Solid State Electronics. Final Examination

Size: px
Start display at page:

Download "Solid State Electronics. Final Examination"

Transcription

1 The University of Toledo EECS:4400/5400/7400 Solid State Electronic Section elssf08fs.fm - 1 Solid State Electronics Final Examination Problems Points Total 40 Was the exam fair? yes no

2 The University of Toledo elssf08fs.fm - 1 Problem 1 1 points For full credit, mark your answers yes, no, or not in all of euhe given choices! 1. 1 In an intrinsic semiconductor material, x concentrations of electrons and holes are unequal, x values of effective masses of electrons and holes are unequal, x mobilities of electrons and holes are unequeal, x diffusion coefficients of electrons and holes are unequal, x amounts of lectrical charges on electrons and holes are unequal. 1. Mean life time of excess minority carriers in semiconductors can be calculated from: x the measured semiconductor material photoconductivity decay, x the measured depletion region capacity of a reverse biased pn-junction, x the measured storage delay time during a reverse recovery transient in a pnjunction, x the measured current intensity through a forward biased pn-junction. 1.3 Useful mechanisms for switching the Silicon Controlled Rectifiers from forward-blocking to forward-conducting state include: x application of an anode to cathode voltage in excess of the peak forward voltage, x application of a rapid changing gate to cathode voltage not in excess of the peak forward voltage, x "base width narrowing", x punch through of the regions n 1 or p, x positive voltage applied to the gate terminal.

3 The University of Toledo elssf08fs.fm The transferred electron mechanism is: x the consequence of a drop in mobility of free electrons with increasing electric field in InP, x responsible for the incremental negative resistance region in the current-voltage characteristic of the Tunnel diode, x the consequence of an increase in mobility of holes with increasing electric field in InP, x the consequence of a drop in mobility of free electrons with increasing electric field in GaAs, x responsible for the incremental negative resistance region in the current-voltage characteristic of the Impact Avalanch Transit Time diode. 1.5 The Hanes-Shockley experiment: x has demonstrated the drift process of minority carriers in semiconductor materials, x has demonstrated the diffusion process of minority carriers in semiconductor materials, x the random motion process of minority carriers in semiconductor materials, x provides information for calculating the mobility value of majority carriers in the semiconductor, x provides information for calculating the diffusion constant value of minority carriers in the semiconductor, 1.6 Thermal Budget is a parameter: x whose value measures the range of applicability of power semiconductor devices, x which is generally maximized in breakdown diodes, x whose value is generally minimized for control over compact doping profiles, x whose value determines whether an oxidation process satisfies the criterion for being considered as "rapid".

4 The University of Toledo elssf08fs.fm - 4 Problem 14 points Given is an abrupt silicon n + p-junction at room temperature, with the following parameters: - room temoerature T = 0 C = 93 K - junction area A = 10-7 m - junction temperature T = 0 C = 93 K - donor concentration N D = donor atoms/m 3 - acceptor concentration N A = 10 1 acceptor atoms/m 3 - intrinsic concentration n i = electron-hole pairs/m 3 - electron mobility µ n = 0.18 m /Vs - hole mobility µ p = 0.06 m /Vs Determine: Solution 1 o contact potential of the junction, o the depletion region width at thermal equilibrium condition, 3 o which junction redesign measure would double the magnitude of the given pn-junction current under forward bias, 4 o if the stated junction redesign measure would have been carried through, how wuld it have affected the following properties of a pn-junction diode which contained the redesigned junction: - the junction capacitance, - the built-in potential of the junction, - the breakdown potential of the junction, - the ohmic losses in the quasi neutral regions of the junction. Hint #1 For full credit, give answers to all questions, prepare all required circuit diagrams, write all equations for which the space is left, and show all symbolic and numerical expressions whose evaluation produces shown numerical results. An explicit demonstration of understanding the following solution steps is expected..1 Calculate the contact potential of the junction; show your work in the space reserved for equation (-1). V bo = V T ln N D N A n i = 0.05 ln = 0.7V (-1)

