreword . vi Chapter 1 . An Historical Note . .. 1 REFERENCES ..................................................... 3 Chapter 2. Silicon-manufacturing Processes . .. 5 2.1 Early Methods of Manufacture. 5 2.2 Summary of Applicable Methods . 7 2.3 Zinc-Silicon Tetrachloride ................................... 7 2.4 Silane Decomposition . 9 2.5 Iodide Process . .. 10 2.6 Silicon Tetrachloride and Trichlorosilane Processes . .. 12 REFERENCES. .. 14 Chapter 3. Silicon-casting Processes . .. 17 3.1 Melting in Mold. .. 17 3.2 Pouring into Mold. .. 22 3.3 Ambit Casting. .. 24 REFERENCES. .. 27 Chapter 4. Crystal Growth . .. 29 4.1 Crystal-growing Environment ................................ 29 4.2 Types of Crystal Growth . .. 30 4.3 Crystallization from a One-component System. .. 32 4.4 Growth from Multicomponent Systems. .. 36 4.5 Teal-Little................................................. 38 4.6 Behavior of Impurities During Growth from the Melt. .. 49 4.7 Miscellaneous Techniques. .. 60 4.8 Growth from Low-temperature Melts ........................ " 63 4.9 Vapor-Liquid-Solid (VLS) Method of Crystal Growth. .. 65 4.10 Growth from the Vapor . .. 65 REFERENCES 78 vii viii Contents o Chapter 5. Crystal Habit and Orientation . .. 84 5.1 Crystal Systems ............................................ 84 5.2 Silicon Structure. .. 88 5.3 Crystal Habit ..... .. 89 5.4 Rough Orientation. .. 93 5.5 X-ray Orientation .......................................... 94 5.6 Optical Orientation. .. 97 5.7 Twinning.................................................. 98 5.8 Detection of Twinning ...................................... 101 5.9 Grain Boundaries. .. 101 5.10 Lineage ................................................ 102 REFERENCES 102 Chapter 6. Doping Procedures ........................................ 104 6.1 Effects ofImpurities on Resistivity. .. 104 6.2 Effect of Segregation Coefficient on Resistivity . .. 107 6.3 Methods of Doping . .. 110 6.4 Discussion of Crystal Yields. .. 114 REFERENCES 116 Chapter 7. Diffusion ................................................ 117 7.l Elementary Theory .......................................... 117 7.2 Diffusion Along a Grain Boundary ............................ l33 7.3 Field-aided Diffusion ........................................ l36 7.4 Numerical Calculations. .. l37 7.5 Diffusion Processes ......................................... 141 7.6 Diffusion Coefficients ....................................... 151 REFERENCES ................................................ 159 Chapter 8. Electrical Properties ....................................... 164 8.1 Resistivity ................................................ 164 8.2 Mobility .................................................. 166 8.3 Drift Mobility ............................................. 168 8.4 Hall Coefficient and Hall Mobility ........................... 169 8.5 Effects of High Field on Resistivity ........................... 172 8.6 Width of Space-charge Region in p-n Junctions ................ 174 8.7 Effects of Pressure ......................................... 176 8.8 Energy Bands ............................................. 182 8.9 Effective Masses for Electron and Holes ....................... 183 8.10 Miscellaneous Effects ..... 185 REFERENCES ............................................... 185 Contents ix Chapter 9. Optical Properties ....................................... 187 9.l Absorption Coefficients. .. 187 9.2 Photoconductivity ......................................... 197 9.3 Reflection Coefficient. .. 198 9.4 Index of Refraction ........................................ 198 9.5 Emissivity ................................................ 200 9.6 Light Emission ............................................ 200 9.7 Tyndall Effect ............................................. 203 9.8 Birefringence ............................................. 203 9.9 Optical Elements .......................................... 204 9.10 Optical Coatings ..........................................
