ECE 3040 Microelectronic Circuits
|
|
- Basil Anthony
- 5 years ago
- Views:
Transcription
1 ECE 3040 Microelectronic Circuits Exam 1 February 17, 2014 Dr. W. Alan Doolittle Print your name clearly and largely: Instructions: Read all the problems carefully and thoroughly before you begin working. You are allowed to use 1 sheet of notes (1 page front and back) as well as a calculator. There are 100 total points. Observe the point value of each problem and allocate your time accordingly. SHOW ALL WORK AND CIRCLE YOUR FINAL ANSWER WITH THE PROPER UNITS INDICA TED. Write legibly. Ifl cannot read it, it will be considered a wrong answer. Do all work on the paper provided. Turn in all scratch paper, even if it did not lead to an answer. Report any and all ethics violations to the instructor. A periodic table is supplied on the last page. Good luck! Sign your name on ONE of the two following cases: I DID NOT observe any ethical violations during this exam: I observed an ethical violation during this exam:
2 True/False (Circle the letter of the most correct answer or answers) 1.) (2-points)~r False: The energy bandgap results from hybridization (intermixing) of sand p orbitals an~es allowed and disallowed energies for electrons in a semiconductor or insulator. 2.) (2-points@ or False: Atoms with weak (small) chemical bond strengths usually result in smaller energy bandgaps and large mobility (due to infrequent collisions resulting from low atomic de~. 3.) (2-points) True r False: The fermi distribution function defines whether a state will be likely to be empty o ed~ 4.) (2-points) True o False lno.3gao.1n 2 is a valid semiconductor formula in standard semicond~ota n. 5.) (2-points True r False: The density of states describes the number of allowed states at a given energy and ar aw~ energy) from the band edges has a decreasing exponential form. 6.) (2-points) True o False To determine th~concentration, one must multiply the density of states by the Fermi 1bution function and integrate that product over all energies. Short Answer 7.) (22 points total) Write in the blanks (on the next page) the answer to the following questions using the information below: Given a semiconductor at room temperature (27 degrees C) has the following parameters and energy band diagram: Hole Diffusion coefficient, Dp=l1.86 cm 2 /Sec Electron Diffusion coefficient, Dn= cm 2 /Sec Substrate intrinsic concentration, ni=lelo cm- 3 Energy-axis a be d e x-axis. f gh I. J
3 Example Answer: '' region c<x<e, region h<x<i and point f' a.) (4-points) Which region(s) contain nonzero electric fields? lo (... X (._ R... ()AJ.. b.) (4-points) Which region(s) are n-type? c.) ( 4-points) Which region(s) are degenerate? d.) (4-points) Which region(s) has zero total (sum) current? e.) (6-points) If the slope ofec for the region h<x<j is 1000 ev/cm what is the electron drift velocity at point i? (Hint: Be careful of your units.) Fenc.,; e"" t~6{ t.ev~ \ ts f (e,. t- K~<.> ""'r".. "t ( I ) ( e I) ) -Itt j ) I -t~t. /ooo,-- (/.b. fo ev.b (o C.. <:.~ (Ooo too o UJ.,.. - f'/" t'\ ~ -= DtJ S ~T('L, -- ( n. b l.:;- '-"'"/r ) ( I ooo '1<,...,) D.D 2)tf V { uol., ::: /. 3 o /o" <-... fs}
