CARLETON UNIVERSITY. FINAL EXAMINATION December 2016

Size: px
Start display at page:

Download "CARLETON UNIVERSITY. FINAL EXAMINATION December 2016"

Transcription

1 CARLETON UNIVERSITY FINAL EXAMINATION December 2016 DURATION: 3 HOURS Department Name & Course Number: Electronics 4705 Course Instructor(s): Tom Smy AUTHORIZED MEMORANDA CALCULATOR (Not Programmable) Students MUST count the number of pages in this examination question paper before beginning to write, and report any discrepancy immediately to a proctor. This question paper has 15 pages. This examination question paper MAY NOT be taken from the examination room. There are 11 questions on the exam. Attempt all questions. Note that the questions are not equally weighted. I suggest you attempt the questions you know best first! There are 178 marks. I think :-) Student Name: Student Number: 1

2 1. Basic Quantum Mechanics (15 Marks total): Sketch a finite electron potential well showing the important features. (2 Marks) (a) (7 Marks) With reference to the sketch write down: i. The time independent Schrodinger s Eq. with the appropriate potential. ii. The appropriate boundary conditions. iii. Describe when quantization of electron energy occurs. (b) (3 marks) Sketch ψ(x) for the first few energy states. (c) (3 Marks) Sketch ψ(x) for the first few energy states greater then the finite potential well height. 2

3 2. Quantum Mechanical Tunneling (10 Marks) Describe what Quantum Mechanical Tunneling is. In particular: (a) Contrast it with the classical situation. (b) Sketch a wave-function for a case of tunneling. (c) What effects the degree of tunneling present? (d) Give an example of a situation when tunneling is important. 3

4 3. Electrons in crystals (Total Marks 20): When describing the electron behaviour in materials we use an E versus k relationship (E(k)). (a) (2 marks) Describe what this relationship is. Specifically what are E and k. (b) (2 marks) What is the E(k) relationship for an electron in a single infinite well? (c) (2 marks) What is the E(k) relationship for perfectly free electrons? (d) (4 marks) Draw an E(k) relationship for free but periodic electrons? How does it differ from the perfectly free electron case? (e) (2 marks) Draw a characteristic E(k) relationship for electrons in a periodic potential with a barrier present. (f) (4 marks) For this case how does the barrier height/width effect the relationship? (g) (4 marks) When we have an electric field present what information about the electron behavior does the E(k) relationship give us? 4

5 (Electrons in crystals Extra page for work.) 5

6 4. Band Structures (Total 25 Marks): (a) (10 Marks) For a crystal of finite size: i. How does the finite size of the crystal effect the potential used in Schrodinger s Eq? ii. How does this change in the potential effect the band structure (E vs k)? iii. Why can bands only accept a finite number of electrons and therefore fill up? iv. If we had small periodic molecule of 20 atoms how many states would you expect to be present in each band? 6

7 Band Structures:(cont.) (b) (5 Marks) What does the band structure of a metal, intrinsic semiconductor, and insulator look like. Draw band structures for each material. (c) (5 marks) Describe in words and with respect to a semiconductor band structure: The Density of States of function The Fermi-Dirac function (d) (5 marks) Describe how the two functions are used to obtain the electron density in a semiconductor. A sketch would be good. 7

8 5. Integrated Circuit Fabrication (Total Marks: 15) (a) (5 Marks) Describe the process of photolithography used in IC fabrication (b) (10 Marks) Describe the steps needed to create a fabricated structure containing: An n region in a p doped wafer A single layer of insulator with a contact cut to the n region An etched metal contact/line to the n region 8

9 6. Schottky Diode: (Total Marks: 12) (a) (2 Marks) Draw the physical structure of a Schottky Diode for an n-type semiconductor. (b) (4 Marks) Draw the band structure at equilibrium and under reverse bias. (c) (6 Marks) Explain the operation of the device in terms of the physical currents flowing in both directions. 9

10 7. Bipolar Junction Transistor: (Total Marks: 10) (a) (7 Marks) Explain why for an NPN bipolar transistor the collector current is given by I c = I c0 eqvbe/kt in forward active operation (base-emitter fwd biased/base-collector reverse biased). Specifically why is it exponentially related to V BE and there is no dependence on V BC? (b) (3 Marks) Can we create an NPN bipolar transistor by connecting two PN diodes backto-back with a metal wire? Why or why not? 10

11 8. Optical Fiber (Total Marks: 10) (a) (2 Marks) If we consider a fiber to be a simple optical structure what fundamental effect do we take advantage of to guide the light? (b) (6 Marks) If we look at the fiber as an electromagnetic problem we find from the solution that modes are present. What are modes and what causes them to exist in this case? (c) (2 Marks) We usually want a fiber to operate using a single mode why? 11