5 The University of Toledo elssf08fs.fm - 5. Calculate the the depletion region width; show your work in the space reserved for equation (-). W= ε s q = N A +N D Vbo N A N D = 0.94µm (-).3 State the description of the junction redesign measure which would double the magnitude of the given pn-junction current under forward bias; write your statement in the space reserved for equation (-3). Concentration of acceptor doping should be reduced by a factor of two. (-3).4 State the effect of the redesign measure proposed under part.3 on the: - pn-junction capacitance by checking the conditions on all three lines below, x pn-junction capacitance would be increased, x pn-junction capacitance would be decreased x pn-junction capacitance would not be affected,.5 State the effect of the redesign measure proposed under part.3 on the: - pn-junctionbuilt-in potential by checking the conditions on all three lines below, x pn-junction built-in potential of the junction would be increased, x pn-junction built-in potential of the junction would be decreased x pn-junction built-in potential of the junction would not be affected,.6 State the effect of the redesign measure proposed under part.3 on the: - pn-junction break down potentiale by checking the conditions on all three lines below, x pn-junction breakdown potential would be increased, x pn-junction breakdown potential would be decreased x pn-junction breakdown potential would not be affected,.7 State the effect of the redesign measure proposed under part.3 on the: - pn-junction ohmic losses by checking the conditions on all three lines below, x pn-junction ohmic losses would be increased, x pn-junction ohmic losses would be decreased x pn-junction ohmic losses would not be affected,

6 The University of Toledo elssf08fs.fm - 6 Problem 3 14 points Given is an abrupt silicon pn-junction at room temperature, with the following parameters: a) whole junction - junction area A = 10-8 m - junction temperature T = 0 C = 93 K b) n-region - donor concentration N D = donor atoms/m 3 - electron/hole mobility µ nn = 0.13 m /Vs - µ np = m /Vs - excess minority carrier life timeτ n = 0.1µs c) p-region - acceptor concentration N A = 10 3 acceptor atoms/m 3 - electron/hole mobility µ pn = 0.07 m /Vs - µ pp = 0.0 m /Vs - excess minority carrier life timeτ p = 10µs Prepare: Solution 1 o Current i D through the junction when junction is forwad biased with v D = 0.5V, o Current i D through the junction when junction is reverse biased with v D = -0.5V. Hint #1 For full credit, give answers to all questions, prepare all required circuit diagrams, write all equations for which the space is left, and show all symbolic and numerical expressions whose evaluation produces shown numerical results. An explicit demonstration of understanding the following solution steps is expected. 3.1 Calculate the values of the majority carrier concentrations in the quasi-neutra regions of the given pn-junction; show your work in the space reserved for equation (3-1). n no N D = free electrons/m 3 (3-1) p po N A = holes/m 3 3. Calculate the values of the minority carrier concentrations in the quasi-neutral regions of the given pn-junction; show your work in the space reserved for equation (3-). n po = p no = n i p = = free electrons/m 3 p 10 3 (3-) n i n n = = holes/m 3

7 The University of Toledo elssf08fs.fm Calculate the values of the minority carrier diffusion constants in the quasi-neutral regions of the given pn-junction; show your work in the space reserved for equation (3-3). D n =µ pn. V T = = = m s -1 D p =µ np. V T = = = m s -1 (3-3) 3.4 Calculate the values of the minority carrier diffusion lengths in the quasi-neutral regions of the given pn-junction; show your work in the space reserved for equation (3-4). L n= D nτ n = = 13.3 [µm] L p= D pτ p = = 106 [µm] (3-4) 3.5 Calculate the values of the reverse saturation current of the given pn-junction; show your work in the space reserved for equation (3-5). D p D n I p o = qa ( n + np ) = ( L p Ln ) = (3-5) = 1.07 fa 3.6 Calculate the value of the given pn-junction current under forward bias; show your work in the space reserved for equation (3-6). i D = I o v D V T 0.5 (3-6) ( e - 1 ) = ( - 1) = e 0.05 ( e - 1) = = 0.5µA 3.7 Calculate the value of the given pn-junction current under reverse bias; show your work in the space reserved for equation (3-7). v D i D = I V T = o ( -15 ( e - 1 ) e - 1) = ( e -0-1) = A (3-7)

Session 6: Solid State Physics. Diode

Session 6: Solid State Physics. Diode Session 6: Solid State Physics Diode 1 Outline A B C D E F G H I J 2 Definitions / Assumptions Homojunction: the junction is between two regions of the same material Heterojunction: the junction is between

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

For the following statements, mark ( ) for true statement and (X) for wrong statement and correct it.

