西安交通大学:《电力电子变电技术》Bipolar junction transistor - History

Bipolar junction transistor -History Basic operation of BJt E(p-type) B(n-type) c(p-type) (2) X(3) Schematic current flows in pnp BJT 「8 (1)Hole particle current from E to B (2) Electron particle current from b to e (3)Recombination current in B (4)Hole particle current originating in E and reaching C (5Reverse electron particle current from C to B (6)Reverse hole particle current from B to C (What is difference between"current and"particle current?) OE F Schubert, Rensselaer Polytechnic Institute, 2003
© E. F. Schubert, Rensselaer Polytechnic Institute, 2003 1 Bipolar junction transistor - History Basic operation of BJT (1) Hole particle current from E to B (2) Electron particle current from B to E (3) Recombination current in B (4) Hole particle current originating in E and reaching C (5) Reverse electron particle current from C to B (6) Reverse hole particle current from B to C (What is difference between “current” and “particle current”?)

Qualitative basic operation of BJts What is a bjt? A BJT consists of two back-to-back p-n junctions The middle region, the base, is very thin The three regions are the emitter, base, and collector Carriers are injected (emitted) into the base from the emitter Since the base is thin most carriers injected into base diffuse into collector What does a thin base thickness "mean Base thickness is much thinner than the diffusion length of carriers injected from the emitter OE F Schubert, Rensselaer Polytechnic Institute, 2003
© E. F. Schubert, Rensselaer Polytechnic Institute, 2003 2 Qualitative basic operation of BJTs What is a BJT? A BJT consists of two back-to-back p-n junctions. The middle region, the base, is very thin. The three regions are the emitter, base, and collector. Carriers are injected (“emitted”) into the base from the emitter. Since the base is thin, most carriers injected into base diffuse into collector. What does a “thin base thickness” mean? Î Base thickness is much thinner than the diffusion length of carriers injected from the emitter

History of point-contact transistor The first transistor was a point-contact transistor The first point-contact transistor John Bardeen, Walter Brattain, and william Shockley Bell Laboratories, Murray Hill, New Jersey (1947) Spring Emitter Bardeen Brattain Collector Base Shockley OE F Schubert, Rensselaer Polytechnic Institute, 2003
© E. F. Schubert, Rensselaer Polytechnic Institute, 2003 3 History of point-contact transistor The first transistor was a point-contact transistor

Model of transistor in bell labs museum Museum is located at 600 Mountain Ave. Murray Hill, New Jersey OE F Schubert, Rensselaer Polytechnic Institute, 2003
© E. F. Schubert, Rensselaer Polytechnic Institute, 2003 4 Model of transistor in Bell Labs museum Museum is located at 600 Mountain Ave., Murray Hill, New Jersey

History of the first transistor The first transistor was about half an inch high. Before Brattain started John Bardeen told him that they would need two metal contacts within 0.002 inches (0.002 inches 50 um) of each other-about the thickness of a sheet of paper. But the finest wires then were almost three times that width and couldn 't provide the kind of precision they needed. Instead of bothering with tiny wires, Brattain attached a single strip of gold foil over the point of a plastic triangle With a razor blade, he sliced through the gold right at the tip of the triangle. Voila: two gold contacts just a hair width apart The whole triangle was then held over a crystal of germanium on a spring, so that the contacts lightly touched the surface. The germanium itself sat on a metal plate attached to a voltage source. This contraption was the very first semiconductor amplifier, because when a bit of current came through one of the gold contacts, another even stronger current came out the other contact OE F Schubert, Rensselaer Polytechnic Institute, 2003
© E. F. Schubert, Rensselaer Polytechnic Institute, 2003 5 History of the first transistor “The first transistor was about half an inch high. Before Brattain started, John Bardeen told him that they would need two metal contacts within 0.002 inches (0.002 inches = 50 µm) of each other - about the thickness of a sheet of paper. But the finest wires then were almost three times that width and couldn’t provide the kind of precision they needed. Instead of bothering with tiny wires, Brattain attached a single strip of gold foil over the point of a plastic triangle. With a razor blade, he sliced through the gold right at the tip of the triangle. Voila: two gold contacts just a hairwidth apart. The whole triangle was then held over a crystal of germanium on a spring, so that the contacts lightly touched the surface. The germanium itself sat on a metal plate attached to a voltage source. This contraption was the very first semiconductor amplifier, because when a bit of current came through one of the gold contacts, another even stronger current came out the other contact