12 9. Optical Devices: (Total Marks: 12) (a) (6 marks) What are the three basic electron transitions that occur in a semi-conductor which involve photons? Describe the transitions. (Use pictures!) (b) (2 marks) If we wish to create an optical amplifier using optical fiber how do we need to modify/alter the fiber? (c) (4 Marks) Would it be possible to make a fiber laser using an optical fiber. How? Can you see any advantages/disadvantages of such a device? 12

13 10. PN Diode Lasers/Detectors (25 Marks). PN diodes can be used for photonic (optical) purposes. (a) (10 Marks) If you wished to design a laser using a pn diode how would you modify the simple structure? Clearly give reasons for each modification and explain it s role in the laser operation. (b) (5 Marks) What would be the two types of electromagnetic modes present in the laser? (c) (5 Marks) What two factors would determine the frequency of operation of the laser? 13

14 PN Diodes. (Cont) (d) (5 Marks) If you wished to design a photodiode using a pn diode how would you modify the structure? Again give reasons for each modification and explain it s role in the detector operation. 14

15 11. MEMS and Nanotechnology: (Total Marks: 24) (a) (2 marks) How would you define the difference between MEMS and nanotechnology? (b) (4 marks) In MEMS process technology describe the role of sacrificial layers. (c) (4 marks) What is a carbon nanotube? Does it have a band structure and why or why not? (d) (6 marks) What is a quantum dot? How big would it be? (e) (6 marks) Propose an application of quantum dots. Explain how the quantum nature of the dot is used. 15

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

Semiconductor Devices and Circuits Fall Midterm Exam. Instructor: Dr. Dietmar Knipp, Professor of Electrical Engineering. Name: Mat. -Nr.

Semiconductor Devices and Circuits Fall Midterm Exam. Instructor: Dr. Dietmar Knipp, Professor of Electrical Engineering. Name: Mat. -Nr. Semiconductor Devices and Circuits Fall 2003 Midterm Exam Instructor: Dr. Dietmar Knipp, Professor of Electrical Engineering Name: Mat. -Nr.: Guidelines: Duration of the Midterm: 1 hour The exam is a closed

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

Solid State Device Fundamentals

Solid State Device Fundamentals Solid State Device Fundamentals ENS 345 Lecture Course by Alexander M. Zaitsev alexander.zaitsev@csi.cuny.edu Tel: 718 982 2812 Office 4N101b 1 Outline - Goals of the course. What is electronic device?

More information

CME 300 Properties of Materials. ANSWERS: Homework 9 November 26, As atoms approach each other in the solid state the quantized energy states:

CME 300 Properties of Materials. ANSWERS: Homework 9 November 26, As atoms approach each other in the solid state the quantized energy states: CME 300 Properties of Materials ANSWERS: Homework 9 November 26, 2011 As atoms approach each other in the solid state the quantized energy states: are split. This splitting is associated with the wave

More information

ECE 305 Exam 2: Spring 2017 March 10, 2017 Muhammad Alam Purdue University

ECE 305 Exam 2: Spring 2017 March 10, 2017 Muhammad Alam Purdue University NAME: PUID: : ECE 305 Exam 2: Spring 2017 March 10, 2017 Muhammad Alam Purdue University This is a closed book exam You may use a calculator and the formula sheet Following the ECE policy, the calculator

More information

Solid State Device Fundamentals

Solid State Device Fundamentals Solid State Device Fundamentals ENS 345 Lecture Course by Alexander M. Zaitsev alexander.zaitsev@csi.cuny.edu Tel: 718 982 2812 Office 4N101b 1 Outline - Goals of the course. What is electronic device?

More information

Semiconductor Theory and Devices

Semiconductor Theory and Devices Semiconductor Theory and Devices Band Theory of Solids Semiconductor Theory Semiconductor Devices Nanotechnology It is evident that many years of research by a great many people, both before and after

More information

Conductivity and Semi-Conductors

Conductivity and Semi-Conductors Conductivity and Semi-Conductors J = current density = I/A E = Electric field intensity = V/l where l is the distance between two points Metals: Semiconductors: Many Polymers and Glasses 1 Electrical Conduction

More information

Semi-Conductor & Diodes

Semi-Conductor & Diodes Semi-Conductor & Diodes Semi-Conductor Some Quantum mechanics refresher Band theory in solids: Semiconductor, insulator and conductor Doping Diode p-n junction Diode types applications Introduction In

More information

Semiconductor Physics fall 2012 problems

Semiconductor Physics fall 2012 problems Semiconductor Physics fall 2012 problems 1. An n-type sample of silicon has a uniform density N D = 10 16 atoms cm -3 of arsenic, and a p-type silicon sample has N A = 10 15 atoms cm -3 of boron. For each

More information

CHAPTER 11 Semiconductor Theory and Devices

CHAPTER 11 Semiconductor Theory and Devices CHAPTER 11 Semiconductor Theory and Devices 11.1 Band Theory of Solids 11.2 Semiconductor Theory 11.3 Semiconductor Devices 11.4 Nanotechnology It is evident that many years of research by a great many