For the following statements, mark ( ) for true statement and (X) for wrong statement and correct it. Benha University Faculty of Engineering Shoubra Electrical Engineering Department First Year communications. Answer all the following questions Illustrate your answers with sketches when necessary. The

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

Schottky Rectifiers Zheng Yang (ERF 3017,

Schottky Rectifiers Zheng Yang (ERF 3017, ECE442 Power Semiconductor Devices and Integrated Circuits Schottky Rectifiers Zheng Yang (ERF 3017, email: yangzhen@uic.edu) Power Schottky Rectifier Structure 2 Metal-Semiconductor Contact The work function

More information

PN Junction

PN Junction P Junction 2017-05-04 Definition Power Electronics = semiconductor switches are used Analogue amplifier = high power loss 250 200 u x 150 100 u Udc i 50 0 0 50 100 150 200 250 300 350 400 i,u dc i,u u

More information

EECS130 Integrated Circuit Devices

EECS130 Integrated Circuit Devices EECS130 Integrated Circuit Devices Professor Ali Javey 9/18/2007 P Junctions Lecture 1 Reading: Chapter 5 Announcements For THIS WEEK OLY, Prof. Javey's office hours will be held on Tuesday, Sept 18 3:30-4:30

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

p-n junction biasing, p-n I-V characteristics, p-n currents Norlaili Mohd. Noh EEE /09

p-n junction biasing, p-n I-V characteristics, p-n currents Norlaili Mohd. Noh EEE /09 CLASS 6&7 p-n junction biasing, p-n I-V characteristics, p-n currents 1 p-n junction biasing Unbiased p-n junction: the potential barrier is 0.7 V for Si and 0.3 V for Ge. Nett current across the p-n junction

More information

Diodes. anode. cathode. cut-off. Can be approximated by a piecewise-linear-like characteristic. Lecture 9-1

Diodes. anode. cathode. cut-off. Can be approximated by a piecewise-linear-like characteristic. Lecture 9-1 Diodes mplest nonlinear circuit element Basic operation sets the foundation for Bipolar Junction Transistors (BJTs) Also present in Field Effect Transistors (FETs) Ideal diode characteristic anode cathode

More information

Semiconductor Physics. Lecture 6

Semiconductor Physics. Lecture 6 Semiconductor Physics Lecture 6 Recap pn junction and the depletion region Driven by the need to have no gradient in the fermi level free carriers migrate across the pn junction leaving a region with few

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

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

Lecture 2. Introduction to semiconductors Structures and characteristics in semiconductors

Lecture 2. Introduction to semiconductors Structures and characteristics in semiconductors Lecture 2 Introduction to semiconductors Structures and characteristics in semiconductors Semiconductor p-n junction Metal Oxide Silicon structure Semiconductor contact Literature Glen F. Knoll, Radiation

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

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

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

L03: pn Junctions, Diodes

L03: pn Junctions, Diodes 8/30/2012 Page 1 of 5 Reference:C:\Users\Bernhard Boser\Documents\Files\Lib\MathCAD\Default\defaults.mcd L03: pn Junctions, Diodes Intrinsic Si Q: What are n, p? Q: Is the Si charged? Q: How could we make

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

junctions produce nonlinear current voltage characteristics which can be exploited

junctions produce nonlinear current voltage characteristics which can be exploited Chapter 6 P-N DODES Junctions between n-and p-type semiconductors are extremely important foravariety of devices. Diodes based on p-n junctions produce nonlinear current voltage characteristics which can

More information

Lecture 2. Introduction to semiconductors Structures and characteristics in semiconductors

Lecture 2. Introduction to semiconductors Structures and characteristics in semiconductors Lecture 2 Introduction to semiconductors Structures and characteristics in semiconductors Semiconductor p-n junction Metal Oxide Silicon structure Semiconductor contact Literature Glen F. Knoll, Radiation

More information

Basic Physics of Semiconductors

Basic Physics of Semiconductors Basic Physics of Semiconductors Semiconductor materials and their properties PN-junction diodes Reverse Breakdown EEM 205 Electronics I Dicle University, EEE Dr. Mehmet Siraç ÖZERDEM Semiconductor Physics

More information

ECE PN Junctions and Diodes

ECE PN Junctions and Diodes ECE 342 2. PN Junctions and iodes Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois jschutt@emlab.uiuc.edu ECE 342 Jose Schutt Aine 1 B: material dependent parameter = 5.4 10

More information

This is the 15th lecture of this course in which we begin a new topic, Excess Carriers. This topic will be covered in two lectures.