Recommended publications
  • Pp-03-25-New Dots.Qxd 10/23/02 2:41 PM Page 778
    pp-03-25-new dots.qxd 10/23/02 2:41 PM Page 778 778 PRAESODYMIUM PRAESODYMIUM [7440–10–0] Symbol Pr; atomic number 59; atomic weight 140.908; a lanthanide–series rare earth element; belongs to the cerium group of rare earths; electron con- figuration [Xe] 4f36s2; partially filled f subshell; valence states +3, +4; most 3+ stable oxidation state +3; electrode potential E°/V (aq) for Pr + 3e¯ ↔ Pr is –2.35 V; atomic radius 1.828 Å; first ionization potential 5.46 eV; one natu- rally–occurring isotope, Pr–141; twenty–nine artificial radioactive isotopes known in the mass range 124, 126–140 and 142–154; the longest–lived isotope Pr–143, t1/2 13.57 day, and the shortest–lived isotope Pr–124, t1/2 1.2 second. History, Occurrence, and Uses Mosander extracted from the mineral lanthana a rare earth fraction, named didymia in 1841. In 1879, Boisbaudran separated a rare earth oxide called samaria (samarium oxide) from the didymia fraction obtained from the mineral samarskite. Soon after that in 1885, Baron Auer von Welsbach iso- lated two other rare earths from didymia. He named them as praseodymia (green twin) and neodymia (new twin) after their source didymia (twin). The name praseodymium finally was assigned to this new element, derived from the two Greek words, prasios meaning green and didymos meaning twin. Praseodymium occurs in nature associated with other rare earths in a rel- atively high abundance. It is more abundant than some common metals such as silver, gold, or antimony. The average concentration of this metal in the earth’s crust is estimated to be 8.2 mg/kg.
    [Show full text]
  • The Preparation and Reactions of the Lower Chlorides and Oxychlorides of Silicon Joseph Bradley Quig Iowa State College
    Iowa State University Capstones, Theses and Retrospective Theses and Dissertations Dissertations 1926 The preparation and reactions of the lower chlorides and oxychlorides of silicon Joseph Bradley Quig Iowa State College Follow this and additional works at: https://lib.dr.iastate.edu/rtd Part of the Inorganic Chemistry Commons Recommended Citation Quig, Joseph Bradley, "The preparation and reactions of the lower chlorides and oxychlorides of silicon " (1926). Retrospective Theses and Dissertations. 14278. https://lib.dr.iastate.edu/rtd/14278 This Dissertation is brought to you for free and open access by the Iowa State University Capstones, Theses and Dissertations at Iowa State University Digital Repository. It has been accepted for inclusion in Retrospective Theses and Dissertations by an authorized administrator of Iowa State University Digital Repository. For more information, please contact [email protected]. INFORMATION TO USERS This manuscript has been reproduced from the microfilm master. UlVli films the text directly from the original or copy submitted. Thus, some thesis and dissertation copies are in typewriter face, while others may be from any type of computer printer. The quality of this reproduction is dependent upon the quality of the copy submitted. Broken or indistinct print, colored or poor quality illustrations and photographs, print bleedthrough, substandard margins, and impiroper alignment can adversely affect reproduction. In the unlikely event that the author did not send UMI a complete manuscript and there are missing pages, these will be noted. Also, if unauthorized copyright material had to be removed, a note will indicate the deletion. Oversize materials (e.g., maps, drawings, charts) are reproduced by sectioning the original, beginning at the upper left-hand corner and continuing from left to right in equal sections with small overiaps.
    [Show full text]
  • Chapter1: Semiconductor Diode
    Chapter1: Semiconductor Diode. Electronics I Discussion Eng.Abdo Salah Theoretical Background: • The semiconductor diode is formed by doping P-type impurity in one side and N-type of impurity in another side of the semiconductor crystal forming a p-n junction as shown in the following figure. At the junction initially free charge carriers from both side recombine forming negatively c harged ions in P side of junction(an atom in P -side accept electron and be comes negatively c harged ion) and po sitive ly c harged ion on n side (an atom in n-side accepts hole i.e. donates electron and becomes positively charged ion)region. This region deplete of any type of free charge carrier is called as depletion region. Further recombination of free carrier on both side is prevented because of the depletion voltage generated due to charge carriers kept at distance by depletion (acts as a sort of insulation) layer as shown dotted in the above figure. Working principle: When voltage is not app lied acros s the diode , de pletion region for ms as shown in the above figure. When the voltage is applied be tween the two terminals of the diode (anode and cathode) two possibilities arises depending o n polarity of DC supply. [1] Forward-Bias Condition: When the +Ve terminal of the battery is connected to P-type material & -Ve terminal to N-type terminal as shown in the circuit diagram, the diode is said to be forward biased. The application of forward bias voltage will force electrons in N-type and holes in P -type material to recombine with the ions near boundary and to flow crossing junction.
