Semiconductor Lasers II

Size: px
Start display at page:

Download "Semiconductor Lasers II"

Transcription

1 Semiconductor Lasers II Materials and Structures Edited by Eli Kapon Institute of Micro and Optoelectronics Department of Physics Swiss Federal Institute oftechnology, Lausanne OPTICS AND PHOTONICS ACADEMIC PRESS San Diego London Boston New York Sydney Tokyo Toronto

2 Contents Preface xi Chapter 1 Visible-Wavelength Laser Diodes 1.1 Introduction Relevance of visible wavelength lasers Thermal aspects; the temperature-dependence of threshold current Beam properties, astigmatism High-power operation Organization of this Chapter Material systems for visible lasers Introduction The InGaAlP material system The MgZnSSe material system The AlInGaN system The chalcopyrites Epitaxial growth and technology The AlGalnP system The MgZnSSe system Introduction MBE OMVPE Ohmic contacts to p-type ZnSe The AlInGaN system OMVPE/MOMBE Processing and contacting Quantum wells and strain in laser diodes The effects of quantum wells The effects of strain 25 v

3 vi Contents 1.5 InGaAlP laser structures Transverse laser structure with bulk InGaP active layer InGaAlP strained layer quantum well lasers Lateral laser structure: gain-guided lasers Electro-optical properties of gain-guided lasers Lateral laser structure: index-guided lasers Electro-optical properties of index-guided lasers High-power operation Laser diode operation at shorter wavelengths ( nm) Temperature dependence of the threshold current Reliability of InGaAlP lasers Short-wavelength visible lasers (blue-green and blue) II VI injection lasers Introduction The use of CdZnSe strained layer quantum wells and quaternary claddings for blue-green II-VI lasers Reliability of II-IV lasers Gallium nitride-based lasers Conclusions and perspectives toward future developments 62 Acknowledgments 63 References 64 Chapter 2 Long Wavelength (A > 2 /лт) Semiconductor Lasers 2.1 Introduction Wavelength ranges of various laser materials Growth techniques Compounds and alloys of III-V type Brief review of III-V materials for longwavelength laser applications Lasers based on III-V materials Type-II heterojunction InGaSbAs/GaSb InSbAsP/InAs and some other lasers Compounds and alloys of II-VI type Brief review of II-VI materials for longwavelength laser applications 100

4 Contents Vll II-VI-based IR semiconductor laser diodes Compounds and alloys of IV-VI type Brief review of IV-VI materials for longwavelength laser applications IV-VI-based IR semiconductor laser diodes; comments on history Homojunction laser diodes of IV-VI type Heterojunction laser diodes of IV-VI type Quantum-well IV-VI lasers Resume of interband laser properties Threshold and power characteristics Mode control and tunability of the laser emission High-temperature operation Longest wavelength of interband semiconductor lasers Hot-hole (unipolar) semiconductor lasers Unipolar tunneling-based semiconductor lasers Theoretical schemes of the tunneling pumping Characteristics of quantum cascade lasers Nonlinear optical conversion in semiconductors Brief review of applications Conclusions 140 Acknowledgments 142 References 142 Chapter 3 Single-Mode and Tunable Laser Diodes 3.1 Introduction Single-mode laser diodes The Fabry-Perot laser diode The distributed Bragg reflector (DBR) laser Coupled-mode theory for DBR laser Purely passive DBR with nonreflecting end mirror Wavelength selectivity of DBR laser Distributed feedback (DFB) laser diodes Coupled mode theory for DFB laser Spectral linewidth Experimental results 189