This is the 15th lecture of this course in which we begin a new topic, Excess Carriers. This topic will be covered in two lectures. Solid State Devices Dr. S. Karmalkar Department of Electronics and Communication Engineering Indian Institute of Technology, Madras Lecture - 15 Excess Carriers This is the 15th lecture of this course

More information

Lecture 15 - The pn Junction Diode (I) I-V Characteristics. November 1, 2005

Lecture 15 - The pn Junction Diode (I) I-V Characteristics. November 1, 2005 6.012 - Microelectronic Devices and Circuits - Fall 2005 Lecture 15-1 Lecture 15 - The pn Junction Diode (I) I-V Characteristics November 1, 2005 Contents: 1. pn junction under bias 2. I-V characteristics

More information

Consider a uniformly doped PN junction, in which one region of the semiconductor is uniformly doped with acceptor atoms and the adjacent region is

Consider a uniformly doped PN junction, in which one region of the semiconductor is uniformly doped with acceptor atoms and the adjacent region is CHAPTER 7 The PN Junction Consider a uniformly doped PN junction, in which one region of the semiconductor is uniformly doped with acceptor atoms and the adjacent region is uniformly doped with donor atoms.

More information

Junction Diodes. Tim Sumner, Imperial College, Rm: 1009, x /18/2006

Junction Diodes. Tim Sumner, Imperial College, Rm: 1009, x /18/2006 Junction Diodes Most elementary solid state junction electronic devices. They conduct in one direction (almost correct). Useful when one converts from AC to DC (rectifier). But today diodes have a wide

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

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

ECE-342 Test 2 Solutions, Nov 4, :00-8:00pm, Closed Book (one page of notes allowed)

ECE-342 Test 2 Solutions, Nov 4, :00-8:00pm, Closed Book (one page of notes allowed) ECE-342 Test 2 Solutions, Nov 4, 2008 6:00-8:00pm, Closed Book (one page of notes allowed) Please use the following physical constants in your calculations: Boltzmann s Constant: Electron Charge: Free

More information

Fundamentals of Semiconductor Physics

Fundamentals of Semiconductor Physics Fall 2007 Fundamentals of Semiconductor Physics 万 歆 Zhejiang Institute of Modern Physics xinwan@zimp.zju.edu.cn http://zimp.zju.edu.cn/~xinwan/ Transistor technology evokes new physics The objective of

More information

1st Year-Computer Communication Engineering-RUC. 4- P-N Junction

1st Year-Computer Communication Engineering-RUC. 4- P-N Junction 4- P-N Junction We begin our study of semiconductor devices with the junction for three reasons. (1) The device finds application in many electronic systems, e.g., in adapters that charge the batteries

More information

Diodes. EE223 Digital & Analogue Electronics Derek Molloy 2012/2013.

Diodes. EE223 Digital & Analogue Electronics Derek Molloy 2012/2013. Diodes EE223 Digital & Analogue Electronics Derek Molloy 2012/2013 Derek.Molloy@dcu.ie Diodes: A Semiconductor? Conductors Such as copper, aluminium have a cloud of free electrons weak bound valence electrons

More information

Lecture-4 Junction Diode Characteristics

Lecture-4 Junction Diode Characteristics 1 Lecture-4 Junction Diode Characteristics Part-II Q: Aluminum is alloyed into n-type Si sample (N D = 10 16 cm 3 ) forming an abrupt junction of circular cross-section, with an diameter of 0.02 in. Assume

More information

pn JUNCTION THE SHOCKLEY MODEL

pn JUNCTION THE SHOCKLEY MODEL The pn Junction: The Shockley Model ( S. O. Kasap, 1990-001) 1 pn JUNCTION THE SHOCKLEY MODEL Safa Kasap Department of Electrical Engineering University of Saskatchewan Canada Although the hole and its

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

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

Diodes for Power Electronic Applications

Diodes for Power Electronic Applications Lecture Notes Diodes for Power Electronic Applications William P. Robbins Professor, Dept. of Electrical and Computer Engineering University of Minnesota OUTLINE PN junction power diode construction Breakdown