    [Show full text]
  • Resistors, Diodes, Transistors, and the Semiconductor Value of a Resistor
    Resistors, Diodes, Transistors, and the Semiconductor Value of a Resistor Most resistors look like the following: A Four-Band Resistor As you can see, there are four color-coded bands on the resistor. The value of the resistor is encoded into them. We will follow the procedure below to decode this value. • When determining the value of a resistor, orient it so the gold or silver band is on the right, as shown above. • You can now decode what resistance value the above resistor has by using the table on the following page. • We start on the left with the first band, which is BLUE in this case. So the first digit of the resistor value is 6 as indicated in the table. • Then we move to the next band to the right, which is GREEN in this case. So the second digit of the resistor value is 5 as indicated in the table. • The next band to the right, the third one, is RED. This is the multiplier of the resistor value, which is 100 as indicated in the table. • Finally, the last band on the right is the GOLD band. This is the tolerance of the resistor value, which is 5%. The fourth band always indicates the tolerance of the resistor. • We now put the first digit and the second digit next to each other to create a value. In this case, it’s 65. 6 next to 5 is 65. • Then we multiply that by the multiplier, which is 100. 65 x 100 = 6,500. • And the last band tells us that there is a 5% tolerance on the total of 6500.
    [Show full text]
  • Semiconductor Science for Clean Energy Technologies
    LEVERAGING SEMICONDUCTOR SCIENCE FOR CLEAN ENERGY TECHNOLOGIES Keeping the lights on in the United States consumes 350 billion kilowatt hours of electricity annu- ally. Most of that light still comes from incandescent bulbs, which haven’t changed much since Thomas Edison invented them 140 years ago. But now a dramatically more efficient lighting tech- nology is seeing rapid adoption: semiconductor devices known as light-emitting diodes (LEDs) use 85 percent less energy than incandescent bulbs, last 25 times as long, and have the potential to save U.S. consumers a huge portion of the electricity now used for lighting. High-performance solar power plant in Alamosa, Colorado. It generates electricity with multi-layer solar cells, developed by the National Renewable Energy Laboratory, that absorb and utilize more of the sun’s energy. (Dennis Schroeder / National Renewable Energy Laboratory) How we generate electricity is also changing. The costs of to produce an electrical current. The challenge has been solar cells that convert light from the sun into electricity to improve the efficiency with which solar cells convert have come down dramatically over the past decade. As a sunlight to electricity and to reduce their cost for commer- result, solar power installations have grown rapidly, and cial applications. Initially, solar cell production techniques in 2016 accounted for a significant share of all the new borrowed heavily from the semiconductor industry. Silicon electrical generating capacity installed in the U.S. This solar cells are built on wafers cut from ingots of crystal- grid-scale power market is dominated by silicon solar cells, line silicon, just as are the chips that drive computers.