4 Short Answer ("Plug and Chug"): For the following problems (8-10) use the following material parameters and assuming total ionization: ni=2e6 cm- 3 N 0 =2e15 cm- 3 donors NA=1e15 cm- 3 acceptors mp*=0.55m 0 mn =0.36mo Ea=l.45 ev Electron mobility, J.ln = 2200 cm 2 Nsec Hole mobility, f..lp = 500 cm 2 N-sec Temperature=27 degrees C 8) (7-points) Where is the Fermi-energy (relative to the valence band which is referenced to zero energy)? II\ -:::: IJ0 ~ Nt<, -r [( Nv:N,.,_)',_ +"'d 'h. ::: ~ tc''i"; ~-~~I) + [ c ID 1 ~ 1 /0 1 <;/' + (L lb' )'-J''' ::: / to"',;: J = "( '- -::: (2. to'- c.~'\) t -:. -l -J P V\ 1 (t> (.{4 Vf,{...(). '' -l 'f ft> C"~-t ;:: -= { "" Q e V p ::- Nv 12. tev-erl/h ~ Ef =. Ev- Jc.T f.) 1...( T~ere. <lre ~ev(/'11 11 ~ )/ a ~ (~(""" ~ hve_ Nv ::.. (Z.)I /D,;. ) (o.~5) 2. = f.jo'',.:-j.-. s 0 ( ""+if) ~) ' EF ::. (0 ev)- (o.o2..s-~ ev\(" ('1~ 1 '"~l' ) ::' f.zq.ev I I o ""' 9) ( 10-points) A 10 urn x 10 urn x 500 urn rectangular semiconductor resistor is made from the semiconductor from problem 8. It is biased on two opposing sides (longest dimension) with 9 volts. Determine both the electron and hole current density and currents flowing in the device. r ::: T' to c.~ tl -J -1 T.v -== t r-v\ t\ t.,.. (f.~ (o- 11 c,)(nod -~~;)(t-to 1 'c..:: 1 )(/So,f) ~> (;,"?,,";(, ~/,'!} Ttl".f>y.JN:: (/o-\,_,')(b).j{, /t/o.,') lt!: : b). ) c.,... A]
5 Section 3 (more short answer) 10) (I 0-points total) The material in problems 8 and 9 is exposed to a laser light that generates 2e 16-3 em extra mmonty earners. a) (2 points) Is this low level or high level injection? ((, -'l AV\-::. ~p-:::. t.. JD c.m n 0 -= I to 1 r c..""-j ----;> b) (8 points) Draw the 1 dimensional energy band diagram showing the placement of both the quasi-fermi levels (numeric answer) relative to~. Ec, and Ev. 11\::. 11\0 + A"' f + 6f ::.. ) /0 J') ~-J + 2 /01b ("'-~ ::: 2...{ fi:l,, (.f'-\-3 r... <J- ;o (...,4., (0 {.Jio\. -~ lb - s ~ 1... I c/fo c."'.. :3. o.1>~ ev E; ::. o.1 ~ ev &v:; 0 e V -.. _----- Fr::. o.jjl e..v
6 Pulling all the concepts together for a useful purpose: 11.) (39-points) A semi-infinite length of semiconductor in a device flies on a satellite launched in 1966 and has been exposed to constant cosmic radiation and sunlight. The light is absorbed uniformly in the semiconductor. Over time, the radiation damages the front surface. This problem deals with the performance after being exposed to the radiation for a very long time (i.e. not the initial pristine condition). The semiconductor is doped p-type with an acceptor