Semiconductor Devices II Physics 355. Zener Diodes With the application of sufficient reverse voltage, a p-n junction will experience a rapid avalanche.

Slides:



Advertisements
Similar presentations
Semiconductors Chapters
Advertisements

Introduction to Semiconductor Devices
Solid state devices Crystal diodes – a crystal and a bronze wire Semiconductors – made from poor conductors with conductive impurities – Poor conductors.
Electronic Devices Ninth Edition Floyd Chapter 11.
PHY 201 (Blum) Transistors and Logic Gates References:
Instructor Name: (Your Name)
TRANSISTOR. TRANSISTOR Background and Introduction A semiconductor device that Amplifies, Oscillates, or Switches the flow of current between two terminals.
Semiconductor basics 1. Vacuum tubes  Diode  Triode 2. Semiconductors  Diode  Transistors Bipolar Bipolar Field Effect Field Effect 3. What’s next?
Introduction to Electronics
Physics I Honors Electronics.
AMPLIFIERS, DIODES,RECTIFIERS,WAVESHAPPING CIRCUITS
1 SEMICONDUCTORS Tunnel an Varactor Diodes. 2 SEMICONDUCTORS PN diodes and zener diodes have lightly doped PN junctions and similar V-I characteristics.
Diodes, Transistors and Tubes
10/4/2004EE 42 fall 2004 lecture 151 Lecture #15 Basic amplifiers, Intro to Bipolar transistors Reading: transistors (chapter 6 and 14)
1 SEMICONDUCTOR Diodes PN junction and diode biasing Diodes PN junction and diode biasing.
Unit 7, Chapter 24 CPO Science Foundations of Physics.
Transistors Student Lecture by: Giangiacomo Groppi Joel Cassell
10/6/2004EE 42 fall 2004 lecture 161 Lecture #16 Bipolar transistors Reading: transistors Bipolar: chapter 6 MOS: chapter 14.
ME 4447 / 6405 Student Lecture “Transistors”
Transistors Electronics 1 CVSD.
NAME OF FACULTY : MR. Harekrishna Avaiya DEPARTMENT: E.C. (PPI-1ST)
Chapter 22 Bipolar Transistors. 2 Objectives –After completing this chapter, the student should be able to: Describe how a transistor is constructed and.
Transistors  The Transistor was invented in 1948 and  The New York Herald Tribune announced the invention of the transistor as the … “Electronic device.
Intro to Mechatronics 18 February 2005 Student Lecture: Transistors
General Licensing Class Oscillators & Components Your organization and dates here.
Basic Circuit Components
SEMICONDUCTOR DEVICES. Diodes as a semiconductor devices Symbol and Structure Diodes is made by joining p-types and n- types semiconductor materials.
Introduction To Semiconductors
Junctions and Semiconductors Theories and practical devices.
Information Technology
Avalanche Transit Time Devices
Electronics Electronics is the science and technology of electronic phenomena. It is a branch of physics that deals with the emission, behaviour, and.
Intro to Semiconductor devices & Diodes Electronics 1 CVHS.
Ashraful Haider Chowdhury
Semiconductor Devices and Microelectronics A subtopic of Basic Electronics.
Transistors and Semiconductors Miracle Makers of Modern Electronics Graphics courtesy intel.com Research at ience/index.html.
AMATEUR RADIO OPERATOR INTRODUCTION January 2013 Active Devices Diodes, Transistors, and Tubes.
Semiconductors. O A Semiconductor is a material whose resistivity is between that of a good conductor and a good insulator. O Examples of materials which.
Chapter 3 Bipolar Junction Transistor (BJT)
Basic Circuit Components Name: gohel khushbu dilipbhai. Enrollment no: Subject : Basic electronics Branch : Co(Shift -1)
1 Concepts of electrons and holes in semiconductors.
Introduction Semiconductors are materials whose electrical properties lie between Conductors and Insulators. Ex : Silicon and Germanium.
CSE251 Lecture 8: Introduction to Bipolar Junction Transistor (BJT)
COURSE NAME: SEMICONDUCTORS Course Code: PHYS 473 Week No. 5.
Transistors According to Dictionary.com a transistor is:
PREPARED BY, SHAIKH SALEHA A VAHORA SHALEHA Y
INTRODUCTION TO SEMICONDUCTORS
Transistors Different types and sizes BJT (PNP) Electrical Diagram First Transistor Modern Electronics FET and BJT Transistor.
CSE251 Lecture 8: Introduction to Bipolar Junction Transistor (BJT)
Bipolar Junction Transistors Working Principle and Applications.
NAME: NITHIN GEORGE PALLIPATT E.N BRANCH-EC(3rd) SUBJECT- ELECTRONICS DEVICE AND CIRCUIT PROJECT TITLE- DIFFERENT TYPES OF DIODES DARSHAN.
1 Lawndale High School AWIM Program Transistor Theory & Experiment Lecture 5.
Transistors Student Lecture by: Giangiacomo Groppi Joel Cassell
PN JUNCTION Sri. S. L. Kulkarni Associate Professor & Head
Basic Circuit Components
SIGMA INSTITUTE OF ENGINEERING AT: BAKROL AJWA NIMETA ROAD VADODARA,
Government Engineering College, Bhavnagar.
5.4 Reverse-Bias Breakdown
PRESENTATION OF ELECTRONICS-I
Transistors and Logic Gates
“Transistors”.
Bipolar Junction Transistors (BJT)
BASIC ELECTRONICS.
Chapter 3. PN Junctions and Related Devices
Department of Electronics
BIPOLAR JUNCTION TRANSISTOR (BJT)
Transistors Magic of Electrons © 2011 Project Lead The Way, Inc.
Bipolar Junction Transistors Md. Rabiul Islam Dept. of Biomedical Engineering 8/3/
Presentation On Schottky Diode. Course Code:3208 Course Title : Microwave radar and satellite communication lab Presented By Salma Akter BKH F.
Presentation transcript:

