3.46 PHOTONIC MATERIALS AND DEVICES Lecture 15: III-V Processing
|
|
- Camron Anthony
- 5 years ago
- Views:
Transcription
1 3.46 PHOTONIC MATERIALS AND DEVICES 15: III-V Processing Double Hetero structure laser (band structure engineering) AlGaAs GaAs AlGaAs e - E n hν P h + X n x I d < 1 μm 1. Large refractive index active region 2. Low E active region g η d is increased faster inversion for same injection current light concentrated for stimulated emission light (guided) confinement carrier (electron and hole) confinement 100 of J th Confinement Γ DH SQW SCH Γ=1 Γ Δ nd 2 Γ Δ nd DH: Double Heterostructure SQW: Single Quantum Well SCH: Separate Confinement Heterostructure 3.46 Photonic Materials and Devices 15: III-V Processing Prof. Lionel C. Kimerling Page 1 of 11
2 DH g g p n as d th g( ν) f g ( ν) ρ bulk ( ν) n th g p : peak gain SQW g g p higher T stability g( ν) f g ( ν) ρ QW ( ν) n th ρ(e) Density of States of QW ) QW 2 ρν) ( = states / cm for de = kt 2m r = d E 1 E 2 E 3 E λ 2 m r g P threshhold 2 hd g τ r multilevel gain Threshhold current density R th = threshold recombination rate J th = er th Cnp R cm 3 s 1 ( cm 3 ) 2 = cm s J th = R th 6.4 ka cm -2 μm l w d 3 1 J th decreases with d 3.46 Photonic Materials and Devices 15: III-V Processing Prof. Lionel C. Kimerling Page 2 of 11
3 DH: d 0.2 μm J th = 1.2 ka/cm 2 I th ma d < 300 Å SQW: Jth < 180 A/cm 2 SQW 1. E levels quantized QW transitions 2. ρν P ν ( )(2D) more efficient, g = const ( ) 3. g saturates 2 4. QW states/cm 2 DH states/cm in d = 1000Å 5. Confinement optimized by separation SCH Strained Layers Strain (compressive) raises the LH sub band reduces carriers to invert J th η d C V d<300å with band filling, transition g p are useless (a) 3.46 Photonic Materials and Devices 15: III-V Processing Prof. Lionel C. Kimerling Page 3 of 11
4 III-V Compound Semiconductor Processing 1. Substrate Preparation GaAs, InP 2. Epitaxial layer growth LPE, MBE, MOCVD, CVD 3. Etch Dry (RIE), wet 4. Contacts Au, silicides, metals 1. Process Constraints A. CSBH laser provides (CSBH: Channeled-Substrate Buried Heterostructure) lateral optical and electrical confinement. i. grow InP:Fe SI layer ii. iii. etch channel grow InP/InGaAsP/InP DH in channel B. APD detector (SAM) i. grow InGaAs/InP het. ii. SiNx dielectric deposition iii. etch contact window iv. diffuse p+ contact/junction v. implant p- guard ring Both devices employ deposited dielectrics for AR coatings (APD) and facet reflectors (laser). 2. Issues A. Groups V volatility i. incongruent vaporization of P from T > 360 C ii. as from T > 600 C Solution: group V overpressure or stable dielectric cap layer. iii. RIE creates group III rich suffice Solution: lower T, lower E, high Z (Z: atomic number) 3.46 Photonic Materials and Devices 15: III-V Processing Prof. Lionel C. Kimerling Page 4 of 11
5 B. Preferential etch of V groove Solution: surface prep. C. Metallization reactions Solution: barriers or stable phases D. Degradation of η i Solution: defect control, life testing 3. Epitaxial Growth A. Dislocation density B. Stoichiometry Concept: Substrate: Single crystal film bonded to a single crystal substrate with a common interface and the lattice of the film having a definite orientation w.r.t. the substrate lattice. semi infinite thickness Surface: atomically flat (ledges) (bond reconstruction) Film: homogeneous, 2D (x, y >> t) (phase separation?) Interface: sharp (interdiffusion) Tangential forces: sinusoidal in a 0 Growth Modes E fs = film/substrate bond strength E ff = film/film bond strength W = E fs = relative strength of bonds to E ff substrate a a η=lattice misfit = s f a f a 0 Si(100) 2 1 or GaAs(100) rows of AS V-termination flat surface 3.46 Photonic Materials and Devices 15: III-V Processing Prof. Lionel C. Kimerling Page 5 of 11