Here's why it worked Germanium is a semiconductor and, if properly treated, can either let lots of current through or let none through. This germanium had an excess of electrons, but when an electric signal traveled in through the gold foil, it injected holes(the opposite of electrons) into the surface. This created a thin layer along the top of the germanium with too few electrons Semiconductors with too many electrons are known as N-type and semiconductors with too few electrons are known as p-type. The boundary between these two kinds of semiconductors is known as a P-N junction, and it's a crucial part of a transistor. In the presence of this unction current can start to flow from one side to the other In the case of Brattain s transistor, current flowed towards the second gold contact Think about what that means. A small current in through one contact changes the nature of the semiconductor so that a larger, separate current starts flowing across the germanium and out the second contact A little current can alter the flow of a much bigger one, effectively amplifying it. Of course, a transistor in a telephone or in a radio has to handle complex signals. The output contact cant just amplify a steady OE F Schubert, Rensselaer Polytechnic Institute, 2003
© E. F. Schubert, Rensselaer Polytechnic Institute, 2003 6 Here’s why it worked: Germanium is a semiconductor and, if properly treated, can either let lots of current through or let none through. This germanium had an excess of electrons, but when an electric signal traveled in through the gold foil, it injected holes (the opposite of electrons) into the surface. This created a thin layer along the top of the germanium with too few electrons. Semiconductors with too many electrons are known as N-type and semiconductors with too few electrons are known as P-type. The boundary between these two kinds of semiconductors is known as a P-N junction, and it’s a crucial part of a transistor. In the presence of this junction, current can start to flow from one side to the other. In the case of Brattain’s transistor, current flowed towards the second gold contact. Think about what that means. A small current in through one contact changes the nature of the semiconductor so that a larger, separate current starts flowing across the germanium and out the second contact. A little current can alter the flow of a much bigger one, effectively amplifying it. Of course, a transistor in a telephone or in a radio has to handle complex signals. The output contact can’t just amplify a steady

hum of current, it has to dutifully replicate a person s voice, or an entire symphony. Luckily, a semiconductor is perfectly suited to this job. It is exquisitely sensitive to how many extra or missing electrons are inside Each time the input signal shoves more holes into the germanium, it changes the way current flows across the crystal-the output current instantly gets larger and smaller, perfectly mimicking the input (after Public Broadcasting System(PBs)television series, 1999 OE F Schubert, Rensselaer Polytechnic Institute, 2003
© E. F. Schubert, Rensselaer Polytechnic Institute, 2003 7 hum of current, it has to dutifully replicate a person’s voice, or an entire symphony. Luckily, a semiconductor is perfectly suited to this job. It is exquisitely sensitive to how many extra or missing electrons are inside. Each time the input signal shoves more holes into the germanium, it changes the way current flows across the crystal - the output current instantly gets larger and smaller, perfectly mimicking the input.” (after Public Broadcasting System (PBS) television series, 1999)

How did first point-contact transistor work? Schematic of the first point-contact transistor Spring Emitter Spring Emitter Collector edge (insulator)/Go Base co∥ lector Semiconductor (Ge) ■■ Gap between E and C cut ■■■■■■■■ by razor blade OE F Schubert, Rensselaer Polytechnic Institute, 2003
© E. F. Schubert, Rensselaer Polytechnic Institute, 2003 8 How did first point-contact transistor work?

a gold foil was glued to a triangular insulating wedge A narrow gap was cut with a razor blade to form the e and c The gap was approximately 50 um wide Under forward bias of the eB junction, minority carriers are injected into base(n case of point-contact transistor, strong forward bias is required) How are minority carriers injected without a p-n junction? Most minority carriers are collected by the reverse-biased bc junction Thus the base controls the current flow between e and c OE F Schubert, Rensselaer Polytechnic Institute, 2003
© E. F. Schubert, Rensselaer Polytechnic Institute, 2003 9 A gold foil was glued to a triangular insulating wedge. A narrow gap was cut with a razor blade to form the E and C. The gap was approximately 50 µm wide. Under forward bias of the EB junction, minority carriers are injected into base (In case of point-contact transistor, strong forward bias is required). How are minority carriers injected without a p-n junction? Most minority carriers are collected by the reverse-biased BC junction. Thus the base controls the current flow between E and C