Semiconductor Devices II Physics 355

Zener Diodes With the application of sufficient reverse voltage, a p-n junction will experience a rapid avalanche breakdown and conduct current in the reverse direction. Valence electrons that break free under the influence of the applied electric field can be accelerated enough that they can knock loose other electrons and the subsequent collisions quickly become an avalanche. When this process is taking place, very small changes in voltage can cause very large changes in current. The breakdown process depends upon the applied electric field, so by changing the thickness of the layer to which the voltage is applied, zener diodes can be formed which break down at voltages from about 4 volts to several hundred volts.

Zener Diodes When forward-biased, Zener diodes behave much the same as standard rectifying diodes: they have a forward voltage drop which follows the "diode equation" and is about 0.7 volts. In reverse-bias mode, they do not conduct until the applied voltage reaches or exceeds the so-called Zener voltage, at which point the diode is able to conduct substantial current, and in doing so will try to limit the voltage dropped across it to that Zener voltage point. So long as the power dissipated by this reverse current does not exceed the diode's thermal limits, the diode will not be harmed.

Tunnel Diodes

NDC region

Tunnel Diodes: Applications In the NDC region, the diode can be used as either an oscillator, as in the case of the Gunn diode, or as an amplifier. Low-noise, tunnel-diode amplifiers represent an important microwave application of tunnel diodes. Tunnel-diode amplifiers with frequencies up to 85 gigahertz have been built in waveguides, coaxial lines, and transmission lines. The low-noise generation, gain ratios of up to 30 dB, high reliability, and light weight make these amplifiers ideal for use as the first stage of amplification in communications and radar receivers.

Transistors Dr. John Bardeen, Dr. Walter Brattain, and Dr. William Shockley discovered the transistor effect and developed the first device in December, 1947, while the three were members of the technical staff at Bell Laboratories in Murray Hill, NJ. They were awarded the Nobel Prize in physics in 1956.

Transistors Transistors are the main components of microprocessors, which are essential to many of the products we use every day such as televisions, cars, radios, home appliances, and, of course, computers. Transistors are miniature electronic switches. They are the building blocks of the microprocessor which is the brain of the computer. At their most basic level, transistors may seem simple. But their development actually required many years of painstaking research. Before transistors, computers relied on slow, inefficient vacuum tubes and mechanical switches to process information. In 1958, engineers (one of them Intel co-founder Robert Noyce) managed to put two transistors onto a silicon crystal and create the first integrated circuit, which led to the microprocessor.

Transistors The bipolar junction transistor acts as a current amplifier, having many applications for amplification and switching.

Unbiased Transistors

Transistors

When a negative voltage is applied to the base (point B), electrons in the base region are pushed ('like' charges repel, in this case both negative) back creating insulation boundaries. The current flow from point E to point C stops. The transistor's state has been changed from a conductor to an insulator.

Transistors We begin with the transistor acting as an insulator. In order to have it conduct, positive voltage must be applied to the base (point B). As opposite charges attract (in this case, positive and negative), electrons are 'pulled' out of the insulating boundaries and flow out of the base region at point B. The barriers that once restricted flow of electrons from the emitter to the collector are diminished. Electrons begin to flow in at the emitter (point E), through the base to the collector (point C). The transistor's state has been changed from an insulator to a conductor.

Transistors: Amplifier Apply different values of the base bias voltage and the collector bias voltage to the npn transistor and see what happens. With two ammeters (shown as red dots) and a voltmeter to measure V CE we can determine the characteristics of the transistor.

Transistors: Amplifier The amount of base current is determined by the base bias voltage.