6 Epitaxy equilibrium: low deposition rate high T (surface diffusion) ΔG (system energy) minimize N f (film atoms) Coherency (dislocations) variables: a, E ff, h 2. minimize energy E = 2 Bh Film thickness strain elastic constant Coherent: η= (strained) Incoherent: η= +δ (relaxed) Frank-Vander Merwe 1D harmonic chain δ=strain relief by dislocations separation of parallel misfit dislocations: b S = δ 1 η (relaxed) = + b cos λ S projection of b on plane of interface Critical h c minimize E vs. E dislocation Matthews Blakelee b h h = ln c +1 c 8 πη (1+ υ) b h c b 4η 10 4 b 1 Å h = 100 h c of η=10 (Å) c Å η% 3.46 Photonic Materials and Devices 15: III-V Processing Prof. Lionel C. Kimerling Page 6 of 11
7 Morphology (wetting) μ = f G N ML: monolayers Nucleation barrier to clustering γ 3 c/ v ΔG* = 8π 3 ρ 2 Δ η F( ) 2 0 density of unstrained film Deposition w = 1 μ 0 1 monolayer coverage G μ 1 2 f-f clustering G w = 2 μ 1 2 layer growth G Stronski-Kranstanov: G after one monolayer Volmer-Weber: G initially (no wetting) F( ) Δ η 2 η N* = 3 16πγ c/v [Δ η)] F( ρ 0 I N Γexp ( ΔG*/RT) = s Morphology + Coherency are determined by nucleation barriers ΔG* for dislocation formation clustering Metastability is common 3.46 Photonic Materials and Devices 15: III-V Processing Prof. Lionel C. Kimerling Page 7 of 11
8 4. Contacts stable selective low R c low T deposition adhesion Eutectics Au(Be) P Au(Ge) n small process window o RTA unreliable R < 10 c for lasers 5 Ω cm 2 surface defects pin E F contact resistance (Schottky Barrier) for n-gaas p-inp heavily doped epilayer under contact Silicides Stable o undefined interface R c Metals reactive with compounds defects, dissociation phase stability 3.46 Photonic Materials and Devices 15: III-V Processing Prof. Lionel C. Kimerling Page 8 of 11
9 AB dominant 500 C Ga MA x dominant MB y AB MB y dominant TiGa 4 Ti 500 C MB y TiGa 3 TiAs As No phase dominant 300 C PtAs 2 PtGa 3 PtAs 2 + PtGa GaAs 3.46 Photonic Materials and Devices 15: III-V Processing Prof. Lionel C. Kimerling Page 9 of 11
10 NiP (conductor) In 3.46 Photonic Materials and Devices 15: III-V Processing Prof. Lionel C. Kimerling Page 10 of 11
11 Adhesion: local structural relaxation ion beam mixing chemical bonding (Cu / Al 2 O 3 with excess 2 ) Interdiffusion Polycrystal: grain boundary diffusion 3E a D bulk = E a D disloc 4 D bulk (T MP ) D gb 1 TMP 2 E a Dgb 2 D= D bulk + f gb Diffusion Barrier (Ti/Pt)Au o high T MP o chemically stable Intermetallic Compound Coherent Interface refractory TM: Cr, Ni, Ta, Ti, Hf Dielectric Deposition SiO 2, SiO x N y, SiN x sputter PECVD e-beam facets, isolation, diffusion masks Etch Wet etch (Br:CH 3 OH, HCl) o layer stop H 2 SO 4 : H 2 O 2 : H 2 O o v-groove Dry etch (CF 2 Cl 2 ), (HBr, HI) o Anisotropy o Photoelectrochemical etch anisotropy 3.46 Photonic Materials and Devices 15: III-V Processing Prof. Lionel C. Kimerling Page 11 of 11
Stimulated Emission Devices: LASERS
Stimulated Emission Devices: LASERS 1. Stimulated Emission and Photon Amplification E 2 E 2 E 2 hυ hυ hυ In hυ Out hυ E 1 E 1 E 1 (a) Absorption (b) Spontaneous emission (c) Stimulated emission The Principle
More informationOPTI510R: 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 informationPhysics and Material Science of Semiconductor Nanostructures
Physics and Material Science of Semiconductor Nanostructures PHYS 570P Prof. Oana Malis Email: omalis@purdue.edu Course website: http://www.physics.purdue.edu/academic_programs/courses/phys570p/ Lecture
More information(b) Spontaneous emission. Absorption, spontaneous (random photon) emission and stimulated emission.