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

Lecture 2. Introduction to semiconductors Structures and characteristics in semiconductors. Fabrication of semiconductor sensor

Lecture 2. Introduction to semiconductors Structures and characteristics in semiconductors. Fabrication of semiconductor sensor Lecture 2 Introduction to semiconductors Structures and characteristics in semiconductors Semiconductor p-n junction Metal Oxide Silicon structure Semiconductor contact Fabrication of semiconductor sensor

More information

PN Junction Diode. Diode Cases. Semiconductor Elements. 2009, EE141Associate Professor PhD. T.Vasileva

PN Junction Diode. Diode Cases. Semiconductor Elements. 2009, EE141Associate Professor PhD. T.Vasileva PN Junction Diode Semiconductor Elements 1 Diode Cases 2 1 Basic Diode Feature The essential feature of a diode is at e magnitude of e current greatly depends on e polarity of applied voltage. Basicaly

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

CHAPTER 4: P-N P N JUNCTION Part 2. M.N.A. Halif & S.N. Sabki

CHAPTER 4: P-N P N JUNCTION Part 2. M.N.A. Halif & S.N. Sabki CHAPTER 4: P-N P N JUNCTION Part 2 Part 2 Charge Storage & Transient Behavior Junction Breakdown Heterojunction CHARGE STORAGE & TRANSIENT BEHAVIOR Once injected across the junction, the minority carriers

More information

Nature of Lesson (Lecture/Tutorial) H3 WK No. Day/ Date. Remarks. Duration. 4.00pm 6.30pm ALL. 2.5 hours. Introduction to Semiconductors Lecture 01

Nature of Lesson (Lecture/Tutorial) H3 WK No. Day/ Date. Remarks. Duration. 4.00pm 6.30pm ALL. 2.5 hours. Introduction to Semiconductors Lecture 01 JANUARY 2018 INTAKE Subject : Semiconductor Physics & Devices Venue : HCI Schedule : Mondays for Tutorial (3pm 5pm / 5pm 7pm) or Tuesdays for Tutorial (3pm 5pm / 5pm 7pm) and Thursdays for Lecture (4pm-6.30

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

Peak Electric Field. Junction breakdown occurs when the peak electric field in the PN junction reaches a critical value. For the N + P junction,

Peak Electric Field. Junction breakdown occurs when the peak electric field in the PN junction reaches a critical value. For the N + P junction, Peak Electric Field Junction breakdown occurs when the peak electric field in the P junction reaches a critical value. For the + P junction, qa E ( x) ( xp x), s W dep 2 s ( bi Vr ) 2 s potential barrier

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

Lecture (02) PN Junctions and Diodes

Lecture (02) PN Junctions and Diodes Lecture (02) PN Junctions and Diodes By: Dr. Ahmed ElShafee ١ I Agenda N type, P type semiconductors N Type Semiconductor P Type Semiconductor PN junction Energy Diagrams of the PN Junction and Depletion

More information

Holes (10x larger). Diode currents proportional to minority carrier densities on each side of the depletion region: J n n p0 = n i 2

Holes (10x larger). Diode currents proportional to minority carrier densities on each side of the depletion region: J n n p0 = n i 2 Part V. (40 pts.) A diode is composed of an abrupt PN junction with N D = 10 16 /cm 3 and N A =10 17 /cm 3. The diode is very long so you can assume the ends are at x =positive and negative infinity. 1.

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

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

SRI VIDYA COLLEGE OF ENGINEERING AND TECHNOLOGY VIRUDHUNAGAR Department of Electronics and Communication Engineering

SRI VIDYA COLLEGE OF ENGINEERING AND TECHNOLOGY VIRUDHUNAGAR Department of Electronics and Communication Engineering SRI VIDYA COLLEGE OF ENGINEERING AND TECHNOLOGY VIRUDHUNAGAR Department of Electronics and Communication Engineering Class/Sem:I ECE/II Question Bank for EC6201-ELECTRONIC DEVICES 1.What do u meant by

More information

SEMICONDUCTORS. Conductivity lies between conductors and insulators. The flow of charge in a metal results from the

SEMICONDUCTORS. Conductivity lies between conductors and insulators. The flow of charge in a metal results from the SEMICONDUCTORS Conductivity lies between conductors and insulators The flow of charge in a metal results from the movement of electrons Electros are negatively charged particles (q=1.60x10-19 C ) The outermost