More information

Semiconductor Physics Problems 2015

Semiconductor Physics Problems 2015 Semiconductor Physics Problems 2015 Page and figure numbers refer to Semiconductor Devices Physics and Technology, 3rd edition, by SM Sze and M-K Lee 1. The purest semiconductor crystals it is possible

More information

UNIVERSITY OF CALIFORNIA, BERKELEY College of Engineering Department of Electrical Engineering and Computer Sciences

UNIVERSITY OF CALIFORNIA, BERKELEY College of Engineering Department of Electrical Engineering and Computer Sciences UNIVERSITY OF CALIFORNIA, BERKELEY College of Engineering Department of Electrical Engineering and Computer Sciences EE 105: Microelectronic Devices and Circuits Spring 2008 MIDTERM EXAMINATION #1 Time

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

B12: Semiconductor Devices

B12: Semiconductor Devices B12: Semiconductor Devices Example Sheet 2: Solutions Question 1 To get from eq. (5.70) of the notes to the expression given in the examples sheet, we simply invoke the relations n 0 p 0, n 0 n 0. In this

More information

Most matter is electrically neutral; its atoms and molecules have the same number of electrons as protons.

Most matter is electrically neutral; its atoms and molecules have the same number of electrons as protons. Magnetism Electricity Magnetism Magnetic fields are produced by the intrinsic magnetic moments of elementary particles associated with a fundamental quantum property, their spin. -> permanent magnets Magnetic

More information

Introduction to Transistors. Semiconductors Diodes Transistors

Introduction to Transistors. Semiconductors Diodes Transistors Introduction to Transistors Semiconductors Diodes Transistors 1 Semiconductors Typical semiconductors, like silicon and germanium, have four valence electrons which form atomic bonds with neighboring atoms

More information

CARLETON UNIVERSITY. FINAL EXAMINATION December DURATION 3 HOURS No. of Students 130

CARLETON UNIVERSITY. FINAL EXAMINATION December DURATION 3 HOURS No. of Students 130 ALETON UNIVESITY FINAL EXAMINATION December 005 DUATION 3 HOUS No. of Students 130 Department Name & ourse Number: Electronics ELE 3509 ourse Instructor(s): Prof. John W. M. ogers and alvin Plett AUTHOIZED

More information

ECE 305 Exam 3: Spring 2015 March 6, 2015 Mark Lundstrom Purdue University

ECE 305 Exam 3: Spring 2015 March 6, 2015 Mark Lundstrom Purdue University NAME: PUID: : ECE 305 Exam 3: March 6, 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 ECE policy,

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

Semiconductor Physics and Devices

Semiconductor Physics and Devices The pn Junction 1) Charge carriers crossing the junction. 3) Barrier potential Semiconductor Physics and Devices Chapter 8. The pn Junction Diode 2) Formation of positive and negative ions. 4) Formation

More information

Effective masses in semiconductors

Effective masses in semiconductors Effective masses in semiconductors The effective mass is defined as: In a solid, the electron (hole) effective mass represents how electrons move in an applied field. The effective mass reflects the inverse

More information

n N D n p = n i p N A

n N D n p = n i p N A Summary of electron and hole concentration in semiconductors Intrinsic semiconductor: E G n kt i = pi = N e 2 0 Donor-doped semiconductor: n N D where N D is the concentration of donor impurity Acceptor-doped

More information

Micro-Syllabus of CSIT Physics

Micro-Syllabus of CSIT Physics Micro-Syllabus of CSIT Physics Garcia Narciso, Damask Arthur, Physics for Computer Science Students, Springer-Verlag Reference Books: (B): Heliday David, Resnick Robert and Walker Gearl, Fundamentals of

More information

ELECTRONIC DEVICES AND CIRCUITS SUMMARY

ELECTRONIC DEVICES AND CIRCUITS SUMMARY ELECTRONIC DEVICES AND CIRCUITS SUMMARY Classification of Materials: Insulator: An insulator is a material that offers a very low level (or negligible) of conductivity when voltage is applied. Eg: Paper,

More information

UNIT I: Electronic Materials.

UNIT I: Electronic Materials. SIDDHARTH INSTITUTE OF ENGINEERING & TECHNOLOGY :: PUTTUR Siddharth Nagar, Narayanavanam Road 517583 QUESTION BANK (DESCRIPTIVE) Subject with Code: SEMICONDUCTOR PHYSICS (18HS0851) Course & Branch: B.Tech

More information

EECS130 Integrated Circuit Devices

EECS130 Integrated Circuit Devices EECS130 Integrated Circuit Devices Professor Ali Javey 10/02/2007 MS Junctions, Lecture 2 MOS Cap, Lecture 1 Reading: finish chapter14, start chapter16 Announcements Professor Javey will hold his OH at