concentration of le15 cm" 3 and has a minority carrier lifetime, of 400 picoseconds (400e-12 seconds). Photons absorbed in the semiconductor generate le19 extra electron-hole pairs per cm 3 per second. It is found that at the surface exposed to the radiation, x=o, the excess electron concentration is smaller than in the rest of the device,!l.n(x=0)=2e9cm 3. If the semiconductor is held at room temperature (27 degrees C), determine the minority carrier diffusion current density at all positions in the semiconductor (x ~ 0 urn). Assume a minority carrier mobility of 100 cm 2 Nsec, 27 degree C operation and the intrinsic concentration is le6cm 3. 1'~ \ ~ (.'tv\ \\t ~ f-~f ~~ rp ~f d 2 ilil Given: 0= Dn 2 P dx ililp Tn General Solution is: d 2!l.n!l.nP Given: 0 = Dn dx2 p --+GL Tn d 2!l.n Given: 0 = Dn dx2 p General Solution is: Given: O=Dn d 2!l.n 2P+GL dx General Solution is: 2 Given: 0 = Dn d dx i'l~p + Gwf(x) General Solution is: MP (x )=[- Gw Jf f(x)dx] + Bx + C DN,t'-1\S v.j)f\1~ d!l.np = _ i'lnp () - t/ Given: General Solution is:!l.np t =!l.np(t = O)e 1 '" dt Tn t~ i r ~!l.~n~ Given: 0 = P + GL General Solution is: f'lji',tj Tn 'f.~.(~e~e.. i~ c... to"\c..t v\'fy"r-h"ta., 0 r~ta;e"'t V\f.Par ft...e >""r.f4c1z t!jf fi,.e- JtviLL, iv\tttttj.. fr"o""- 6. lr(c) 1' b~.-t"'. How.ev.t1, otf J..e..f f\.,s.f"-t".fl.er ~,., ft,e. S"'rfi'-e., f~ll c_,..,._~... fv... h'b... ;)Y"~c~,'eA+ )ec.rt.~t~j A V\ r ( ~) = G(., t.., J'l.A~f{ =0 Jy. x::~
7 Extra work can be done here, but clearly indicate which problem you are solving. r'v\(_\ t~+- \l,_t,+ ~ ~ ~ ;~X (d~pfl, i~<~.f-o ~~vite) 0 [So ).c,l( (.:;>.,.dj fiov\5 '. b ~ f l 0 J :::::- l... ' { D 1 C..M... ~ (,.e~ Q..('"Cf { s & t l.1 +if)~ : o = D ~~~f. -?VI_t_ ~ '=- N )~~ t~ ~ 1::> Vlf l)c.) ~ A, e.... x lt..n -+ g e.jrx.jt.."' 4 l:>l. t.., ~ V\t c 0 ') -::: A -t B -+ tf.. I 0 '~ ':: 2. I D (."" 1 -J A;, + B -= - L '(D' (~ A ( \ 0 ( \..J.. ll I 1 -~ c1 1 ~ 3 uvir' QO J - 0 -t D 1'6) 1 1. o C.!'-) -= 7 fo c.,.., [3;:.0 A = - L [ Gflrl
8 Extra work can be done here, but clearly indicate which problem you are solving. ~ r\1 :: ):1'; t fa~~~. :: (_o. D l.) 1 V) ( l o o c..~ "l.lv s) :: 2!>1 c."" fs Lrv:: JDw't~~~ = J(2.)'1 c.~/s)( ~ {o.. 10 s) =- 3.2'2.. to~r c.tl-, -;: ,..,.."" J rj ;: tprv V"' -=- t 0~ ~~VJ.t (l." fo...,~ (..)[1 51 "~A)(-2. /D1c., -3) -x!o.~',_r-r't -r 3.22 to ("' e
ECE 3040 Microelectronic Circuits. Exam 1. February 20, 2012
ECE 3040 Microelectronic Circuits Exam 1 February 20, 2012 Dr. W. Alan Doolittle Print your name clearly and largely: 5tJ(u 'f-:()/0 Instructions: Read all the problems carefully and thoroughly before
More informationECE 3040 Microelectronic Circuits
ECE 3040 Microelectronic Circuits Exam 1 February 18, 2013 Dr. W. Alan Doolittle Print your name clearly and largely: Instructions: Read all the problems carefully and thoroughly before you begin working.