More information

collisions of electrons. In semiconductor, in certain temperature ranges the conductivity increases rapidly by increasing temperature

collisions of electrons. In semiconductor, in certain temperature ranges the conductivity increases rapidly by increasing temperature 1.9. Temperature Dependence of Semiconductor Conductivity Such dependence is one most important in semiconductor. In metals, Conductivity decreases by increasing temperature due to greater frequency of

More information

ECE-305: Spring 2018 Exam 2 Review

ECE-305: Spring 2018 Exam 2 Review ECE-305: Spring 018 Exam Review Pierret, Semiconductor Device Fundamentals (SDF) Chapter 3 (pp. 75-138) Chapter 5 (pp. 195-6) Professor Peter Bermel Electrical and Computer Engineering Purdue University,

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

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

FYS 3028/8028 Solar Energy and Energy Storage. Calculator with empty memory Language dictionaries

FYS 3028/8028 Solar Energy and Energy Storage. Calculator with empty memory Language dictionaries Faculty of Science and Technology Exam in: FYS 3028/8028 Solar Energy and Energy Storage Date: 11.05.2016 Time: 9-13 Place: Åsgårdvegen 9 Approved aids: Type of sheets (sqares/lines): Number of pages incl.

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

Lecture (02) Introduction to Electronics II, PN Junction and Diodes I

Lecture (02) Introduction to Electronics II, PN Junction and Diodes I Lecture (02) Introduction to Electronics II, PN Junction and Diodes I By: Dr. Ahmed ElShafee ١ Agenda Current in semiconductors/conductors N type, P type semiconductors N Type Semiconductor P Type Semiconductor

More information

( )! N D ( x) ) and equilibrium

( )! N D ( x) ) and equilibrium ECE 66: SOLUTIONS: ECE 66 Homework Week 8 Mark Lundstrom March 7, 13 1) The doping profile for an n- type silicon wafer ( N D = 1 15 cm - 3 ) with a heavily doped thin layer at the surface (surface concentration,

More information

Concept of Core IENGINEERS- CONSULTANTS LECTURE NOTES SERIES ELECTRONICS ENGINEERING 1 YEAR UPTU. Page 1

Concept of Core IENGINEERS- CONSULTANTS LECTURE NOTES SERIES ELECTRONICS ENGINEERING 1 YEAR UPTU. Page 1 Concept of Core Conductivity of conductor and semiconductor can also be explained by concept of Core. Core: Core is a part of an atom other than its valence electrons. Core consists of all inner shells

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

ECE 340 Lecture 27 : Junction Capacitance Class Outline:

ECE 340 Lecture 27 : Junction Capacitance Class Outline: ECE 340 Lecture 27 : Junction Capacitance Class Outline: Breakdown Review Junction Capacitance Things you should know when you leave M.J. Gilbert ECE 340 Lecture 27 10/24/11 Key Questions What types of

More information

Department of Electrical and Computer Engineering, Cornell University. ECE 3150: Microelectronics. Spring Due on Feb. 15, 2018 by 7:00 PM

Department of Electrical and Computer Engineering, Cornell University. ECE 3150: Microelectronics. Spring Due on Feb. 15, 2018 by 7:00 PM Department of Electrical and Computer Engineering, Cornell University ECE 3150: Microelectronics Spring 018 Homework 3 Due on Feb. 15, 018 by 7:00 PM Suggested Readings: a) Lecture notes Important Note:

More information

Chap. 11 Semiconductor Diodes

Chap. 11 Semiconductor Diodes Chap. 11 Semiconductor Diodes Semiconductor diodes provide the best resolution for energy measurements, silicon based devices are generally used for charged-particles, germanium for photons. Scintillators

More information

PHYSICAL ELECTRONICS(ECE3540) CHAPTER 9 METAL SEMICONDUCTOR AND SEMICONDUCTOR HETERO-JUNCTIONS

PHYSICAL ELECTRONICS(ECE3540) CHAPTER 9 METAL SEMICONDUCTOR AND SEMICONDUCTOR HETERO-JUNCTIONS PHYSICAL ELECTRONICS(ECE3540) CHAPTER 9 METAL SEMICONDUCTOR AND SEMICONDUCTOR HETERO-JUNCTIONS Tennessee Technological University Monday, November 11, 013 1 Introduction Chapter 4: we considered the 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