Lecture 10 Stimulated Emission Devices Lasers Stimulated emission and light amplification Einstein coefficients Optical fiber amplifiers Gas laser and He-Ne Laser The output spectrum of a gas laser Laser
More informationSegmented 1.55um Laser with 400% Differential Quantum Efficiency J. Getty, E. Skogen, L. Coldren, University of California, Santa Barbara, CA.
Segmented 1.55um Laser with 400% Differential Quantum Efficiency J. Getty, E. Skogen, L. Coldren, University of California, Santa Barbara, CA. Abstract: By electrically segmenting, and series-connecting
More informationFabrication Technology, Part I
EEL5225: Principles of MEMS Transducers (Fall 2004) Fabrication Technology, Part I Agenda: Microfabrication Overview Basic semiconductor devices Materials Key processes Oxidation Thin-film Deposition Reading:
More informationChapter 5. Semiconductor Laser
Chapter 5 Semiconductor Laser 5.0 Introduction Laser is an acronym for light amplification by stimulated emission of radiation. Albert Einstein in 1917 showed that the process of stimulated emission must
More informationSelf-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 informationIntroduction 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 informationρ ρ LED access resistances d A W d s n s p p p W the output window size p-layer d p series access resistance d n n-layer series access resistance
LED access resistances W the output window size p-layer series access resistance d p n-layer series access resistance d n The n-layer series access resistance R = ρ s n where the resistivity of the n-layer
More informationHigh Power Diode Lasers
Lecture 10/1 High Power Diode Lasers Low Power Lasers (below tenth of mw) - Laser as a telecom transmitter; - Laser as a spectroscopic sensor; - Laser as a medical diagnostic tool; - Laser as a write-read
More informationLaser Diodes. Revised: 3/14/14 14: , Henry Zmuda Set 6a Laser Diodes 1
Laser Diodes Revised: 3/14/14 14:03 2014, Henry Zmuda Set 6a Laser Diodes 1 Semiconductor Lasers The simplest laser of all. 2014, Henry Zmuda Set 6a Laser Diodes 2 Semiconductor Lasers 1. Homojunction
More informationOPTI510R: 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 #6 is assigned, due April 23 rd Final exam May 2 Semiconductor
More information3-1-2 GaSb Quantum Cascade Laser
3-1-2 GaSb Quantum Cascade Laser A terahertz quantum cascade laser (THz-QCL) using a resonant longitudinal optical (LO) phonon depopulation scheme was successfully demonstrated from a GaSb/AlSb material
More informationLecture 10 Thin Film Growth
Lecture 10 Thin Film Growth 1/76 Announcements Homework: Homework Number 2 is returned today, please pick it up from me at the end of the class. Solutions are online. Homework 3 will be set Thursday (2
More informationCVD: General considerations.
CVD: General considerations. PVD: Move material from bulk to thin film form. Limited primarily to metals or simple materials. Limited by thermal stability/vapor pressure considerations. Typically requires
More informationGeSi Quantum Dot Superlattices
GeSi Quantum Dot Superlattices ECE440 Nanoelectronics Zheng Yang Department of Electrical & Computer Engineering University of Illinois at Chicago Nanostructures & Dimensionality Bulk Quantum Walls Quantum
More informationOptical Spectroscopies of Thin Films and Interfaces. Dietrich R. T. Zahn Institut für Physik, Technische Universität Chemnitz, Germany
Optical Spectroscopies of Thin Films and Interfaces Dietrich R. T. Zahn Institut für Physik, Technische Universität Chemnitz, Germany 1. Introduction 2. Vibrational Spectroscopies (Raman and Infrared)
More informationLaser Basics. What happens when light (or photon) interact with a matter? Assume photon energy is compatible with energy transition levels.