More informationECE 3040 Microelectronic Circuits
~ 'o~,1.,,~tl A' ECE 3040 Microelectronic Circuits Exam 1 September 23, 2009 Dr. W. Alan Doolittle Print your name clearly and largely: Instructions: Read all the problems carefully and thoroughly before
More informationESE 372 / Spring 2013 / Lecture 5 Metal Oxide Semiconductor Field Effect Transistor
Metal Oxide Semiconductor Field Effect Transistor V G V G 1 Metal Oxide Semiconductor Field Effect Transistor We will need to understand how this current flows through Si What is electric current? 2 Back
More informationECE 606 Homework Week 7 Mark Lundstrom Purdue University (revised 2/25/13) e E i! E T
ECE 606 Homework Week 7 Mark Lundstrom Purdue University (revised 2/25/13) 1) Consider an n- type semiconductor for which the only states in the bandgap are donor levels (i.e. ( E T = E D ). Begin with
More information1 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 informationDepartment of Electrical and Computer Engineering, Cornell University. ECE 3150: Microelectronics. Spring Exam 1 ` March 22, 2018
Department of Electrical and Computer Engineering, Cornell University ECE 3150: Microelectronics Spring 2018 Exam 1 ` March 22, 2018 INSTRUCTIONS: Every problem must be done in the separate booklet Only
More informationEECS130 Integrated Circuit Devices
EECS130 Integrated Circuit Devices Professor Ali Javey 8/30/2007 Semiconductor Fundamentals Lecture 2 Read: Chapters 1 and 2 Last Lecture: Energy Band Diagram Conduction band E c E g Band gap E v Valence
More informationECE-305: Fall 2016 Minority Carrier Diffusion Equation (MCDE)
ECE-305: Fall 2016 Minority Carrier Diffusion Equation (MCDE) Professor Peter Bermel Electrical and Computer Engineering Purdue University, West Lafayette, IN USA pbermel@purdue.edu Pierret, Semiconductor
More informationSemiconductor 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 informationChapter 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 informationReview of Semiconductor Fundamentals
ECE 541/ME 541 Microelectronic Fabrication Techniques Review of Semiconductor Fundamentals Zheng Yang (ERF 3017, email: yangzhen@uic.edu) Page 1 Semiconductor A semiconductor is an almost insulating material,
More information6.012 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 informationFundamentals of the Metal Oxide Semiconductor Field-Effect Transistor
Triode Working FET Fundamentals of the Metal Oxide Semiconductor Field-Effect Transistor The characteristics of energy bands as a function of applied voltage. Surface inversion. The expression for the
More informationThe German University in Cairo. Faculty of Information Engineering & Technology Semiconductors (Elct 503) Electronics Department Fall 2014
The German University in Cairo th Electronics 5 Semester Faculty of Information Engineering & Technology Semiconductors (Elct 503) Electronics Department Fall 2014 Problem Set 3 1- a) Find the resistivity
More informationCarriers Concentration and Current in Semiconductors
Carriers Concentration and Current in Semiconductors Carrier Transport Two driving forces for carrier transport: electric field and spatial variation of the carrier concentration. Both driving forces lead
More informationsmal band gap Saturday, April 9, 2011
small band gap upper (conduction) band empty small gap valence band filled 2s 2p 2s 2p hybrid (s+p)band 2p no gap 2s (depend on the crystallographic orientation) extrinsic semiconductor semi-metal electron
More informationSpring 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 informationEE3901 A2001. Semiconductor Devices. Exam 1
Name ECE Box # Problem Score Points 1 10 2 30 3 35 4 25 EE3901 A2001 Semiconductor Devices Exam 1 This is a closed book test! You are allowed one sheet (both sides) of notes. Note: Potentially useful reference
More informationCharge Carriers in Semiconductor
Charge Carriers in Semiconductor To understand PN junction s IV characteristics, it is important to understand charge carriers behavior in solids, how to modify carrier densities, and different mechanisms
More informationConsider 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 informationSOLUTIONS: ECE 606 Exam 2: Spring 2013 February 14, 2013 Mark Lundstrom Purdue University
NAME: PUID: : SOLUIONS: ECE 66 Exam : February 14, 13 Mark Lundstrom Purdue University his is a closed book exam. You may use a calculator and the formula sheet at the end of this exam. here are four equally
More informationSemiconductor Physics
Semiconductor Physics Motivation Is it possible that there might be current flowing in a conductor (or a semiconductor) even when there is no potential difference supplied across its ends? Look at the
More informationECE 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 informationEE 346: Semiconductor Devices. 02/08/2017 Tewodros A. Zewde 1
EE 346: Semiconductor Devices 02/08/2017 Tewodros A. Zewde 1 DOPANT ATOMS AND ENERGY LEVELS Without help the total number of carriers (electrons and holes) is limited to 2ni. For most materials, this is
More informationUNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences. Midterm I
UNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences EECS 130 Fall 2006 Professor Ali Javey Midterm I Name: 1. Closed book. One sheet of notes is allowed.