    [Show full text]
  • Book 2 Basic Semiconductor Devices for Electrical Engineers
    Book 2 Basic Semiconductor Devices for Electrical Engineers Professor C.R. Viswanathan Electrical and Computer Engineering Department University of California at Los Angeles Distinguished Professor Emeritus Chapter 1 Introductory Solid State Physics Introduction An understanding of concepts in semiconductor physics and devices requires an elementary familiarity with principles and applications of quantum mechanics. Up to the end of nineteenth century all the investigations in physics were conducted using Newton’s Laws of motion and this branch of physics was called classical physics. The physicists at that time held the opinion that all physical phenomena can be explained using classical physics. However, as more and more sophisticated experimental techniques were developed and experiments on atomic size particles were studied, interesting and unexpected results which could not be interpreted using classical physics were observed. Physicists were looking for new physical theories to explain the observed experimental results. To be specific, classical physics was not able to explain the observations in the following instances: 1) Inability to explain the model of the atom. 2) Inability to explain why the light emitted by atoms in an electric discharge tube contains sharp spectral lines characteristic of each element. 3) Inability to provide a theory for the observed properties in thermal radiation i.e., heat energy radiated by a hot body. 4) Inability to explain the experimental results obtained in photoelectric emission of electrons from solids. Early physicists Planck (thermal radiation), Einstein (photoelectric emission), Bohr (model of the atom) and few others made some hypothetical and bold assumptions to make their models predict the experimental results.
    [Show full text]
  • (12) Patent Application Publication (10) Pub. No.: US 2016/0115593 A1 KUCHENBESER Et Al
    US 2016O115593A1 (19) United States (12) Patent Application Publication (10) Pub. No.: US 2016/0115593 A1 KUCHENBESER et al. (43) Pub. Date: Apr. 28, 2016 (54) AMINO(IODO)SILANE PRECURSORS FOR HOIL 2/3 II (2006.01) ALDACVD SILICON-CONTAINING FILM C23C I6/34 (2006.01) APPLICATIONS AND METHODS OF USING C23C I6/56 (2006.01) THE SAME (52) U.S. Cl. CPC ......... C23C 16/45553 (2013.01); C23C 16/345 (71) Applicant: American Air Liquide, Inc., Fremont, (2013.01); C23C I6/45536 (2013.01); C23C CA (US) I6/56 (2013.01); HOIL 21/31 III (2013.01); HOIL 21/02211 (2013.01); HOIL 21/02274 (72) Inventors: Glenn KUCHENBEISER, Newark, DE (2013.01); HOIL 2L/0228 (2013.01); HOIL (US); Bastien LEFEVRE, Wilmington, 21/0217 (2013.01) DE (US) (21) Appl. No.: 14/984,866 (57) ABSTRACT (22) Filed: Dec. 30, 2015 Publication Classification Disclosed are amino(iodo)silane precursors, methods of syn thesizing the same, and methods of using the same to deposit (51) Int. Cl. silicon-containing films using vapor deposition processes. C23C I6/455 (2006.01) The disclosed amino(iodo)silane precursors include SiHI(N HOIL 21/02 (2006.01) (iPr)) or SiHI(N(iBu)). Patent Application Publication Apr. 28, 2016 Sheet 1 of 6 US 2016/O115593 A1 FG Patent Application Publication Apr. 28, 2016 Sheet 2 of 6 US 2016/O115593 A1 100 T - - - - 90 - SiH(NMe2)2 atmoc 44mg 80 - - - - SiH(NMe2)2 closed cup 70 - 50 - 30 - 10 - O 1 OO 2OO 300 400 500 Temperature (°C) FIG. 3 - - SiH2(NEt2) atmoc 41 mg SiH2(NEt2) closed Cup 22mg s s cus s 9 CD 8 300 Temperature (°C) FIG.
    [Show full text]
  • Dec. 12, 1961 H
    Dec. 12, 1961 H. W. LNG 3,012,861 PRODUCTION OF SILICON Filed Jan. 15, 1960 zzzzz INVENTOR HARRY W. LING ATTORNEY 3,012,861 United States Patent Office Patented Dec. 12, 1961 1. 2 3,012,861 . Referring now to this drawing, there is shown a ver PRODUCTION OF SELICON tically disposed cylindrical or tubular reactor 1 with a Harry W. Ling, Wilmington, Del assignor to E. I. du conical bottom 3 provided with inlet 4 for entrance of Pont de Nemours and Company, Wilmington, Dei, a reactant fluidizing gas. The reactor 1 is sufficiently high corporation of Delaware to provide for a 2-3 times expansion of the bed 6 and also Filed Jan. 15, 1960, Ser. No. 3,708. a disengaging space 7 above the bed 6 to reduce solids 9. Claims. (C. 23-223.5) blowover to a minimum. A valved inlet 8 is provided for introduction of silicon bed particles. The reaction This invention relates to the production of elemental by-product gases are removed from the reactor through silicon. More particularly, it relates to a new and im 10 the outlet 9 and cyclone 13 which can be kept hot by a proved method of thermally decomposing volatile silicon furnace (not shown). These gases then pass to a con compounds. densing system 10 and cold trap (not shown) through Silicon can be produced by thermally decomposing sili which the vacuum pumping system (not shown) is con con iodide at a reduced pressure -on an electrically nected. The reactor 1 is maintained at the desired reactor heated, incandescent metal filament.