What happens when light (or photon) interact with a matter? Assume photon energy is compatible with energy transition levels. Electron energy levels in an hydrogen atom n=5 n=4 - + n=3 n=2 13.6 = [ev]
More informationinterband transitions in semiconductors M. Fox, Optical Properties of Solids, Oxford Master Series in Condensed Matter Physics
interband transitions in semiconductors M. Fox, Optical Properties of Solids, Oxford Master Series in Condensed Matter Physics interband transitions in quantum wells Atomic wavefunction of carriers in
More informationPHYSICAL 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 information1300nm-Range GaInNAs-Based Quantum Well Lasers with High Characteristic Temperature
3nm-Range GaInNAs-Based Quantum Well Lasers with High Characteristic Temperature by Hitoshi Shimizu *, Kouji Kumada *, Seiji Uchiyama * and Akihiko Kasukawa * Long wavelength- SQW lasers that include a
More informationPhysics of Semiconductors (Problems for report)
Physics of Semiconductors (Problems for report) Shingo Katsumoto Institute for Solid State Physics, University of Tokyo July, 0 Choose two from the following eight problems and solve them. I. Fundamentals
More informationIntroduction to Optoelectronic Device Simulation by Joachim Piprek
NUSOD 5 Tutorial MA Introduction to Optoelectronic Device Simulation by Joachim Piprek Outline:. Introduction: VCSEL Example. Electron Energy Bands 3. Drift-Diffusion Model 4. Thermal Model 5. Gain/Absorption
More informationSEMICONDUCTOR GROWTH TECHNIQUES. Introduction to growth techniques (bulk, epitaxy) Basic concepts in epitaxy (MBE, MOCVD)
SEMICONDUCTOR GROWTH TECHNIQUES Introduction to growth techniques (bulk, epitaxy) Basic concepts in epitaxy (MBE, MOCVD) Growth Processes Bulk techniques (massive semiconductors, wafers): Si, compounds
More informationEmission Spectra of the typical DH laser
Emission Spectra of the typical DH laser Emission spectra of a perfect laser above the threshold, the laser may approach near-perfect monochromatic emission with a spectra width in the order of 1 to 10
More informationExternal (differential) quantum efficiency Number of additional photons emitted / number of additional electrons injected
Semiconductor Lasers Comparison with LEDs The light emitted by a laser is generally more directional, more intense and has a narrower frequency distribution than light from an LED. The external efficiency
More informationQuantum Dot Lasers. Andrea Fiore. Ecole Polytechnique Fédérale de Lausanne
Quantum Dot Lasers Ecole Polytechnique Fédérale de Lausanne Outline: Quantum-confined active regions Self-assembled quantum dots Laser applications Electronic states in semiconductors Schrödinger eq.:
More informationSolid Surfaces, Interfaces and Thin Films
Hans Lüth Solid Surfaces, Interfaces and Thin Films Fifth Edition With 427 Figures.2e Springer Contents 1 Surface and Interface Physics: Its Definition and Importance... 1 Panel I: Ultrahigh Vacuum (UHV)
More informationSemiconductor Lasers for Optical Communication
Semiconductor Lasers for Optical Communication Claudio Coriasso Manager claudio.coriasso@avagotech.com Turin Technology Centre 10Gb/s DFB Laser MQW 1 Outline 1) Background and Motivation Communication
More informationPlasma Deposition (Overview) Lecture 1
Plasma Deposition (Overview) Lecture 1 Material Processes Plasma Processing Plasma-assisted Deposition Implantation Surface Modification Development of Plasma-based processing Microelectronics needs (fabrication
More informationPHYSICAL 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 informationPaper Review. Special Topics in Optical Engineering II (15/1) Minkyu Kim. IEEE Journal of Quantum Electronics, Feb 1985
Paper Review IEEE Journal of Quantum Electronics, Feb 1985 Contents Semiconductor laser review High speed semiconductor laser Parasitic elements limitations Intermodulation products Intensity noise Large
More informationOPTI510R: 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 Homework #6 is assigned, due May 1 st Final exam May 8, 10:30-12:30pm
More informationLecture 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 informationIntroduction 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 informationTMT4320 Nanomaterials November 10 th, Thin films by physical/chemical methods (From chapter 24 and 25)
1 TMT4320 Nanomaterials November 10 th, 2015 Thin films by physical/chemical methods (From chapter 24 and 25) 2 Thin films by physical/chemical methods Vapor-phase growth (compared to liquid-phase growth)