5 VUl Contents 3.3 Wavelength tunable laser diodes Physical mechanisms for electronic wavelength tuning in laser diodes Continuously wavelength tunable laser diodes Longitudinally integrated structures Transversely integrated structures Spectral linewidth Physical limitations on tuning range of continuously tunable laser diodes Discontinously tunable laser diodes DBR-type laser structures Wavelength tunable Y-laser Codirectionally mode-coupled lasers Outlook Conclusion 250 References 251 Chapter 4 High-Power Semiconductor Lasers 4.1 Introduction Why high power? Power limitations Case study: index-guided single-mode lasers Beam quality Carrier-induced gain and refractive index The effective index method for finding spatial modes Gain and index waveguiding Filamentation and the a-parameter Brightness, Strehl ratio, and M Brightness Strehl ratio M 2 -factor Case study: monolithic flared amplifier master oscillator power amplifier Thermal management Operating parameters Thermal resistance Characteristic temperature, T Reliability and activation energy 305

6 Contents ix Case study: QUASI-CW 1 cm-wide laser array bars Conclusions 318 Acknowledgments 318 References 318 Chapter 5 Surface-Emitting Lasers Abstract Introduction Configurations of surface-emitting lasers Categorization of surface-emitting lasers Vertical-cavity surface emitting lasers Grating coupled surface emitting lasers Deflecting-mirror surface-emitting lasers Folded cavity semiconductor lasers Basics of vertical cavity surface-emitting lasers Threshold current and quantum efficiency Fundamental elements for vertical cavity surfaceemitting lasers Dielectric multilayer mirrors Semiconductor multi-layer structures Quantum wells for gain medium Periodic and matched gain structures Current and optical confinement Device design and technology Long wavelength surface-emitting lasers GaAlAs/GaAs surface emitting lasers GalnAs/GaAs surface-emitting lasers Short-wavelength surface-emitting lasers Lasing characteristics of VCSELs Ultimate performances Single-mode behavior Polarization characteristics Quantum noise Spontaneous emission control Photon recycling Integrations and applied optical subsystems Photonic-stack integration Surface operating devices and monolithic integrations 358

7 Two-dimensional arrays of surface-emitting lasers Applied subsystems Summary References Index 373

Diode Lasers and Photonic Integrated Circuits

Diode Lasers and Photonic Integrated Circuits Diode Lasers and Photonic Integrated Circuits L. A. COLDREN S. W. CORZINE University of California Santa Barbara, California A WILEY-INTERSCIENCE PUBLICATION JOHN WILEY & SONS, INC. NEW YORK / CHICHESTER

More information

Distributed feedback semiconductor lasers

Distributed feedback semiconductor lasers Distributed feedback semiconductor lasers John Carroll, James Whiteaway & Dick Plumb The Institution of Electrical Engineers SPIE Optical Engineering Press 1 Preface Acknowledgments Principal abbreviations

More information

Stimulated Emission Devices: LASERS

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 information

(b) Spontaneous emission. Absorption, spontaneous (random photon) emission and stimulated emission.

(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 information

Optics, Optoelectronics and Photonics

Optics, Optoelectronics and Photonics Optics, Optoelectronics and Photonics Engineering Principles and Applications Alan Billings Emeritus Professor, University of Western Australia New York London Toronto Sydney Tokyo Singapore v Contents

More information

Introduction to Semiconductor Integrated Optics

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

More information

Laser Basics. What happens when light (or photon) interact with a matter? Assume photon energy is compatible with energy transition levels.

Laser 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 information

Emission Spectra of the typical DH laser

Emission 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 information

Blue-green Emitting Semiconductor Disk Lasers with Intra-Cavity Frequency Doubling

Blue-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 information

Quantum Dot Lasers. Jose Mayen ECE 355

Quantum 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 information

Chapter 5. Semiconductor Laser

Chapter 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 information

Lasers and Electro-optics

Lasers and Electro-optics Lasers and Electro-optics Second Edition CHRISTOPHER C. DAVIS University of Maryland III ^0 CAMBRIDGE UNIVERSITY PRESS Preface to the Second Edition page xv 1 Electromagnetic waves, light, and lasers 1