More information

Molecules and Condensed Matter

Molecules and Condensed Matter Chapter 42 Molecules and Condensed Matter PowerPoint Lectures for University Physics, Thirteenth Edition Hugh D. Young and Roger A. Freedman Lectures by Wayne Anderson Goals for Chapter 42 To understand

More information

Session 0: Review of Solid State Devices. From Atom to Transistor

Session 0: Review of Solid State Devices. From Atom to Transistor Session 0: Review of Solid State Devices From Atom to Transistor 1 Objective To Understand: how Diodes, and Transistors operate! p n p+ n p- n+ n+ p 2 21 Century Alchemy! Ohm s law resistivity Resistivity

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

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

Modern Physics for Scientists and Engineers International Edition, 4th Edition

Modern Physics for Scientists and Engineers International Edition, 4th Edition Modern Physics for Scientists and Engineers International Edition, 4th Edition http://optics.hanyang.ac.kr/~shsong 1. THE BIRTH OF MODERN PHYSICS 2. SPECIAL THEORY OF RELATIVITY 3. THE EXPERIMENTAL BASIS

More information

CLASS 12th. Semiconductors

CLASS 12th. Semiconductors CLASS 12th Semiconductors 01. Distinction Between Metals, Insulators and Semi-Conductors Metals are good conductors of electricity, insulators do not conduct electricity, while the semiconductors have

More information

Lecture 18: Semiconductors - continued (Kittel Ch. 8)

Lecture 18: Semiconductors - continued (Kittel Ch. 8) Lecture 18: Semiconductors - continued (Kittel Ch. 8) + a - Donors and acceptors J U,e e J q,e Transport of charge and energy h E J q,e J U,h Physics 460 F 2006 Lect 18 1 Outline More on concentrations

More information

3. Two-dimensional systems

3. Two-dimensional systems 3. Two-dimensional systems Image from IBM-Almaden 1 Introduction Type I: natural layered structures, e.g., graphite (with C nanostructures) Type II: artificial structures, heterojunctions Great technological

More information

Electronic Circuits 1. Transistor Devices. Contents BJT and FET Characteristics Operations. Prof. C.K. Tse: Transistor devices

Electronic Circuits 1. Transistor Devices. Contents BJT and FET Characteristics Operations. Prof. C.K. Tse: Transistor devices Electronic Circuits 1 Transistor Devices Contents BJT and FET Characteristics Operations 1 What is a transistor? Three-terminal device whose voltage-current relationship is controlled by a third voltage

More information

Semiconductor Physical Electronics

Semiconductor Physical Electronics Semiconductor Physical Electronics Sheng S. Li Department of Electrical Engineering University of Florida Gainesville, Florida Plenum Press New York and London Contents CHAPTER 1. Classification of Solids

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

3. Consider a semiconductor. The concentration of electrons, n, in the conduction band is given by

3. Consider a semiconductor. The concentration of electrons, n, in the conduction band is given by Colloqium problems to chapter 13 1. What is meant by an intrinsic semiconductor? n = p All the electrons are originating from thermal excitation from the valence band for an intrinsic semiconductor. Then

More information

6.012 Electronic Devices and Circuits

6.012 Electronic Devices and Circuits Page 1 of 1 YOUR NAME Department of Electrical Engineering and Computer Science Massachusetts Institute of Technology 6.12 Electronic Devices and Circuits Exam No. 1 Wednesday, October 7, 29 7:3 to 9:3

More information

16EC401 BASIC ELECTRONIC DEVICES UNIT I PN JUNCTION DIODE. Energy Band Diagram of Conductor, Insulator and Semiconductor:

16EC401 BASIC ELECTRONIC DEVICES UNIT I PN JUNCTION DIODE. Energy Band Diagram of Conductor, Insulator and Semiconductor: 16EC401 BASIC ELECTRONIC DEVICES UNIT I PN JUNCTION DIODE Energy bands in Intrinsic and Extrinsic silicon: Energy Band Diagram of Conductor, Insulator and Semiconductor: 1 2 Carrier transport: Any motion

More information

Semiconductors and Optoelectronics. Today Semiconductors Acoustics. Tomorrow Come to CH325 Exercises Tours

Semiconductors and Optoelectronics. Today Semiconductors Acoustics. Tomorrow Come to CH325 Exercises Tours Semiconductors and Optoelectronics Advanced Physics Lab, PHYS 3600 Don Heiman, Northeastern University, 2017 Today Semiconductors Acoustics Tomorrow Come to CH325 Exercises Tours Semiconductors and Optoelectronics

More information

Sheng S. Li. Semiconductor Physical Electronics. Second Edition. With 230 Figures. 4) Springer

Sheng S. Li. Semiconductor Physical Electronics. Second Edition. With 230 Figures. 4) Springer Sheng S. Li Semiconductor Physical Electronics Second Edition With 230 Figures 4) Springer Contents Preface 1. Classification of Solids and Crystal Structure 1 1.1 Introduction 1 1.2 The Bravais Lattice