More informationPerformance Enhancement of P-channel InGaAs Quantum-well FETs by Superposition of Process-induced Uniaxial Strain and Epitaxially-grown Biaxial Strain
Performance Enhancement of P-channel InGaAs Quantum-well FETs by Superposition of Process-induced Uniaxial Strain and Epitaxially-grown Biaxial Strain Ling Xia 1, Vadim Tokranov 2, Serge R. Oktyabrsky
More informationJOHN G. EKERDT RESEARCH FOCUS
JOHN G. EKERDT RESEARCH FOCUS We study the surface, growth and materials chemistry of metal, dielectric, ferroelectric, and polymer thin films. We seek to understand and describe nucleation and growth
More informationMetal Vapour Lasers Use vapoured metal as a gain medium Developed by W. Silfvast (1966) Two types: Ionized Metal vapour (He-Cd) Neutral Metal vapour
Metal Vapour Lasers Use vapoured metal as a gain medium Developed by W. Silfvast (1966) Two types: Ionized Metal vapour (He-Cd) Neutral Metal vapour (Cu) All operate by vaporizing metal in container Helium
More informationInfluence of Size on the Properties of Materials
Influence of Size on the Properties of Materials M. J. O Shea Kansas State University mjoshea@phys.ksu.edu If you cannot get the papers connected to this work, please e-mail me for a copy 1. General Introduction
More information3.155J/6.152J Microelectronic Processing Technology Fall Term, 2004
3.155J/6.152J Microelectronic Processing Technology Fall Term, 2004 Bob O'Handley Martin Schmidt Quiz Nov. 17, 2004 Ion implantation, diffusion [15] 1. a) Two identical p-type Si wafers (N a = 10 17 cm
More informationSemiconductor Disk Laser on Microchannel Cooler
Semiconductor Disk Laser on Microchannel Cooler Eckart Gerster An optically pumped semiconductor disk laser with a double-band Bragg reflector mirror is presented. This mirror not only reflects the laser
More information1. Binary III-V compounds 2 p From which atoms are the 16 binary III-V compounds formed?...column III B, Al, Ga and In...column V N, P, As and Sb...
PROBLEMS part B, Semiconductor Materials. 2006 1. Binary III-V compounds 2 p From which atoms are the 16 binary III-V compounds formed?...column III B, Al, Ga and In...column V N, P, As and Sb... 2. Semiconductors
More informationSelf-Assembled InAs Quantum Dots
Self-Assembled InAs Quantum Dots Steve Lyon Department of Electrical Engineering What are semiconductors What are semiconductor quantum dots How do we make (grow) InAs dots What are some of the properties
More informationHigh characteristic temperature of 1.3 #m crescent buried heterostructure laser diodes
Bull. Mater. Sci., Vol. 11, No. 4, December 1988, pp. 291 295. Printed in India. High characteristic temperature of 1.3 #m crescent buried heterostructure laser diodes Y K SU and T L CHEN Institute of
More informationFilm Deposition Part 1
1 Film Deposition Part 1 Chapter 11 : Semiconductor Manufacturing Technology by M. Quirk & J. Serda Spring Semester 2013 Saroj Kumar Patra Semidonductor Manufacturing Technology, Norwegian University of
More informationQuantum Dot Lasers. Jose Mayen ECE 355
Quantum Dot Lasers Jose Mayen ECE 355 Overview of Presentation Quantum Dots Operation Principles Fabrication of Q-dot lasers Advantages over other lasers Characteristics of Q-dot laser Types of Q-dot lasers
More informationPhotovoltaic cell and module physics and technology. Vitezslav Benda, Prof Czech Technical University in Prague
Photovoltaic cell and module physics and technology Vitezslav Benda, Prof Czech Technical University in Prague benda@fel.cvut.cz www.fel.cvut.cz 1 Outlines Photovoltaic Effect Photovoltaic cell structure
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 informationPhysics of Semiconductors
Physics of Semiconductors 9 th 2016.6.13 Shingo Katsumoto Department of Physics and Institute for Solid State Physics University of Tokyo Site for uploading answer sheet Outline today Answer to the question
More informationPlan for Lectures #4, 5, & 6. Theme Of Lectures: Nano-Fabrication
Plan for Lectures #4, 5, & 6 Theme Of Lectures: Nano-Fabrication Quantum Wells, SLs, Epitaxial Quantum Dots Carbon Nanotubes, Semiconductor Nanowires Self-assembly and Self-organization Two Approaches
More informationLecture 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 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 informationSemiconductor Integrated Process Design (MS 635)
Semiconductor Integrated Process Design (MS 635) Instructor: Prof. Keon Jae Lee - Office: 응용공학동 #4306, Tel: #3343 - Email: keonlee@kaist.ac.kr Lecture: (Tu, Th), 1:00-2:15 #2425 Office hour: Tues & Thur