More information

Modern Semiconductor Lasers. Isabel Reis

Modern Semiconductor Lasers. Isabel Reis Modern Semiconductor Lasers Isabel Reis University Stuttgart Advanced Seminar 23rd June 2016 Supervisor: Dr. Michael Jetter Today, lasers are used in a wide range of important applications and especially

More information

Segmented 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. 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 information

Chemistry Instrumental Analysis Lecture 5. Chem 4631

Chemistry Instrumental Analysis Lecture 5. Chem 4631 Chemistry 4631 Instrumental Analysis Lecture 5 Light Amplification by Stimulated Emission of Radiation High Intensities Narrow Bandwidths Coherent Outputs Applications CD/DVD Readers Fiber Optics Spectroscopy

More information

Photonics and Optical Communication

Photonics and Optical Communication Photonics and Optical Communication (Course Number 300352) Spring 2007 Optical Source Dr. Dietmar Knipp Assistant Professor of Electrical Engineering http://www.faculty.iu-bremen.de/dknipp/ 1 Photonics

More information

Introduction to Optoelectronic Device Simulation by Joachim Piprek

Introduction 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 information

Laser Physics OXFORD UNIVERSITY PRESS SIMON HOOKER COLIN WEBB. and. Department of Physics, University of Oxford

Laser Physics OXFORD UNIVERSITY PRESS SIMON HOOKER COLIN WEBB. and. Department of Physics, University of Oxford Laser Physics SIMON HOOKER and COLIN WEBB Department of Physics, University of Oxford OXFORD UNIVERSITY PRESS Contents 1 Introduction 1.1 The laser 1.2 Electromagnetic radiation in a closed cavity 1.2.1

More information

Optics, Light and Lasers

Optics, Light and Lasers Dieter Meschede Optics, Light and Lasers The Practical Approach to Modern Aspects of Photonics and Laser Physics Second, Revised and Enlarged Edition BICENTENNIAL.... n 4 '':- t' 1 8 0 7 $W1LEY 2007 tri

More information

Study on Quantum Dot Lasers and their advantages

Study on Quantum Dot Lasers and their advantages Study on Quantum Dot Lasers and their advantages Tae Woo Kim Electrical and Computer Engineering University of Illinois, Urbana Champaign Abstract Basic ideas for understanding a Quantum Dot Laser were

More information

Signal regeneration - optical amplifiers

Signal 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 information

School of Electrical and Computer Engineering, Cornell University. ECE 5330: Semiconductor Optoelectronics. Fall Due on Nov 20, 2014 by 5:00 PM

School of Electrical and Computer Engineering, Cornell University. ECE 5330: Semiconductor Optoelectronics. Fall Due on Nov 20, 2014 by 5:00 PM School of Electrical and Computer Engineering, Cornell University ECE 533: Semiconductor Optoelectronics Fall 14 Homewor 8 Due on Nov, 14 by 5: PM This is a long -wee homewor (start early). It will count

More information

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

OPTI510R: Photonics. Khanh Kieu College of Optical Sciences, University of Arizona Meinel building R.626 OPTI510R: Photonics Khanh Kieu College of Optical Sciences, University of Arizona kkieu@optics.arizona.edu Meinel building R.626 Announcements HW #6 is assigned, due April 23 rd Final exam May 2 Semiconductor

More information

Introduction Fundamentals of laser Types of lasers Semiconductor lasers

Introduction Fundamentals of laser Types of lasers Semiconductor lasers Introduction Fundamentals of laser Types of lasers Semiconductor lasers Is it Light Amplification and Stimulated Emission Radiation? No. So what if I know an acronym? What exactly is Light Amplification

More information

Semiconductor Disk Laser on Microchannel Cooler

Semiconductor 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 information

Other Devices from p-n junctions

Other Devices from p-n junctions Memory (5/7 -- Glenn Alers) Other Devices from p-n junctions Electron to Photon conversion devices LEDs and SSL (5/5) Lasers (5/5) Solid State Lighting (5/5) Photon to electron conversion devices Photodectors