More information

Engineering 2000 Chapter 8 Semiconductors. ENG2000: R.I. Hornsey Semi: 1

Engineering 2000 Chapter 8 Semiconductors. ENG2000: R.I. Hornsey Semi: 1 Engineering 2000 Chapter 8 Semiconductors ENG2000: R.I. Hornsey Semi: 1 Overview We need to know the electrical properties of Si To do this, we must also draw on some of the physical properties and we

More information

EE301 Electronics I , Fall

EE301 Electronics I , Fall EE301 Electronics I 2018-2019, Fall 1. Introduction to Microelectronics (1 Week/3 Hrs.) Introduction, Historical Background, Basic Consepts 2. Rewiev of Semiconductors (1 Week/3 Hrs.) Semiconductor materials

More information

KATIHAL FİZİĞİ MNT-510

KATIHAL FİZİĞİ MNT-510 KATIHAL FİZİĞİ MNT-510 YARIİLETKENLER Kaynaklar: Katıhal Fiziği, Prof. Dr. Mustafa Dikici, Seçkin Yayıncılık Katıhal Fiziği, Şakir Aydoğan, Nobel Yayıncılık, Physics for Computer Science Students: With

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 35 - Bipolar Junction Transistor (cont.) November 27, Current-voltage characteristics of ideal BJT (cont.)

Lecture 35 - Bipolar Junction Transistor (cont.) November 27, Current-voltage characteristics of ideal BJT (cont.) 6.720J/3.43J - Integrated Microelectronic Devices - Fall 2002 Lecture 35-1 Lecture 35 - Bipolar Junction Transistor (cont.) November 27, 2002 Contents: 1. Current-voltage characteristics of ideal BJT (cont.)

More information

Nanomaterials and their Optical Applications

Nanomaterials and their Optical Applications Nanomaterials and their Optical Applications Winter Semester 2013 Lecture 02 rachel.grange@uni-jena.de http://www.iap.uni-jena.de/multiphoton Lecture 2: outline 2 Introduction to Nanophotonics Theoretical

More information

EE 3329 Electronic Devices Syllabus ( Extended Play )

EE 3329 Electronic Devices Syllabus ( Extended Play ) EE 3329 - Electronic Devices Syllabus EE 3329 Electronic Devices Syllabus ( Extended Play ) The University of Texas at El Paso The following concepts can be part of the syllabus for the Electronic Devices

More information

VALLIAMMAI ENGINEERING COLLEGE

VALLIAMMAI ENGINEERING COLLEGE VALLIAMMAI ENGINEERING COLLEGE SRM Nagar, Kattankulathur 603 203 DEPARTMENT OF PHYSICS QUESTION BANK II SEMESTER PH8252 - PHYSICS FOR INFORMATION SCIENCE (Common to CSE & IT) Regulation 2017 Academic Year

More information

Lecture 20: Semiconductor Structures Kittel Ch 17, p , extra material in the class notes

Lecture 20: Semiconductor Structures Kittel Ch 17, p , extra material in the class notes Lecture 20: Semiconductor Structures Kittel Ch 17, p 494-503, 507-511 + extra material in the class notes MOS Structure Layer Structure metal Oxide insulator Semiconductor Semiconductor Large-gap Semiconductor

More information

The pn junction. [Fonstad, Ghione]

The pn junction. [Fonstad, Ghione] The pn junction [Fonstad, Ghione] Band diagram On the vertical axis: potential energy of the electrons On the horizontal axis: now there is nothing: later we ll put the position qf s : work function (F

More information

Photonic Devices. Light absorption and emission. Transitions between discrete states

Photonic Devices. Light absorption and emission. Transitions between discrete states Light absorption and emission Photonic Devices Transitions between discrete states Transition rate determined by the two states: Fermi s golden rule Absorption and emission of a semiconductor Vertical

More information

Introduction to semiconductor nanostructures. Peter Kratzer Modern Concepts in Theoretical Physics: Part II Lecture Notes

Introduction to semiconductor nanostructures. Peter Kratzer Modern Concepts in Theoretical Physics: Part II Lecture Notes Introduction to semiconductor nanostructures Peter Kratzer Modern Concepts in Theoretical Physics: Part II Lecture Notes What is a semiconductor? The Fermi level (chemical potential of the electrons) falls

More information

The Physics of Semiconductors

The Physics of Semiconductors The Physics of Semiconductors with applications to optoelectronic devices KEVIN F. BRENNAN CAMBRIDGE UNIVERSITY PRESS Contents Preface page xi Chapter1 Basic Concepts in Quantum Mechanics 1.1 Introduction

More information

Problem 9.20 Threshold bias for an n-channel MOSFET: In the text we used a criterion that the inversion of the MOSFET channel occurs when V s = ;2 F w