More informationStructural and Optical Properties of III-III-V-N Type
i Structural and Optical Properties of III-III-V-N Type Alloy Films and Their Quantum Wells ( III-III-V- N 型混晶薄膜および量子井戸の構造的および光学的性質 ) This dissertation is submitted as a partial fulfillment of the requirements
More informationELECTRONIC 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 informationEE 6313 Homework Assignments
EE 6313 Homework Assignments 1. Homework I: Chapter 1: 1.2, 1.5, 1.7, 1.10, 1.12 [Lattice constant only] (Due Sept. 1, 2009). 2. Homework II: Chapter 1, 2: 1.17, 2.1 (a, c) (k = π/a at zone edge), 2.3
More informationModern Methods in Heterogeneous Catalysis Research: Preparation of Model Systems by Physical Methods
Modern Methods in Heterogeneous Catalysis Research: Preparation of Model Systems by Physical Methods Methods for catalyst preparation Methods discussed in this lecture Physical vapour deposition - PLD
More informationPhotodetector Basics
Photodetection: Absorption => Current Generation hυ Currents Materials for photodetection: t ti E g
More informationSaroj P. Dash. Chalmers University of Technology. Göteborg, Sweden. Microtechnology and Nanoscience-MC2
Silicon Spintronics Saroj P. Dash Chalmers University of Technology Microtechnology and Nanoscience-MC2 Göteborg, Sweden Acknowledgement Nth Netherlands University of Technology Sweden Mr. A. Dankert Dr.
More informationBlue-green Emitting Semiconductor Disk Lasers with Intra-Cavity Frequency Doubling
Blue-green Emitting Semiconductor Disk Lasers with Intra-Cavity Frequency Doubling Eckart Schiehlen and Michael Riedl Diode-pumped semiconductor disk lasers, also referred to as VECSEL (Vertical External
More informationThermal and electronic analysis of GaInAs/AlInAs mid-ir
Thermal and electronic analysis of GaInAs/AlInAs mid-ir QCLs Gaetano Scamarcio Miriam S. Vitiello, Vincenzo Spagnolo, Antonia Lops oratory LIT 3, CNR - INFM Physics Dept.,University of Bari, Italy T. Gresch,
More informationLecture 0: Introduction
Lecture 0: Introduction Introduction q Integrated circuits: many transistors on one chip q Very Large Scale Integration (VLSI): bucketloads! q Complementary Metal Oxide Semiconductor Fast, cheap, low power
More informationWide Bandgap Semiconductor Research at Mississippi State University
Wide Bandgap Semiconductor Research at Mississippi State University Dr. Yaroslav Koshka Associate Professor Department of Electrical and Computer Engineering Mississippi State University Presentation Outline
More informationLecture 6 Plasmas. Chapters 10 &16 Wolf and Tauber. ECE611 / CHE611 Electronic Materials Processing Fall John Labram 1/68
Lecture 6 Plasmas Chapters 10 &16 Wolf and Tauber 1/68 Announcements Homework: Homework will be returned to you on Thursday (12 th October). Solutions will be also posted online on Thursday (12 th October)
More informationInGaAs-AlAsSb quantum cascade lasers
InGaAs-AlAsSb quantum cascade lasers D.G.Revin, L.R.Wilson, E.A.Zibik, R.P.Green, J.W.Cockburn Department of Physics and Astronomy, University of Sheffield, UK M.J.Steer, R.J.Airey EPSRC National Centre
More informationOptical Investigation of the Localization Effect in the Quantum Well Structures
Department of Physics Shahrood University of Technology Optical Investigation of the Localization Effect in the Quantum Well Structures Hamid Haratizadeh hamid.haratizadeh@gmail.com IPM, SCHOOL OF PHYSICS,
More informationMetallic: 2n 1. +n 2. =3q Armchair structure always metallic = 2
Properties of CNT d = 2.46 n 2 2 1 + n1n2 + n2 2π Metallic: 2n 1 +n 2 =3q Armchair structure always metallic a) Graphite Valence(π) and Conduction(π*) states touch at six points(fermi points) Carbon Nanotube:
More informationPractical Quantum-Dot Lasers Monolithically Grown on Silicon for Silicon Photonics
Department of Electronic and Electrical Engineering London Centre for Nanotechnology Practical Quantum-Dot Lasers Monolithically Grown on Silicon for Silicon Photonics Huiyun Liu Outline Why lasers on
More informationLecture 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 informationSignal regeneration - optical amplifiers
Signal regeneration - optical amplifiers In any atom or solid, the state of the electrons can change by: 1) Stimulated absorption - in the presence of a light wave, a photon is absorbed, the electron is
More informationElectron Energy, E E = 0. Free electron. 3s Band 2p Band Overlapping energy bands. 3p 3s 2p 2s. 2s Band. Electrons. 1s ATOM SOLID.