How are minority carriers injected without a p-n junction? Answer: Metal Semiconductor Band diagram of Schottky diode under (a)equilibrium conditions, (b)forward bias, and (c)strong forward bias Under strong forward bias, minority carrier injection occurs strong forward-bias is needed for minority carrier injection Can Schottky contacts emit light? If yes, under which circumstances? Are there other circumstances under which Schottky contacts emit light? OE F Schubert, Rensselaer Polytechnic Institute, 2003
© E. F. Schubert, Rensselaer Polytechnic Institute, 2003 10 How are minority carriers injected without a p-n junction? Answer: … strong forward-bias is needed for minority carrier injection. Can Schottky contacts emit light? If yes, under which circumstances? Are there other circumstances under which Schottky contacts emit light?
按次数下载不扣除下载券;
注册用户24小时内重复下载只扣除一次;
顺序:VIP每日次数-->可用次数-->下载券;
- 西安交通大学:《电力电子变电技术》TOSHIBA Bipolar Linear Integrated Circuit Silicon Monolithic.pdf
- 西安交通大学:《电力电子变电技术》IGCT1.pdf
- 西安交通大学:《电力电子变电技术》IGCT.pdf
- 西安交通大学:《电力电子变电技术》Power MOSFET Basics.pdf
- 西安交通大学:《电力电子变电技术》IGBT (Discrete).pdf
- 西安交通大学:《电力电子变电技术》IGBT-INTRO.pdf
- 西安交通大学:《电力电子变电技术》5SGA30j2501.pdf
- 西安交通大学:《电力电子变电技术》schottky power rectifier.pdf
- 西安交通大学:《电力电子变电技术》power diodes.pdf
- 西安交通大学:《电力电子变电技术》high power diode laser.pdf
- 西安交通大学:《电力电子变电技术》high power diode driver for pulsed laser diode.pdf
- 西安交通大学:《电力电子变电技术》fast recovery diode module.pdf
- 西安交通大学:《电力电子变电技术》fast recovery diode 5SDF05D2505.pdf
- 西安交通大学:《电力电子变电技术》fast rcovery diode.pdf
- 西安交通大学:《电力电子变电技术》Rectifier Diode.pdf
- 西安交通大学:《电力电子变电技术》Diodes Rectifier diode 1SR154400/1sR154600.pdf
- 西安交通大学:《电力电子变电技术》使用说明书.doc
- 职业学校课程《接触器自锁正转控制》PPT教学设计(郭医军).ppt
- 南京理工大学自动化学院系:《电力系统分析》电子书(共六章).ppt
- 南京理工大学自动化学院系:《电力系统分析》课程简介.ppt
- 西安交通大学:《电力电子变电技术》The Bipolar Junction Transistor.pdf
- 西安交通大学:《电力电子变电技术》Bi-Directional Control Thyristor.pdf
- 西安交通大学:《电力电子变电技术》DCR1473SY/DCR1473SV.pdf
- 西安交通大学:《电力电子变电技术》fast switching thyristor.pdf
- 西安交通大学:《电力电子变电技术》TECHNICAL REPORTS.pdf
- 西安交通大学:《电力电子变电技术》Phase Control Thyristor.pdf
- 西安交通大学:《电力电子变电技术》SCR-DNX_MP02XXX190.pdf
- 西安交通大学:《电力电子变电技术》MP02XXX190 Series.pdf
- 西安交通大学:《电力电子变电技术》课程教学资源(PPT课件)第一章 电力电子器件概述.pps
- 西安交通大学:《电力电子变电技术》课程教学资源(PPT课件)第二章 整流电路.pps
- 西安交通大学:《电力电子变电技术》课程教学资源(PPT课件)第三章 直流斩波电路.pps
- 西安交通大学:《电力电子变电技术》课程教学资源(PPT课件)第四章 交流电力控制电路和交变频电路.pps
- 西安交通大学:《电力电子变电技术》课程教学资源(PPT课件)第五章 逆变电路.pps
- 西安交通大学:《电力电子变电技术》课程教学资源(PPT课件)第六章 脉宽调(PWM)技术.pps
- 西安交通大学:《电力电子变电技术》课程教学资源(PPT课件)第七章 软开关技术.pps
- 西安交通大学:《电力电子变电技术》课程教学资源(PPT课件)第八章 组合变流电路.pps
- 西安交通大学:《电力电子变电技术》课程教学资源(PPT课件)绪论.pps
- 西安交通大学:《电力电子变电技术》课程教学资源(PPT课件)课程总目录.pps
- 《电工学》答案 第1章 电路的基本概念与定律.pdf
- 《电工学》答案 第10章 继电接触器控制系统.pdf