More informationRecitation 2: Equilibrium Electron and Hole Concentration from Doping
Recitation : Equilibrium Electron and Hole Concentration from Doping Here is a list of new things we learned yesterday: 1. Electrons and Holes. Generation and Recombination 3. Thermal Equilibrium 4. Law
More informationUNIVERSITY 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 informationn 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 informationFYS 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 informationUNIVERSITY 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 informationCLASS 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 informationESE 570: Digital Integrated Circuits and VLSI Fundamentals
ESE 570: Digital Integrated Circuits and VLSI Fundamentals Lec 4: January 23, 2018 MOS Transistor Theory, MOS Model Penn ESE 570 Spring 2018 Khanna Lecture Outline! CMOS Process Enhancements! Semiconductor
More informationLecture 15: Optoelectronic devices: Introduction
Lecture 15: Optoelectronic devices: Introduction Contents 1 Optical absorption 1 1.1 Absorption coefficient....................... 2 2 Optical recombination 5 3 Recombination and carrier lifetime 6 3.1
More informationQuiz #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 informationNote that it is traditional to draw the diagram for semiconductors rotated 90 degrees, i.e. the version on the right above.
5 Semiconductors The nearly free electron model applies equally in the case where the Fermi level lies within a small band gap (semiconductors), as it does when the Fermi level lies within a band (metal)
More informationBasic cell design. Si cell
Basic cell design Si cell 1 Concepts needed to describe photovoltaic device 1. energy bands in semiconductors: from bonds to bands 2. free carriers: holes and electrons, doping 3. electron and hole current:
More informationUNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences. Fall Exam 1
UNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences EECS 143 Fall 2008 Exam 1 Professor Ali Javey Answer Key Name: SID: 1337 Closed book. One sheet
More informationCh. 2: Energy Bands And Charge Carriers In Semiconductors
Ch. 2: Energy Bands And Charge Carriers In Semiconductors Discrete energy levels arise from balance of attraction force between electrons and nucleus and repulsion force between electrons each electron
More informationA semiconductor is an almost insulating material, in which by contamination (doping) positive or negative charge carriers can be introduced.
Semiconductor A semiconductor is an almost insulating material, in which by contamination (doping) positive or negative charge carriers can be introduced. Page 2 Semiconductor materials Page 3 Energy levels
More informationECE 442. Spring, Lecture -2
ECE 442 Power Semiconductor Devices and Integrated circuits Spring, 2006 University of Illinois at Chicago Lecture -2 Semiconductor physics band structures and charge carriers 1. What are the types of
More informationUNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences. Professor Ali Javey. Spring 2009.
UNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences EE143 Professor Ali Javey Spring 2009 Exam 1 Name: SID: Closed book. One sheet of notes is allowed.