More information

Contents Part I Concepts 1 The History of Heterostructure Lasers 2 Stress-Engineered Quantum Dots: Nature s Way

Contents Part I Concepts 1 The History of Heterostructure Lasers 2 Stress-Engineered Quantum Dots: Nature s Way Contents Part I Concepts 1 The History of Heterostructure Lasers Zhores I. Alferov... 3 1.1 Introduction... 3 1.2 The DHS Concept and Its Application for Semiconductor Lasers. 3 1.3 Quantum Dot Heterostructure

More information

Semiconductor Lasers EECE 484. Winter Dr. Lukas Chrostowski

Semiconductor Lasers EECE 484. Winter Dr. Lukas Chrostowski Semiconductor Lasers EECE 484 Winter 2013 Dr. Lukas Chrostowski 1 484 - Course Information Web Page: http://siepic.ubc.ca/eece484 (password DBR, check for updates) + Piazza, https://piazza.com/ubc.ca/winterterm22013/eece484

More information

Optoelectronics ELEC-E3210

Optoelectronics ELEC-E3210 Optoelectronics ELEC-E3210 Lecture 3 Spring 2017 Semiconductor lasers I Outline 1 Introduction 2 The Fabry-Pérot laser 3 Transparency and threshold current 4 Heterostructure laser 5 Power output and linewidth

More information

Recent progress on single-mode quantum cascade lasers

Recent progress on single-mode quantum cascade lasers Recent progress on single-mode quantum cascade lasers B. Hinkov 1,*, P. Jouy 1, A. Hugi 1, A. Bismuto 1,2, M. Beck 1, S. Blaser 2 and J. Faist 1 * bhinkov@phys.ethz.ch 1 Institute of Quantum Electronics,

More information

FIBER OPTICS. Prof. R.K. Shevgaonkar. Department of Electrical Engineering. Indian Institute of Technology, Bombay. Lecture: 17.

FIBER OPTICS. Prof. R.K. Shevgaonkar. Department of Electrical Engineering. Indian Institute of Technology, Bombay. Lecture: 17. FIBER OPTICS Prof. R.K. Shevgaonkar Department of Electrical Engineering Indian Institute of Technology, Bombay Lecture: 17 Optical Sources- Introduction to LASER Fiber Optics, Prof. R.K. Shevgaonkar,

More information

High Power Diode Lasers

High 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 information

Metal Vapour Lasers Use vapourized metal as a gain medium Developed by W. Silfvast (1966) Put metal in a cavity with a heater Vapourize metal, then

Metal Vapour Lasers Use vapourized metal as a gain medium Developed by W. Silfvast (1966) Put metal in a cavity with a heater Vapourize metal, then Metal Vapour Lasers Use vapourized metal as a gain medium Developed by W. Silfvast (1966) Put metal in a cavity with a heater Vapourize metal, then pump metal vapour with current Walter at TRG (1966) then

More information

ELECTRONS AND PHONONS IN SEMICONDUCTOR MULTILAYERS

ELECTRONS AND PHONONS IN SEMICONDUCTOR MULTILAYERS ELECTRONS AND PHONONS IN SEMICONDUCTOR MULTILAYERS Second Edition B.K. RIDLEY University of Essex CAMBRIDGE UNIVERSITY PRESS Contents Preface Introduction 1 Simple Models of the Electron-Phonon Interaction

More information

Tunable GaN-Based Laser Diode

Tunable GaN-Based Laser Diode Tunable GaN-Based Laser Diode Christoph Eichler We have investigated the wavelength tuning characteristics of a GaN-based cw-laser diode with an emission wavelength of 425 nm. Temperature dependent spectra

More information

Semiconductor Lasers for Optical Communication

Semiconductor 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 information

Semiconductor Optoelectronics Prof. M. R. Shenoy Department of Physics Indian Institute of Technology, Delhi