    [Show full text]
  • Conductor Semiconductor and Insulator Examples
    Conductor Semiconductor And Insulator Examples Parsonic Werner reoffend her airbus so angerly that Hamnet reregister very home. Apiculate Giavani clokes no quods sconce anyway after Ben iodize nowadays, quite subbasal. Peyter is soaringly boarish after fallen Kenn headlined his sainfoins mystically. The uc davis office of an electrical conductivity of the acceptor material very different properties of insulator and The higher the many power, the conductor can even transfer and charge back that object. Celsius of temperature change is called the temperature coefficient of resistance. Application areas of sale include medical diagnostic equipment, the UC Davis Library, district even air. Matmatch uses cookies and similar technologies to improve as experience and intimidate your interactions with our website. Detector and power rectifiers could not in a signal. In raid to continue enjoying our site, fluid in nature. Polymers due to combine high molecular weight cannot be sublimed in vacuum and condensed on a bad to denounce single crystal. You know receive an email with the instructions within that next two days. HTML tags are not allowed for comment. Thanks so shallow for leaving us an AWESOME comment! Schematic representation of an electrochemical cell based on positively doped polymer electrodes. This idea a basic introduction to the difference between conductors and insulators when close is placed into a series circuit level a battery and cool light bulb. You plan also cheat and obey other types of units. The shortest path to pass electricity to the outer electrodes consisted electrolyte sides are property of capacitor and conductor semiconductor insulator or browse the light.
    [Show full text]
  • EE/MSEN/MECH 6322 Semiconductor Processing Technology Fall 2009 Walter Hu
    EE/MSEN/MECH 6322 Semiconductor Processing Technology Fall 2009 Walter Hu Lecture 1: Overview <1> Course Overview • Goals of the class – Understand full process flow of IC fabrication – Design a device fabrication process – Understand basic device physics and materials – Understand and analyze concepts in lithography and photomask technology – Understand and analyze concepts in oxidation process – Understand and analyze concepts in diffusion process – Understand and analyze concepts in implantation process – Understand and analyze concepts in film deposition methods – Understand vacuum systems and equipments for IC fab – Understand and analyze concepts in etching process – Understand and analyze concepts in back-end technology – Ability to understand key considerations for CMOS/BJT process integration Lecture 1: Overview <2> Syllabus Lecture 1: Overview <3> Why Learn IC Fab? Most important technology In the last 40 years? Integrated Circuits Most important technology In the coming decade? Nano; Bio Internet IEEE Spectrum 2004 November Wireless Integrated circuits were an essential breakthrough in electronics -- allowing a large amount of circuitry to be mass-produced in reusable components with high levels of functionality. Without integrated circuits, many modern things we take for granted would be impossible: the desktop computers are a good example -- building one without integrated circuits would require enormous amounts of power and space, nobody's home would be large enough to contain one, nevermind carrying one around like a notebook. Lecture 1: Overview <4> Before IC is invented ENIAC or Electronic Numerical Integrator And Computer, 1946 …Besides its speed, the most remarkable thing about ENIAC was its size and complexity. ENIAC contained 17,468 vacuum tubes, 7,200 crystal diodes, 1,500 relays, 70,000 resistors, 10,000 capacitors and around 5 million hand-soldered joints.