More informationSection 12: Intro to Devices
Section 12: Intro to Devices Extensive reading materials on reserve, including Robert F. Pierret, Semiconductor Device Fundamentals Bond Model of Electrons and Holes Si Si Si Si Si Si Si Si Si Silicon
More informationECE 250 Electronic Devices 1. Electronic Device Modeling
ECE 250 Electronic Devices 1 ECE 250 Electronic Device Modeling ECE 250 Electronic Devices 2 Introduction to Semiconductor Physics You should really take a semiconductor device physics course. We can only
More informationChapter 12: Semiconductors
Chapter 12: Semiconductors Bardeen & Shottky January 30, 2017 Contents 1 Band Structure 4 2 Charge Carrier Density in Intrinsic Semiconductors. 6 3 Doping of Semiconductors 12 4 Carrier Densities in Doped
More informationBasic Semiconductor Physics
6 Basic Semiconductor Physics 6.1 Introduction With this chapter we start with the discussion of some important concepts from semiconductor physics, which are required to understand the operation of solar
More informationEE143 Fall 2016 Microfabrication Technologies. Evolution of Devices
EE143 Fall 2016 Microfabrication Technologies Prof. Ming C. Wu wu@eecs.berkeley.edu 511 Sutardja Dai Hall (SDH) 1-1 Evolution of Devices Yesterday s Transistor (1947) Today s Transistor (2006) 1-2 1 Why
More informationSection 12: Intro to Devices
Section 12: Intro to Devices Extensive reading materials on reserve, including Robert F. Pierret, Semiconductor Device Fundamentals EE143 Ali Javey Bond Model of Electrons and Holes Si Si Si Si Si Si Si
More informationSession 5: Solid State Physics. Charge Mobility Drift Diffusion Recombination-Generation
Session 5: Solid State Physics Charge Mobility Drift Diffusion Recombination-Generation 1 Outline A B C D E F G H I J 2 Mobile Charge Carriers in Semiconductors Three primary types of carrier action occur
More informationSemiconductor 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 informationElectronics The basics of semiconductor physics
Electronics The basics of semiconductor physics Prof. Márta Rencz, Gergely Nagy BME DED September 16, 2013 The basic properties of semiconductors Semiconductors conductance is between that of conductors
More informationUNIVERSITY 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 informationLecture 1. OUTLINE Basic Semiconductor Physics. Reading: Chapter 2.1. Semiconductors Intrinsic (undoped) silicon Doping Carrier concentrations
Lecture 1 OUTLINE Basic Semiconductor Physics Semiconductors Intrinsic (undoped) silicon Doping Carrier concentrations Reading: Chapter 2.1 EE105 Fall 2007 Lecture 1, Slide 1 What is a Semiconductor? Low
More informationLecture 04 Review of MOSFET
ECE 541/ME 541 Microelectronic Fabrication Techniques Lecture 04 Review of MOSFET Zheng Yang (ERF 3017, email: yangzhen@uic.edu) What is a Transistor? A Switch! An MOS Transistor V GS V T V GS S Ron D
More informationChemistry Instrumental Analysis Lecture 8. Chem 4631
Chemistry 4631 Instrumental Analysis Lecture 8 UV to IR Components of Optical Basic components of spectroscopic instruments: stable source of radiant energy transparent container to hold sample device
More informationFor 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 informationESE 570: Digital Integrated Circuits and VLSI Fundamentals
ESE 570: Digital Integrated Circuits and VLSI Fundamentals Lec 4: January 29, 2019 MOS Transistor Theory, MOS Model Penn ESE 570 Spring 2019 Khanna Lecture Outline! CMOS Process Enhancements! Semiconductor
More informationMath 310 Introduction to Ordinary Differential Equations Final Examination August 9, Instructor: John Stockie
Make sure this exam has 15 pages. Math 310 Introduction to Ordinary Differential Equations inal Examination August 9, 2006 Instructor: John Stockie Name: (Please Print) Student Number: Special Instructions
More information( )! 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 informationcollisions 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 informationEE 446/646 Photovoltaic Devices I. Y. Baghzouz
EE 446/646 Photovoltaic Devices I Y. Baghzouz What is Photovoltaics? First used in about 1890, the word has two parts: photo, derived from the Greek word for light, volt, relating to electricity pioneer
More informationPHOTOVOLTAICS Fundamentals
PHOTOVOLTAICS Fundamentals PV FUNDAMENTALS Semiconductor basics pn junction Solar cell operation Design of silicon solar cell SEMICONDUCTOR BASICS Allowed energy bands Valence and conduction band Fermi
More informationDue to the quantum nature of electrons, one energy state can be occupied only by one electron.