Semiconductor Optoelectronics Prof. M. R. Shenoy Department of Physics Indian Institute of Technology, Delhi Semiconductor Optoelectronics Prof. M. R. Shenoy Department of Physics Indian Institute of Technology, Delhi Lecture - 1 Context and Scope of the Course (Refer Slide Time: 00:44) Welcome to this course

More information

Chapter9. Amplification of light. Lasers Part 2

Chapter9. Amplification of light. Lasers Part 2 Chapter9. Amplification of light. Lasers Part 06... Changhee Lee School of Electrical and Computer Engineering Seoul National Univ. chlee7@snu.ac.kr /9 9. Stimulated emission and thermal radiation The

More information

Distributed-Feedback Lasers

Distributed-Feedback Lasers Distributed-Feedback Lasers Class: Integrated Photonic Devices Tie: Fri. 8:00a ~ 11:00a. Classroo: 資電 06 Lecturer: Prof. 李明昌 (Ming-Chang Lee) Wavelength Dependence of Bragg Reflections Free-Space Bragg

More information

Carrier Loss Analysis for Ultraviolet Light-Emitting Diodes

Carrier Loss Analysis for Ultraviolet Light-Emitting Diodes Carrier Loss Analysis for Ultraviolet Light-Emitting Diodes Joachim Piprek, Thomas Katona, Stacia Keller, Steve DenBaars, and Shuji Nakamura Solid State Lighting and Display Center University of California

More information

- Outline. Chapter 4 Optical Source. 4.1 Semiconductor physics

- Outline. Chapter 4 Optical Source. 4.1 Semiconductor physics Chapter 4 Optical Source - Outline 4.1 Semiconductor physics - Energy band - Intrinsic and Extrinsic Material - pn Junctions - Direct and Indirect Band Gaps 4. Light Emitting Diodes (LED) - LED structure

More information

Effect of non-uniform distribution of electric field on diffusedquantum well lasers

Effect of non-uniform distribution of electric field on diffusedquantum well lasers Title Effect of non-uniform distribution of electric field on diffusedquantum well lasers Author(s) Man, WM; Yu, SF Citation IEEE Hong Kong Electron Devices Meeting Proceedings, Hong Kong, China, 29 August

More information

Photonic Crystal Nanocavities for Efficient Light Confinement and Emission

Photonic Crystal Nanocavities for Efficient Light Confinement and Emission Journal of the Korean Physical Society, Vol. 42, No., February 2003, pp. 768 773 Photonic Crystal Nanocavities for Efficient Light Confinement and Emission Axel Scherer, T. Yoshie, M. Lončar, J. Vučković

More information

Fiber Gratings p. 1 Basic Concepts p. 1 Bragg Diffraction p. 2 Photosensitivity p. 3 Fabrication Techniques p. 4 Single-Beam Internal Technique p.

Fiber Gratings p. 1 Basic Concepts p. 1 Bragg Diffraction p. 2 Photosensitivity p. 3 Fabrication Techniques p. 4 Single-Beam Internal Technique p. Preface p. xiii Fiber Gratings p. 1 Basic Concepts p. 1 Bragg Diffraction p. 2 Photosensitivity p. 3 Fabrication Techniques p. 4 Single-Beam Internal Technique p. 4 Dual-Beam Holographic Technique p. 5

More information

Nonlinear Dynamics of Quantum Cascade Laser in Ring Cavity

Nonlinear Dynamics of Quantum Cascade Laser in Ring Cavity Nonlinear Dynamics of Quantum Cascade Laser in Ring Cavity A THESIS SUBMITTED TO THE FACULTY OF THE GRADUATE SCHOOL OF THE UNIVERSITY OF MINNESOTA BY HADI MADANIAN IN PARTIAL FULFILLMENT OF THE REQUIREMENTS