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 EECS 40 Spring 2000 Introduction to Microelectronic Devices Prof. King MIDTERM EXAMINATION

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

Lecture 19 - p-n Junction (cont.) October 18, Ideal p-n junction out of equilibrium (cont.) 2. pn junction diode: parasitics, dynamics

Lecture 19 - p-n Junction (cont.) October 18, Ideal p-n junction out of equilibrium (cont.) 2. pn junction diode: parasitics, dynamics 6.720J/3.43J - Integrated Microelectronic Devices - Fall 2002 Lecture 19-1 Lecture 19 - p-n Junction (cont.) October 18, 2002 Contents: 1. Ideal p-n junction out of equilibrium (cont.) 2. pn junction diode:

More information

ITT Technical Institute ET215 Devices I Unit 1

ITT Technical Institute ET215 Devices I Unit 1 ITT Technical Institute ET215 Devices I Unit 1 Chapter 1 Chapter 2, Sections 2.1-2.4 Chapter 1 Basic Concepts of Analog Circuits Recall ET115 & ET145 Ohms Law I = V/R If voltage across a resistor increases

More information

(Refer Slide Time: 03:41)

(Refer Slide Time: 03:41) Solid State Devices Dr. S. Karmalkar Department of Electronics and Communication Engineering Indian Institute of Technology, Madras Lecture - 25 PN Junction (Contd ) This is the 25th lecture of this course

More information

Unit IV Semiconductors Engineering Physics

Unit IV Semiconductors Engineering Physics Introduction A semiconductor is a material that has a resistivity lies between that of a conductor and an insulator. The conductivity of a semiconductor material can be varied under an external electrical

More information

PHYSICAL ELECTRONICS(ECE3540) CHAPTER 9 METAL SEMICONDUCTOR AND SEMICONDUCTOR HETERO-JUNCTIONS

PHYSICAL ELECTRONICS(ECE3540) CHAPTER 9 METAL SEMICONDUCTOR AND SEMICONDUCTOR HETERO-JUNCTIONS PHYSICAL ELECTRONICS(ECE3540) CHAPTER 9 METAL SEMICONDUCTOR AND SEMICONDUCTOR HETERO-JUNCTIONS Tennessee Technological University Wednesday, October 30, 013 1 Introduction Chapter 4: we considered the

More information

Introduction to Power Semiconductor Devices

Introduction to Power Semiconductor Devices ECE442 Power Semiconductor Devices and Integrated Circuits Introduction to Power Semiconductor Devices Zheng Yang (ERF 3017, email: yangzhen@uic.edu) Power Semiconductor Devices Applications System Ratings

More information

3.7 Physical Operation of Diodes

3.7 Physical Operation of Diodes 10/4/2005 3_7 Physical Operation of Diodes blank.doc 1/2 3.7 Physical Operation of Diodes Reading Assignment: pp. 190200, 203205 A. Semiconductor Materials Q: So, what exactly is a junction diode made

More information

Lecture 12: MOS Capacitors, transistors. Context

Lecture 12: MOS Capacitors, transistors. Context Lecture 12: MOS Capacitors, transistors Context In the last lecture, we discussed PN diodes, and the depletion layer into semiconductor surfaces. Small signal models In this lecture, we will apply those

More information

BJT - Mode of Operations

BJT - Mode of Operations JT - Mode of Operations JTs can be modeled by two back-to-back diodes. N+ P N- N+ JTs are operated in four modes. HO #6: LN 251 - JT M Models Page 1 1) Forward active / normal junction forward biased junction

More information

The Devices. Digital Integrated Circuits A Design Perspective. Jan M. Rabaey Anantha Chandrakasan Borivoje Nikolic. July 30, 2002

The Devices. Digital Integrated Circuits A Design Perspective. Jan M. Rabaey Anantha Chandrakasan Borivoje Nikolic. July 30, 2002 igital Integrated Circuits A esign Perspective Jan M. Rabaey Anantha Chandrakasan Borivoje Nikolic The evices July 30, 2002 Goal of this chapter Present intuitive understanding of device operation Introduction