In crystalline solids, not all values of the electron energy are possible. The allowed intervals of energy are called allowed bands (shown as blue and chess-board blue). The forbidden intervals are called
More informationECE 340 Lecture 21 : P-N Junction II Class Outline:
ECE 340 Lecture 21 : P-N Junction II Class Outline: Contact Potential Equilibrium Fermi Levels Things you should know when you leave Key Questions What is the contact potential? Where does the transition
More informationThe Semiconductor in Equilibrium
Lecture 6 Semiconductor physics IV The Semiconductor in Equilibrium Equilibrium, or thermal equilibrium No external forces such as voltages, electric fields. Magnetic fields, or temperature gradients are
More informationPN 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 informationSemiconductor Physics. Lecture 3
Semiconductor Physics Lecture 3 Intrinsic carrier density Intrinsic carrier density Law of mass action Valid also if we add an impurity which either donates extra electrons or holes the number of carriers
More informationSilicon. tetrahedron diamond structure
Silicon a tetrahedron a a diamond structure Tetrahedral bonding Hund s Rule 14Si [e] 3s 3p [e] hybridize 3sp 3 Hybridized level has higher energy for an isolated atom, but allows overall reduction in energy
More informationThe 5 basic equations of semiconductor device physics: We will in general be faced with finding 5 quantities:
6.012 - Electronic Devices and Circuits Solving the 5 basic equations - 2/12/08 Version The 5 basic equations of semiconductor device physics: We will in general be faced with finding 5 quantities: n(x,t),
More informationCarrier Recombination
Notes for ECE-606: Spring 013 Carrier Recombination Professor Mark Lundstrom Electrical and Computer Engineering Purdue University, West Lafayette, IN USA lundstro@purdue.edu /19/13 1 carrier recombination-generation
More informationECE-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 informationSolid State Device Fundamentals
Solid State Device Fundamentals ES 345 Lecture Course by Alexander M. Zaitsev alexander.zaitsev@csi.cuny.edu Tel: 718 982 2812 Oice 4101b 1 The ree electron model o metals The ree electron model o metals
More informationECE 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 informationL5: Surface Recombination, Continuity Equation & Extended Topics tanford University
L5: Surface Recombination, Continuity Equation & Extended Topics EE 216 : Aneesh Nainani 1 Announcements Project Select topic by Jan 29 (Tuesday) 9 topics, maximum 4 students per topic Quiz Thursday (Jan
More informationLecture 2 Electrons and Holes in Semiconductors
EE 471: Transport Phenomena in Solid State Devices Spring 2018 Lecture 2 Electrons and Holes in Semiconductors Bryan Ackland Department of Electrical and Computer Engineering Stevens Institute of Technology
More informationESE 570: Digital Integrated Circuits and VLSI Fundamentals
ESE 570: Digital Integrated Circuits and VLSI Fundamentals Lec 4: January 24, 2017 MOS Transistor Theory, MOS Model Penn ESE 570 Spring 2017 Khanna Lecture Outline! Semiconductor Physics " Band gaps "
More informationEE 346: Semiconductor Devices
EE 346: Semiconductor Devices Lecture - 6 02/06/2017 Tewodros A. Zewde 1 DENSTY OF STATES FUNCTON Since current is due to the flow of charge, an important step in the process is to determine the number
More informationElectronics EC /2/2012. * In-class exams: 40% 7 th week exam 25% 12 th week exam 15%
Arab Academy for Science, Technology and Maritime Transport Electronics EC 331 Dr. Mohamed Hassan Course Assessment * In-class exams: 40% 7 th week exam 25% 12 th week exam 15% *Tutorial exams and activities:
More informationECE-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 informationThe photovoltaic effect occurs in semiconductors where there are distinct valence and
How a Photovoltaic Cell Works The photovoltaic effect occurs in semiconductors where there are distinct valence and conduction bands. (There are energies at which electrons can not exist within the solid)