Problem 9.20 Threshold bias for an n-channel MOSFET: In the text we used a criterion that the inversion of the MOSFET channel occurs when V s = ;2 F w Prof. Jasprit Singh Fall 2001 EECS 320 Homework 11 The nals for this course are set for Friday December 14, 6:30 8:30 pm and Friday Dec. 21, 10:30 am 12:30 pm. Please choose one of these times and inform

More information

Erik Lind

Erik Lind High-Speed Devices, 2011 Erik Lind (Erik.Lind@ftf.lth.se) Course consists of: 30 h Lectures (H322, and Fys B check schedule) 8h Excercises 2x2h+4h Lab Excercises (2 Computer simulations, 4 RF measurment

More information

Electronic Circuits for Mechatronics ELCT 609 Lecture 2: PN Junctions (1)

Electronic Circuits for Mechatronics ELCT 609 Lecture 2: PN Junctions (1) Electronic Circuits for Mechatronics ELCT 609 Lecture 2: PN Junctions (1) Assistant Professor Office: C3.315 E-mail: eman.azab@guc.edu.eg 1 Electronic (Semiconductor) Devices P-N Junctions (Diodes): Physical

More information

ECE335F: Electronic Devices Syllabus. Lecture*

ECE335F: Electronic Devices Syllabus. Lecture* Lecture 1 - Introduction: Course Overview 1 - Introduction: Course Overview 2 1 Crystal Structure of Solids 2 1 Crystal Structure of Solids 1.1 Semiconductor materials 1.1 Semiconductor materials 1.2 Types

More information

Introduction to Semiconductor Devices

Introduction to Semiconductor Devices Physics 233 Experiment 48 Introduction to Semiconductor Devices References 1. G.W. Neudeck, The PN Junction Diode, Addison-Wesley MA 1989 2. Background notes (Appendix A) 3. Specification sheet for Diode

More information

A SEMICONDUCTOR DIODE. P-N Junction

A SEMICONDUCTOR DIODE. P-N Junction A SEMICONDUCTOR DIODE P-N Junction Analog Electronics Pujianto Department of Physics Edu. State University of Yogyakarta A Semiconductor Devices A Semiconductor devices can be defined as a unit which consists,

More information

1.9.5 Stoichiometry, Nonstoichiometry, and Defect Structures 75

1.9.5 Stoichiometry, Nonstoichiometry, and Defect Structures 75 Chapter 1 Elementary Materials Science Concepts 3 1.1 Atomic Structure and Atomic Number 3 1.2 Atomic Mass and Mole 8 1.3 Bonding and Types of Solids 9 1.3.1 Molecules and General Bonding Principles 9

More information

01 01 Intro to Course

01 01 Intro to Course ECE 474 Spring 2011 Day Date Lecture Chapter Topics M 10 Jan 01 01 Intro to Course Physical structures of crystal systems that are important for devices W 12 02 01 How to quantify physical structures of

More information

Review Energy Bands Carrier Density & Mobility Carrier Transport Generation and Recombination

Review Energy Bands Carrier Density & Mobility Carrier Transport Generation and Recombination Review Energy Bands Carrier Density & Mobility Carrier Transport Generation and Recombination The Metal-Semiconductor Junction: Review Energy band diagram of the metal and the semiconductor before (a)

More information

Recitation 17: BJT-Basic Operation in FAR

Recitation 17: BJT-Basic Operation in FAR Recitation 17: BJT-Basic Operation in FAR BJT stands for Bipolar Junction Transistor 1. Can be thought of as two p-n junctions back to back, you can have pnp or npn. In analogy to MOSFET small current

More information

Midterm I - Solutions

Midterm I - Solutions UNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences EECS 130 Spring 2008 Professor Chenming Hu Midterm I - Solutions Name: SID: Grad/Undergrad: Closed

More information

OPTI510R: Photonics. Khanh Kieu College of Optical Sciences, University of Arizona Meinel building R.626

OPTI510R: Photonics. Khanh Kieu College of Optical Sciences, University of Arizona Meinel building R.626 OPTI510R: Photonics Khanh Kieu College of Optical Sciences, University of Arizona kkieu@optics.arizona.edu Meinel building R.626 Announcements HW#3 is assigned due Feb. 20 st Mid-term exam Feb 27, 2PM

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

Mod. Sim. Dyn. Sys. Amplifiers page 1

Mod. Sim. Dyn. Sys. Amplifiers page 1 AMPLIFIERS A circuit containing only capacitors, amplifiers (transistors) and resistors may resonate. A circuit containing only capacitors and resistors may not. Why does amplification permit resonance

More information

ELEC 3908, Physical Electronics, Lecture 18. The Early Effect, Breakdown and Self-Heating

ELEC 3908, Physical Electronics, Lecture 18. The Early Effect, Breakdown and Self-Heating ELEC 3908, Physical Electronics, Lecture 18 The Early Effect, Breakdown and Self-Heating Lecture Outline Previous 2 lectures analyzed fundamental static (dc) carrier transport in the bipolar transistor

More information

A. F. J. Levi 1 EE539: Engineering Quantum Mechanics. Fall 2017.

A. F. J. Levi 1 EE539: Engineering Quantum Mechanics. Fall 2017. A. F. J. Levi 1 Engineering Quantum Mechanics. Fall 2017. TTh 9.00 a.m. 10.50 a.m., VHE 210. Web site: http://alevi.usc.edu Web site: http://classes.usc.edu/term-20173/classes/ee EE539: Abstract and Prerequisites

More information

II/IV B.Tech (Regular/Supplementary) DEGREE EXAMINATION. Answer ONE question from each unit.