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

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

ELECTRONICS IA 2017 SCHEME

ELECTRONICS IA 2017 SCHEME ELECTRONICS IA 2017 SCHEME CONTENTS 1 [ 5 marks ]...4 2...5 a. [ 2 marks ]...5 b. [ 2 marks ]...5 c. [ 5 marks ]...5 d. [ 2 marks ]...5 3...6 a. [ 3 marks ]...6 b. [ 3 marks ]...6 4 [ 7 marks ]...7 5...8

More information

Operation and Modeling of. The MOS Transistor. Second Edition. Yannis Tsividis Columbia University. New York Oxford OXFORD UNIVERSITY PRESS

Operation and Modeling of. The MOS Transistor. Second Edition. Yannis Tsividis Columbia University. New York Oxford OXFORD UNIVERSITY PRESS Operation and Modeling of The MOS Transistor Second Edition Yannis Tsividis Columbia University New York Oxford OXFORD UNIVERSITY PRESS CONTENTS Chapter 1 l.l 1.2 1.3 1.4 1.5 1.6 1.7 Chapter 2 2.1 2.2

More information

Semiconductor Junctions

Semiconductor Junctions 8 Semiconductor Junctions Almost all solar cells contain junctions between different materials of different doping. Since these junctions are crucial to the operation of the solar cell, we will discuss

More information

PN Junction and MOS structure

PN Junction and MOS structure PN Junction and MOS structure Basic electrostatic equations We will use simple one-dimensional electrostatic equations to develop insight and basic understanding of how semiconductor devices operate Gauss's

More information

Lecture 6 PN Junction and MOS Electrostatics(III) Metal-Oxide-Semiconductor Structure

Lecture 6 PN Junction and MOS Electrostatics(III) Metal-Oxide-Semiconductor Structure Lecture 6 PN Junction and MOS Electrostatics(III) Metal-Oxide-Semiconductor Structure Outline 1. Introduction to MOS structure 2. Electrostatics of MOS in thermal equilibrium 3. Electrostatics of MOS with

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

Electronics I. Midterm 2

Electronics I. Midterm 2 The University of Toledo Section s5m2s_elct7.fm - S:3400 lectronics I r. nthony. Johnson lectronics I Midterm 2 Problems Points. 4 2. 5 3. 6 Total 5 Was the exam fair? yes no The University of Toledo s5m2s_elct7.fm

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

Metal Semiconductor Contacts

Metal Semiconductor Contacts Metal Semiconductor Contacts The investigation of rectification in metal-semiconductor contacts was first described by Braun [33-35], who discovered in 1874 the asymmetric nature of electrical conduction

More information

electronics fundamentals

electronics fundamentals electronics fundamentals circuits, devices, and applications THOMAS L. FLOYD DAVID M. BUCHLA Lesson 1: Diodes and Applications Semiconductors Figure 1-1 The Bohr model of an atom showing electrons in orbits

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

The Devices. Jan M. Rabaey

The Devices. Jan M. Rabaey The Devices Jan M. Rabaey Goal of this chapter Present intuitive understanding of device operation Introduction of basic device equations Introduction of models for manual analysis Introduction of models

More information

Schottky diodes. JFETs - MESFETs - MODFETs

Schottky diodes. JFETs - MESFETs - MODFETs Technische Universität Graz Institute of Solid State Physics Schottky diodes JFETs - MESFETs - MODFETs Quasi Fermi level When the charge carriers are not in equilibrium the Fermi energy can be different

More information

ECEN 3320 Semiconductor Devices Final exam - Sunday December 17, 2000

ECEN 3320 Semiconductor Devices Final exam - Sunday December 17, 2000 Your Name: ECEN 3320 Semiconductor Devices Final exam - Sunday December 17, 2000 1. Review questions a) Illustrate the generation of a photocurrent in a p-n diode by drawing an energy band diagram. Indicate

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

UNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences. Professor Chenming Hu.

UNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences. Professor Chenming Hu. UNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences EECS 130 Spring 2009 Professor Chenming Hu Midterm I Name: Closed book. One sheet of notes is

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

Lecture 18. New gas detectors Solid state trackers

Lecture 18. New gas detectors Solid state trackers Lecture 18 New gas detectors Solid state trackers Time projection Chamber Full 3-D track reconstruction x-y from wires and segmented cathode of MWPC z from drift time de/dx information (extra) Drift over

More information