More informationPHYS208 p-n junction. January 15, 2010
1 PHYS208 p-n junction January 15, 2010 List of topics (1) Density of states Fermi-Dirac distribution Law of mass action Doped semiconductors Dopinglevel p-n-junctions 1 Intrinsic semiconductors List of
More informationECE 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 informationEECS143 Microfabrication Technology
EECS143 Microfabrication Technology Professor Ali Javey Introduction to Materials Lecture 1 Evolution of Devices Yesterday s Transistor (1947) Today s Transistor (2006) Why Semiconductors? Conductors e.g
More informationECE 340 Lecture 39 : MOS Capacitor II
ECE 340 Lecture 39 : MOS Capacitor II Class Outline: Effects of Real Surfaces Threshold Voltage MOS Capacitance-Voltage Analysis Things you should know when you leave Key Questions What are the effects
More informationChapter 1 Semiconductor basics
Chapter 1 Semiconductor basics ELEC-H402/CH1: Semiconductor basics 1 Basic semiconductor concepts Semiconductor basics Semiconductors, silicon and hole-electron pair Intrinsic silicon properties Doped
More informationLecture 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 informationStanford University MatSci 152: Principles of Electronic Materials and Devices Spring Quarter, Final Exam, June 8, 2010
Stanford University MatSci 152: Principles of Electronic Materials and Devices Spring Quarter, 2009-2010 Final Exam, June 8, 2010 This is a closed book, closed notes exam. You are allowed two double-sided
More informationKATIHAL 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 informationAtoms? All matters on earth made of atoms (made up of elements or combination of elements).
Chapter 1 Atoms? All matters on earth made of atoms (made up of elements or combination of elements). Atomic Structure Atom is the smallest particle of an element that can exist in a stable or independent
More informationEE301 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 informationCarrier Mobility and Hall Effect. Prof.P. Ravindran, Department of Physics, Central University of Tamil Nadu, India
Carrier Mobility and Hall Effect 1 Prof.P. Ravindran, Department of Physics, Central University of Tamil Nadu, India http://folk.uio.no/ravi/semi2013 calculation Calculate the hole and electron densities
More information3. 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 informationElectrons are shared in covalent bonds between atoms of Si. A bound electron has the lowest energy state.
Photovoltaics Basic Steps the generation of light-generated carriers; the collection of the light-generated carriers to generate a current; the generation of a large voltage across the solar cell; and
More informationSemiconductor 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 informationBasic 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 information4. I-V characteristics of electric
KL 4. - characteristics of electric conductors 4.1 ntroduction f an electric conductor is connected to a voltage source with voltage a current is produced. We define resistance being the ratio of the voltage
More informationFirst-Hand Investigation: Modeling of Semiconductors
perform an investigation to model the behaviour of semiconductors, including the creation of a hole or positive charge on the atom that has lost the electron and the movement of electrons and holes in
More informationIn this block the two transport mechanisms will be discussed: diffusion and drift.
ET3034TUx - 2.3.3 Transport of charge carriers What are the charge carrier transport principles? In this block the two transport mechanisms will be discussed: diffusion and drift. We will discuss that
More information! CMOS Process Enhancements. ! Semiconductor Physics. " Band gaps. " Field Effects. ! MOS Physics. " Cut-off. " Depletion.
ESE 570: Digital Integrated Circuits and VLSI Fundamentals Lec 4: January 9, 019 MOS Transistor Theory, MOS Model Lecture Outline CMOS Process Enhancements Semiconductor Physics Band gaps Field Effects
More informationSample 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