II/IV B.Tech (Regular/Supplementary) DEGREE EXAMINATION. Answer ONE question from each unit. 14ECEI302/EC 212 1. Answer all questions (1X12=12 Marks) a What are the applications of linked list? b Compare singly linked list and doubly linked list. c Define ADT. d What are the basic operations of

More information

From Last Time. Several important conceptual aspects of quantum mechanics Indistinguishability. Symmetry

From Last Time. Several important conceptual aspects of quantum mechanics Indistinguishability. Symmetry From Last Time Several important conceptual aspects of quantum mechanics Indistinguishability particles are absolutely identical Leads to Pauli exclusion principle (one Fermion / quantum state). Symmetry

More information

Introduction to Semiconductor Integrated Optics

Introduction to Semiconductor Integrated Optics Introduction to Semiconductor Integrated Optics Hans P. Zappe Artech House Boston London Contents acknowledgments reface itroduction Chapter 1 Basic Electromagnetics 1 1.1 General Relationships 1 1.1.1

More information

(DPHY 21) 1) a) Discuss the propagation of light in conducting surface. b) Discuss about the metallic reflection at oblique incidence.

(DPHY 21) 1) a) Discuss the propagation of light in conducting surface. b) Discuss about the metallic reflection at oblique incidence. (DPHY 21) ASSIGNMENT - 1, MAY - 2015. PAPER- V : ELECTROMAGNETIC THEORY AND MODERN OPTICS 1) a) Discuss the propagation of light in conducting surface. b) Discuss about the metallic reflection at oblique

More information

EC/EE DIGITAL ELECTRONICS

EC/EE DIGITAL ELECTRONICS EC/EE 214(R-15) Total No. of Questions :09] [Total No. of Pages : 02 II/IV B.Tech. DEGREE EXAMINATIONS, DECEMBER- 2016 First Semester EC/EE DIGITAL ELECTRONICS Time: Three Hours 1. a) Define Encoder Answer

More information

Semiconductor Physics and Devices Chapter 3.

Semiconductor Physics and Devices Chapter 3. Introduction to the Quantum Theory of Solids We applied quantum mechanics and Schrödinger s equation to determine the behavior of electrons in a potential. Important findings Semiconductor Physics and

More information

6.012 Electronic Devices and Circuits

6.012 Electronic Devices and Circuits Page 1 of 12 YOUR NAME Department of Electrical Engineering and Computer Science Massachusetts Institute of Technology 6.012 Electronic Devices and Circuits FINAL EXAMINATION Open book. Notes: 1. Unless

More information

ELEC 4700 Assignment #2

ELEC 4700 Assignment #2 ELEC 4700 Assignment #2 Question 1 (Kasop 4.2) Molecular Orbitals and Atomic Orbitals Consider a linear chain of four identical atoms representing a hypothetical molecule. Suppose that each atomic wavefunction

More information

Sample Exam # 2 ECEN 3320 Fall 2013 Semiconductor Devices October 28, 2013 Due November 4, 2013

Sample Exam # 2 ECEN 3320 Fall 2013 Semiconductor Devices October 28, 2013 Due November 4, 2013 Sample Exam # 2 ECEN 3320 Fall 203 Semiconductor Devices October 28, 203 Due November 4, 203. Below is the capacitance-voltage curve measured from a Schottky contact made on GaAs at T 300 K. Figure : Capacitance

More information

PHYSICS. Course Syllabus. Section 1: Mathematical Physics. Subject Code: PH. Course Structure. Electromagnetic Theory

PHYSICS. Course Syllabus. Section 1: Mathematical Physics. Subject Code: PH. Course Structure. Electromagnetic Theory PHYSICS Subject Code: PH Course Structure Sections/Units Topics Section 1 Section 2 Section 3 Section 4 Section 5 Section 6 Section 7 Section 8 Mathematical Physics Classical Mechanics Electromagnetic

More information

Introduction to Semiconductor Devices

Introduction to Semiconductor Devices Physics 233 Experiment 48 Introduction to Semiconductor Devices References 1. G.W. Neudeck, The PN Junction Diode, Addison-Wesley MA 1989 2. Background notes (Appendix A) 3. Specification sheet for Diode

More information

6.301 Solid-State Circuits Recitation 22: More on Transimpedance Amplifiers, and Intro to Zener Diode References Prof. Joel L.