More information

Thermal crosstalk in densely packed high power VCSEL arrays

Thermal crosstalk in densely packed high power VCSEL arrays 26 Annual report 1998, Dept. of Optoelectronics, University of Ulm Thermal crosstalk in densely packed high power VCSEL arrays M. Grabherr, M. Miller, H.J. Unold We present detailed investigations on the

More information

PRINCIPLES OF PHYSICAL OPTICS

PRINCIPLES OF PHYSICAL OPTICS PRINCIPLES OF PHYSICAL OPTICS C. A. Bennett University of North Carolina At Asheville WILEY- INTERSCIENCE A JOHN WILEY & SONS, INC., PUBLICATION CONTENTS Preface 1 The Physics of Waves 1 1.1 Introduction

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION doi:10.1038/nature12036 We provide in the following additional experimental data and details on our demonstration of an electrically pumped exciton-polariton laser by supplementing optical and electrical

More information

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

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 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 information

Abnormal PL spectrum in InGaN MQW surface emitting cavity

Abnormal PL spectrum in InGaN MQW surface emitting cavity Abnormal PL spectrum in InGaN MQW surface emitting cavity J. T. Chu a, Y.-J. Cheng b, H. C. Kuo a, T. C. Lu a, and S. C. Wang a a Department of Photonics & Institute of Electro-Optical Engineering, National

More information

Oscillateur paramétrique optique en

Oscillateur paramétrique optique en C. Ozanam 1, X. Lafosse 2, I. Favero 1, S. Ducci 1, G. Leo 1 1 Université Paris Diderot, Sorbonne Paris Cité, Laboratoire MPQ, CNRS-UMR 7162, Paris, France, 2 Laboratoire de Photonique et Nanostructures,

More information

Lasers. Stimulated Emission Lasers: Trapping Photons Terahertz Lasers Course Overview

Lasers. Stimulated Emission Lasers: Trapping Photons Terahertz Lasers Course Overview Lasers Stimulated Emission Lasers: Trapping Photons Terahertz Lasers Course Overview 1 P-N Junctions and LEDs Terminal Pins Emitted Light Beams Diode Transparent Plastic Case High energy electrons (n-type)

More information

EE 472 Solutions to some chapter 4 problems

EE 472 Solutions to some chapter 4 problems EE 472 Solutions to some chapter 4 problems 4.4. Erbium doped fiber amplifier An EDFA is pumped at 1480 nm. N1 and N2 are the concentrations of Er 3+ at the levels E 1 and E 2 respectively as shown in

More information

External (differential) quantum efficiency Number of additional photons emitted / number of additional electrons injected

External (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 information

Paper Review. Special Topics in Optical Engineering II (15/1) Minkyu Kim. IEEE Journal of Quantum Electronics, Feb 1985

Paper 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 information

1300nm-Range GaInNAs-Based Quantum Well Lasers with High Characteristic Temperature

1300nm-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 information

6. Light emitting devices

6. Light emitting devices 6. Light emitting devices 6. The light emitting diode 6.. Introduction A light emitting diode consist of a p-n diode which is designed so that radiative recombination dominates. Homojunction p-n diodes,

More information

Characterization of Active Regions for InP-Based MEMS-VCSELs

Characterization of Active Regions for InP-Based MEMS-VCSELs MASTER S THESIS Characterization of Active Regions for InP-Based MEMS-VCSELs Erik Haglund Department of Microtechnology and Nanoscience CHALMERS UNIVERSITY OF TECHNOLOGY Walter Schottky Institut TECHNISCHE

More information

THREE-dimensional electronic confinement in semiconductor

THREE-dimensional electronic confinement in semiconductor IEEE JOURNAL OF QUANTUM ELECTRONICS, VOL. 43, NO. 3, MARCH 2007 287 Differential Gain and Gain Compression in Quantum-Dot Lasers Andrea Fiore and Alexander Markus Abstract The dynamics of optical gain