Electron Energy, E Free electron Vacuum level 3p 3s 2p 2s 2s Band 3s Band 2p Band Overlapping energy bands Electrons E = 0 1s ATOM 1s SOLID In a metal the various energy bands overlap to give a single
More informationHeterostructures and sub-bands
Heterostructures and sub-bands (Read Datta 6.1, 6.2; Davies 4.1-4.5) Quantum Wells In a quantum well, electrons are confined in one of three dimensions to exist within a region of length L z. If the barriers
More informationCME 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 informationCVD-3 LFSIN SiN x Process
CVD-3 LFSIN SiN x Process Top Electrode, C Bottom Electrode, C Pump to Base Time (s) SiH 4 Flow Standard LFSIN Process NH 3 Flow N 2 HF (watts) LF (watts) Pressure (mtorr Deposition Time min:s.s Pump to
More informationChapter 3 Basics Semiconductor Devices and Processing
Chapter 3 Basics Semiconductor Devices and Processing Hong Xiao, Ph. D. www2.austin.cc.tx.us/hongxiao/book.htm Hong Xiao, Ph. D. www2.austin.cc.tx.us/hongxiao/book.htm 1 Objectives Identify at least two
More informationCross-Section Scanning Tunneling Microscopy of InAs/GaSb Superlattices
Cross-Section Scanning Tunneling Microscopy of InAs/GaSb Superlattices Cecile Saguy A. Raanan, E. Alagem and R. Brener Solid State Institute. Technion, Israel Institute of Technology, Haifa 32000.Israel
More informationBand Alignment and Graded Heterostructures. Guofu Niu Auburn University
Band Alignment and Graded Heterostructures Guofu Niu Auburn University Outline Concept of electron affinity Types of heterojunction band alignment Band alignment in strained SiGe/Si Cusps and Notches at
More informationLecture contents. Stress and strain Deformation potential. NNSE 618 Lecture #23
1 Lecture contents Stress and strain Deformation potential Few concepts from linear elasticity theory : Stress and Strain 6 independent components 2 Stress = force/area ( 3x3 symmetric tensor! ) ij ji
More informationISSN Review. Progress to a Gallium-Arsenide Deep-Center Laser
Materials 2009, 2, 1599-1635; doi:10.3390/ma2041599 OPEN ACCESS materials ISSN 1996-1944 www.mdpi.com/journal/materials Review Progress to a Gallium-Arsenide Deep-Center Laser Janet L. Pan Yale University,
More information1 Semiconductor Quantum Dots for Ultrafast Optoelectronics
j1 1 Semiconductor Quantum Dots for Ultrafast Optoelectronics 1.1 The Role of Dimensionality in Semiconductor Materials The history of semiconductor lasers has been punctuated by dramatic revolutions.