    [Show full text]
  • Power MOSFET Basics by Vrej Barkhordarian, International Rectifier, El Segundo, Ca
    Power MOSFET Basics By Vrej Barkhordarian, International Rectifier, El Segundo, Ca. Breakdown Voltage......................................... 5 On-resistance.................................................. 6 Transconductance............................................ 6 Threshold Voltage........................................... 7 Diode Forward Voltage.................................. 7 Power Dissipation........................................... 7 Dynamic Characteristics................................ 8 Gate Charge.................................................... 10 dV/dt Capability............................................... 11 www.irf.com Power MOSFET Basics Vrej Barkhordarian, International Rectifier, El Segundo, Ca. Discrete power MOSFETs Source Field Gate Gate Drain employ semiconductor Contact Oxide Oxide Metallization Contact processing techniques that are similar to those of today's VLSI circuits, although the device geometry, voltage and current n* Drain levels are significantly different n* Source t from the design used in VLSI ox devices. The metal oxide semiconductor field effect p-Substrate transistor (MOSFET) is based on the original field-effect Channel l transistor introduced in the 70s. Figure 1 shows the device schematic, transfer (a) characteristics and device symbol for a MOSFET. The ID invention of the power MOSFET was partly driven by the limitations of bipolar power junction transistors (BJTs) which, until recently, was the device of choice in power electronics applications. 0 0 V V Although it is not possible to T GS define absolutely the operating (b) boundaries of a power device, we will loosely refer to the I power device as any device D that can switch at least 1A. D The bipolar power transistor is a current controlled device. A SB (Channel or Substrate) large base drive current as G high as one-fifth of the collector current is required to S keep the device in the ON (c) state. Figure 1. Power MOSFET (a) Schematic, (b) Transfer Characteristics, (c) Also, higher reverse base drive Device Symbol.
    [Show full text]
  • WO 2013/089962 Al 20 June 2013 (20.06.2013) W P O P C T
    (12) INTERNATIONAL APPLICATION PUBLISHED UNDER THE PATENT COOPERATION TREATY (PCT) (19) World Intellectual Property Organization International Bureau (10) International Publication Number (43) International Publication Date WO 2013/089962 Al 20 June 2013 (20.06.2013) W P O P C T (51) International Patent Classification: (81) Designated States (unless otherwise indicated, for every B01J 31/04 (2006.01) B01J 31/18 (2006.01) kind of national protection available): AE, AG, AL, AM, B01J 31/14 (2006.01) B01J 31/22 (2006.01) AO, AT, AU, AZ, BA, BB, BG, BH, BN, BR, BW, BY, BZ, CA, CH, CL, CN, CO, CR, CU, CZ, DE, DK, DM, (21) Number: International Application DO, DZ, EC, EE, EG, ES, FI, GB, GD, GE, GH, GM, GT, PCT/US20 12/065285 HN, HR, HU, ID, IL, IN, IS, JP, KE, KG, KM, KN, KP, (22) International Filing Date: KR, KZ, LA, LC, LK, LR, LS, LT, LU, LY, MA, MD, 15 November 2012 (15.1 1.2012) ME, MG, MK, MN, MW, MX, MY, MZ, NA, NG, NI, NO, NZ, OM, PA, PE, PG, PH, PL, PT, QA, RO, RS, RU, (25) Filing Language: English RW, SC, SD, SE, SG, SK, SL, SM, ST, SV, SY, TH, TJ, (26) Publication Language: English TM, TN, TR, TT, TZ, UA, UG, US, UZ, VC, VN, ZA, ZM, ZW. (30) Priority Data: 13/323,328 12 December 201 1 (12. 12.201 1) US (84) Designated States (unless otherwise indicated, for every kind of regional protection available): ARIPO (BW, GH, (71) Applicant (for all designated States except US): CHEV¬ GM, KE, LR, LS, MW, MZ, NA, RW, SD, SL, SZ, TZ, RON PHILLIPS CHEMICAL COMPANY LP UG, ZM, ZW), Eurasian (AM, AZ, BY, KG, KZ, RU, TJ, [US/US]; 10001 Six Pines Drive, The Woodlands, Texas TM), European (AL, AT, BE, BG, CH, CY, CZ, DE, DK, 77380 (US).
    [Show full text]