1. A photoresistor is formed from a square 1 cm x 1 cm slab of GaAs. Light of wavelength 830 nm falls onto it at a power density of 1, generating electron-hole.

Slides:



Advertisements
Similar presentations
Chapter 2-4. Equilibrium carrier concentrations
Advertisements

Fig_18_04 fig_18_04.
Semiconductor Device Physics
Lecture #5 OUTLINE Intrinsic Fermi level Determination of E F Degenerately doped semiconductor Carrier properties Carrier drift Read: Sections 2.5, 3.1.
LECTURE- 5 CONTENTS  PHOTOCONDUCTING MATERIALS  CONSTRUCTION OF PHOTOCONDUCTING MATERIALS  APPLICATIONS OF PHOTOCONDUCTING MATERIALS.
Budapest University of Technology and Economics Department of Electron Devices Microelectronics, BSc course Basic semiconductor physics.
PN Junction Diodes.
(Capacitance and capacitors)
EE105 Fall 2007Lecture 3, Slide 1Prof. Liu, UC Berkeley Lecture 3 ANNOUNCEMENTS HW2 is posted, due Tu 9/11 TAs will hold their office hours in 197 Cory.
Department of Aeronautics and Astronautics NCKU Nano and MEMS Technology LAB. 1 Chapter IV June 14, 2015June 14, 2015June 14, 2015 P-n Junction.
EE105 Fall 2007Lecture 1, Slide 1 Lecture 1 OUTLINE Basic Semiconductor Physics – Semiconductors – Intrinsic (undoped) silicon – Doping – Carrier concentrations.
Department of Aeronautics and Astronautics NCKU Nano and MEMS Technology LAB. 1 Chapter I Introduction June 20, 2015June 20, 2015June 20, 2015.
Normalized plot of n 0 /N D as a function of temperature. This plot is for N D = cm  3. Figure
Lecture #8 OUTLINE Generation and recombination Excess carrier concentrations Minority carrier lifetime Read: Section 3.3.
Deviations from simple theory and metal-semiconductor junctions
Ideal Diode Model.
MatE/EE 1671 EE/MatE 167 Diode Review. MatE/EE 1672 Topics to be covered Energy Band Diagrams V built-in Ideal diode equation –Ideality Factor –RS Breakdown.
Dr. Nasim Zafar Electronics 1 EEE 231 – BS Electrical Engineering Fall Semester – 2012 COMSATS Institute of Information Technology Virtual campus Islamabad.
Electron And Hole Equilibrium Concentrations 18 and 20 February 2015  Chapter 4 Topics-Two burning questions: What is the density of states in the conduction.
Electron And Hole Equilibrium Concentrations 24 February 2014  Return and discuss Quiz 2  Chapter 4 Topics-Two burning questions: What is the density.
I. ELECTRICAL CONDUCTION
Chapter 4 Photonic Sources.
Potential vs. Kinetic Energy
Electronic Devices Laboratory CE/EE 3110 Conductivity and the Hall Effect.
ECE 4339 L. Trombetta ECE 4339: Physical Principles of Solid State Devices Len Trombetta Summer 2006 Chapter 3: Carrier Action Goal: To understand what.
ECE 250 – Electronic Devices 1 ECE 250 Electronic Device Modeling.
Basic Electronics By Asst Professor : Dhruba Shankar Ray For B.Sc. Electronics Ist Year 1.
Chapter 5 Junctions. 5.1 Introduction (chapter 3) 5.2 Equilibrium condition Contact potential Equilibrium Fermi level Space charge at.
Network for Computational Nanotechnology (NCN) UC Berkeley, Univ.of Illinois, Norfolk State, Northwestern, Purdue, UTEP First-Time User Guide Drift-Diffusion.
ENE 311 Lecture 9.
EXAMPLE 12.1 OBJECTIVE Solution Comment
Ch 140 Lecture Notes #13 Prepared by David Gleason
Numericals on semiconductors
ECE 340 Lecture 6 Intrinsic Material, Doping, Carrier Concentrations
ECEE 302: Electronic Devices
CHAPTER 3: CARRIER CONCENTRATION PHENOMENA
CHAPTER 3: CARRIER CONCENTRATION PHENOMENA
Lecture 3 OUTLINE Semiconductor Fundamentals (cont’d) – Thermal equilibrium – Fermi-Dirac distribution Boltzmann approximation – Relationship between E.
Introduction to semiconductor technology. Outline –4 Excitation of semiconductors Optical absorption and excitation Luminescence Recombination Diffusion.
The review of modern physics has given us a description of nature. Waves are described with a wave equation. Particles are described with particle equations.
President UniversityErwin SitompulSDP 4/1 Lecture 4 Semiconductor Device Physics Dr.-Ing. Erwin Sitompul President University
Electron and Hole Concentrations in Extrinsic Semiconductor
Introduction to Semiconductor Technology. Outline 3 Energy Bands and Charge Carriers in Semiconductors.
ELECTRONICS II VLSI DESIGN Fall 2013
EXAMPLE 4.1 OBJECTIVE Solution Comment
Solid-State Electronics Chap. 5 Instructor: Pei-Wen Li Dept. of E. E. NCU 1 Chap 5. Carrier Motion  Carrier Drift  Carrier Diffusion  Graded Impurity.
EE105 - Spring 2007 Microelectronic Devices and Circuits
pn Junction Diodes: I-V Characteristics
Chapter 4 Excess Carriers in Semiconductors
Slide 1EE40 Fall 2007Prof. Chang-Hasnain EE40 Lecture 32 Prof. Chang-Hasnain 11/21/07 Reading: Supplementary Reader.
President UniversityErwin SitompulSDP 3/1 Dr.-Ing. Erwin Sitompul President University Lecture 3 Semiconductor Device Physics
Carrier generation and recombination A sudden increase in temperature increases the generation rate. An incident burst of photons increases the generation.
Carrier Motion - Electric Fields ECE Movement of Electrons and Holes Nearly free electrons can easily move in a semiconductor since they are not.
Animation Demonstration No. 2. Interaction of Light with Semiconductors Normally a semiconductor material has only a few thermally excited free electrons.
ספרות עזר : פרופ ' אדיר בר - לב, מוליכים למחצה והתקנים אלקטרוניים, עמ ' P.A. Tipler, Modern Physics, pp Mc Kelvey, Solidstate and Semiconductor.
Issued: May 5, 2010 Due: May 12, 2010 (at the start of class) Suggested reading: Kasap, Chapter 5, Sections Problems: Stanford University MatSci.
Multiple choise questions related to lecture PV2
Lecture 3 OUTLINE Semiconductor Fundamentals (cont’d)
Lecture 3 OUTLINE Semiconductor Fundamentals (cont’d)
P-n Junctions ECE 2204.
3.1.4 Direct and Indirect Semiconductors
Lecture 5 OUTLINE Semiconductor Fundamentals (cont’d)
Lecture #8 OUTLINE Generation and recombination
Chapter 4 Excess Carriers in Semiconductors
Lecture 3 OUTLINE Semiconductor Fundamentals (cont’d)
Review of semiconductor physics
pn Junction Diodes: I-V Characteristics
반도체 기초 이론 Vol. I Semiconductor Fundamentals by R. F
Presentation transcript:

1. A photoresistor is formed from a square 1 cm x 1 cm slab of GaAs. Light of wavelength 830 nm falls onto it at a power density of 1, generating electron-hole pairs of 10 m s lifetime. i) if each incident photon produces one EHP, what is the resistance of the GaAs slab. (Assume the carrier concentration with no light is negligible). ii) Explain whether a similar measurement on a slab of AlSb would yield a similar result. Assignment # 4 Given February 4, 2000 Due February 11, 2000 W/m 2

2. A Hall effect measurement is made on a semiconductor sample with length 0.5 cm, width 0.2 cm, and cross-sectional area of cm 2. With a constant current supply, 0.4 mA flow through the length of the sample. Determine: a)The resistivity of the sample if the potential V x across the length of the sample is 1.0 V. b)The carrier type. A magnetic field of 0.75 T is applied normal to the sample, and a Hall voltage V H = 0.1 V is measured (across the width with polarity as indicated). - see next page -

Question 2 cont’d: c)The carrier concentration. d)The carrier mobility. e)The values of V x and V H if the carrier concentration is doubled. 3. For Si that is very lightly doped with N A =3.7  cm -3, calculate the equilibrium electron and hole concentrations ( n i = 1.5  cm -3, T = 300K ). Find the displacement of the Fermi energy level E F from the band gap position. Note: You can use 4.Problem 3.10, p 93, textbook, 4 th edition