More informationResonator Fabrication for Cavity Enhanced, Tunable Si/Ge Quantum Cascade Detectors
Resonator Fabrication for Cavity Enhanced, Tunable Si/Ge Quantum Cascade Detectors M. Grydlik 1, P. Rauter 1, T. Fromherz 1, G. Bauer 1, L. Diehl 2, C. Falub 2, G. Dehlinger 2, H. Sigg 2, D. Grützmacher
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 informationDO NOT WRITE YOUR NAME OR KAUST ID NUMBER ON THIS PAGE OR ANY OTHER PAGE PUT YOUR EXAM ID NUMBER ON THIS PAGE AND EVERY OTHER PAGE YOU SUBMIT
DO NOT WRITE YOUR NAME OR KAUST ID NUMBER ON THIS PAGE OR ANY OTHER PAGE PUT YOUR EXAM ID NUMBER ON THIS PAGE AND EVERY OTHER PAGE YOU SUBMIT WRITE YOUR SOLUTIONS ON ONLY ONE SIDE OF EMPTY SOLUTION SHEETS
More informationThree-Dimensional Silicon-Germanium Nanostructures for Light Emitters and On-Chip Optical. Interconnects
Three-Dimensional Silicon-Germanium Nanostructures for Light Emitters and On-Chip Optical eptember 2011 Interconnects Leonid Tsybeskov Department of Electrical and Computer Engineering New Jersey Institute
More informationCHAPTER 6: Etching. Chapter 6 1
Chapter 6 1 CHAPTER 6: Etching Different etching processes are selected depending upon the particular material to be removed. As shown in Figure 6.1, wet chemical processes result in isotropic etching
More informationPhotoluminescence characterization of quantum dot laser epitaxy
Photoluminescence characterization of quantum dot laser epitaxy Y. Li *, Y. C. Xin, H. Su and L. F. Lester Center for High Technology Materials, University of New Mexico 1313 Goddard SE, Albuquerque, NM
More informationMOSFET: Introduction
E&CE 437 Integrated VLSI Systems MOS Transistor 1 of 30 MOSFET: Introduction Metal oxide semiconductor field effect transistor (MOSFET) or MOS is widely used for implementing digital designs Its major
More informationAdvantages / Disadvantages of semiconductor detectors
Advantages / Disadvantages of semiconductor detectors Semiconductor detectors have a high density (compared to gas detector) large energy loss in a short distance diffusion effect is smaller than in gas
More informationLEC E T C U T R U E R E 17 -Photodetectors
LECTURE 17 -Photodetectors Topics to be covered Photodetectors PIN photodiode Avalanche Photodiode Photodetectors Principle of the p-n junction Photodiode A generic photodiode. Photodetectors Principle
More informationEE C245 ME C218 Introduction to MEMS Design Fall 2007
EE C245 ME C218 Introduction to MEMS Design Fall 2007 Prof. Clark T.-C. Nguyen Dept. of Electrical Engineering & Computer Sciences University of California at Berkeley Berkeley, CA 94720 Lecture 4: Film
More information4FNJDPOEVDUPS 'BCSJDBUJPO &UDI
2010.5.4 1 Major Fabrication Steps in CMOS Process Flow UV light oxygen Silicon dioxide Silicon substrate Oxidation (Field oxide) photoresist Photoresist Coating Mask exposed photoresist Mask-Wafer Exposed
More informationSurfaces, Interfaces, and Layered Devices
Surfaces, Interfaces, and Layered Devices Building blocks for nanodevices! W. Pauli: God made solids, but surfaces were the work of Devil. Surfaces and Interfaces 1 Interface between a crystal and vacuum
More informationLecture 150 Basic IC Processes (10/10/01) Page ECE Analog Integrated Circuits and Systems P.E. Allen
Lecture 150 Basic IC Processes (10/10/01) Page 1501 LECTURE 150 BASIC IC PROCESSES (READING: TextSec. 2.2) INTRODUCTION Objective The objective of this presentation is: 1.) Introduce the fabrication of
More informationChapter 7. Solar Cell
Chapter 7 Solar Cell 7.0 Introduction Solar cells are useful for both space and terrestrial application. Solar cells furnish the long duration power supply for satellites. It converts sunlight directly
More informationUltrafast single photon emitting quantum photonic structures. based on a nano-obelisk
Ultrafast single photon emitting quantum photonic structures based on a nano-obelisk Je-Hyung Kim, Young-Ho Ko, Su-Hyun Gong, Suk-Min Ko, Yong-Hoon Cho Department of Physics, Graduate School of Nanoscience
More informationThe first three categories are considered a bottom-up approach while lithography is a topdown
Nanowires and Nanorods One-dimensional structures have been called in different ways: nanowires, nanorod, fibers of fibrils, whiskers, etc. The common characteristic of these structures is that all they
More informationDopant and Self-Diffusion in Semiconductors: A Tutorial
Dopant and Self-Diffusion in Semiconductors: A Tutorial Eugene Haller and Hughes Silvestri MS&E, UCB and LBNL FLCC Tutorial 1/26/04 1 FLCC Outline Motivation Background Fick s Laws Diffusion Mechanisms
More informationQuantum Well and Quantum Dot Intermixing for Optoelectronic Device Integration
Quantum Well and Quantum Dot Intermixing for Optoelectronic Device Integration Chennupati Jagadish Australian National University Research School of Physical Sciences and Engineering, Canberra, ACT 0200
More information