6.301 Solid-State Circuits Recitation 22: More on Transimpedance Amplifiers, and Intro to Zener Diode References Prof. Joel L. Recitation 22: More on Transimpedance Amplifiers, and Intro to Zener Diode References Before we leave the topic of transimpedance amplifiers completely, there is one biasing mystery that is worth clearing

More information

Lecture 20 - Semiconductor Structures

Lecture 20 - Semiconductor Structures Lecture 0: Structures Kittel Ch 17, p 494-503, 507-511 + extra material in the class notes MOS Structure metal Layer Structure Physics 460 F 006 Lect 0 1 Outline What is a semiconductor Structure? Created

More information

Chapter 7. The pn Junction

Chapter 7. The pn Junction Chapter 7 The pn Junction Chapter 7 PN Junction PN junction can be fabricated by implanting or diffusing donors into a P-type substrate such that a layer of semiconductor is converted into N type. Converting

More information

CONTENTS. vii. CHAPTER 2 Operators 15

CONTENTS. vii. CHAPTER 2 Operators 15 CHAPTER 1 Why Quantum Mechanics? 1 1.1 Newtonian Mechanics and Classical Electromagnetism 1 (a) Newtonian Mechanics 1 (b) Electromagnetism 2 1.2 Black Body Radiation 3 1.3 The Heat Capacity of Solids and

More information

Figure 3.1 (p. 141) Figure 3.2 (p. 142)

Figure 3.1 (p. 141) Figure 3.2 (p. 142) Figure 3.1 (p. 141) Allowed electronic-energy-state systems for two isolated materials. States marked with an X are filled; those unmarked are empty. System 1 is a qualitative representation of a metal;

More information

Electronic Devices & Circuits

Electronic Devices & Circuits Electronic Devices & Circuits For Electronics & Communication Engineering By www.thegateacademy.com Syllabus Syllabus for Electronic Devices Energy Bands in Intrinsic and Extrinsic Silicon, Carrier Transport,

More information

LECTURE 23. MOS transistor. 1 We need a smart switch, i.e., an electronically controlled switch. Lecture Digital Circuits, Logic

LECTURE 23. MOS transistor. 1 We need a smart switch, i.e., an electronically controlled switch. Lecture Digital Circuits, Logic LECTURE 23 Lecture 16-20 Digital Circuits, Logic 1 We need a smart switch, i.e., an electronically controlled switch 2 We need a gain element for example, to make comparators. The device of our dreams

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 I Name: Closed book. One sheet of notes is allowed.

More information

Lecture 17 - The Bipolar Junction Transistor (I) Forward Active Regime. April 10, 2003

Lecture 17 - The Bipolar Junction Transistor (I) Forward Active Regime. April 10, 2003 6.012 - Microelectronic Devices and Circuits - Spring 2003 Lecture 17-1 Lecture 17 - The Bipolar Junction Transistor (I) Contents: Forward Active Regime April 10, 2003 1. BJT: structure and basic operation

More information

Photosynthesis & Solar Power Harvesting

Photosynthesis & Solar Power Harvesting Lecture 23 Semiconductor Detectors - Photodetectors Principle of the pn junction photodiode Absorption coefficient and photodiode materials Properties of semiconductor detectors The pin photodiodes Avalanche

More information

Engineering Physics-II. Question Bank

Engineering Physics-II. Question Bank Engineering Physics-II Question Bank Unit No I Short Answer Type 1. What are de-broglie waves? 2. Discuss few properties of matter waves. 3. What do you mean by phase velocity and group velocity? 4. What

More information

Capacitors Diodes Transistors. PC200 Lectures. Terry Sturtevant. Wilfrid Laurier University. June 4, 2009

Capacitors Diodes Transistors. PC200 Lectures. Terry Sturtevant. Wilfrid Laurier University. June 4, 2009 Wilfrid Laurier University June 4, 2009 Capacitor an electronic device which consists of two conductive plates separated by an insulator Capacitor an electronic device which consists of two conductive

More information

Electronic PRINCIPLES

Electronic PRINCIPLES MALVINO & BATES Electronic PRINCIPLES SEVENTH EDITION Chapter 2 Semiconductors Topics Covered in Chapter 2 Conductors Semiconductors Silicon crystals Intrinsic semiconductors Two types of flow Doping a

More information

Self-study problems and questions Processing and Device Technology, FFF110/FYSD13

Self-study problems and questions Processing and Device Technology, FFF110/FYSD13 Self-study problems and questions Processing and Device Technology, FFF110/FYSD13 Version 2016_01 In addition to the problems discussed at the seminars and at the lectures, you can use this set of problems

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

Quiz #1 Practice Problem Set

Quiz #1 Practice Problem Set Name: Student Number: ELEC 3908 Physical Electronics Quiz #1 Practice Problem Set? Minutes January 22, 2016 - No aids except a non-programmable calculator - All questions must be answered - All questions

More information