More information

A Guide to Experiments in Quantum Optics

A Guide to Experiments in Quantum Optics Hans-A. Bachor and Timothy C. Ralph A Guide to Experiments in Quantum Optics Second, Revised and Enlarged Edition WILEY- VCH WILEY-VCH Verlag CmbH Co. KGaA Contents Preface 1 Introduction 1.1 Historical

More information

ISSN Review. Progress to a Gallium-Arsenide Deep-Center Laser

ISSN 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 information

An impact of the electrical pumping scheme on some VCSEL performance characteristics

An impact of the electrical pumping scheme on some VCSEL performance characteristics Optica Applicata, Vol. XXXIX, No. 4, 2009 An impact of the electrical pumping scheme on some VCSEL performance characteristics SEWERYN MORAWIEC, PIOTR KOWALCZEWSKI, ROBERT P. SARZAŁA * Laboratory of Computer

More information

1 Semiconductor Quantum Dots for Ultrafast Optoelectronics

1 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 information

Lecture 8 Con,nuous- Wave Laser*

Lecture 8 Con,nuous- Wave Laser* Lecture 8 Con,nuous- Wave Laser* Min Yan Op,cs and Photonics, KTH 24/04/15 1 * Some figures and texts belong to: O. Svelto, Principles of Lasers, 5th Ed., Springer. Reading Principles of Lasers (5th Ed.):

More information

Optical Feedback in Vertical-Cavity Surface-Emitting Lasers

Optical Feedback in Vertical-Cavity Surface-Emitting Lasers IEEE JOURNAL OF QUANTUM ELECTRONICS, VOL. 37, NO. 12, DECEMBER 2001 1643 Optical Feedback in Vertical-Cavity Surface-Emitting Lasers A. Hsu, Student Member, IEEE, J.-F. P. Seurin, S. L. Chuang, Fellow,

More information

Principles of Electron Optics

Principles of Electron Optics Principles of Electron Optics Volume 2 Applied Geometrical Optics by P. W. HAWKES CNRS Laboratory of Electron Optics, Toulouse, France and E. KASPER Institut für Angewandte Physik Universität Tübingen,

More information

Study on Semiconductor Lasers of Circular Structures Fabricated by EB Lithography

Study on Semiconductor Lasers of Circular Structures Fabricated by EB Lithography Study on Semiconductor Lasers of Circular Structures Fabricated by EB Lithography Ashim Kumar Saha (D3) Supervisor: Prof. Toshiaki Suhara Doctoral Thesis Defense Quantum Engineering Design Course Graduate

More information

Refractive Index Measurement by Gain- or Loss-Induced Resonance

Refractive Index Measurement by Gain- or Loss-Induced Resonance Refractive Index Measurement by Gain- or Loss-Induced Resonance 59 Refractive Index Measurement by Gain- or Loss-Induced Resonance Markus Miller Using a semiconductor optical resonator consisting of a

More information

COMPLEX laser structures such as distributed feedback

COMPLEX laser structures such as distributed feedback IEEE JOURNAL OF QUANTUM ELECTRONICS, VOL. 33, NO. 11, NOVEMBER 1997 2105 Semiclassical Model of Semiconductor Laser Noise and Amplitude Noise Squeezing Part II: Application to Complex Laser Structures

More information

Widely Tunable and Intense Mid-Infrared PL Emission from Epitaxial Pb(Sr)Te Quantum Dots in a CdTe Matrix

Widely Tunable and Intense Mid-Infrared PL Emission from Epitaxial Pb(Sr)Te Quantum Dots in a CdTe Matrix Widely Tunable and Intense Mid-Infrared PL Emission from Epitaxial Pb(Sr)Te Quantum Dots in a Matrix S. Kriechbaumer 1, T. Schwarzl 1, H. Groiss 1, W. Heiss 1, F. Schäffler 1,T. Wojtowicz 2, K. Koike 3,

More information

S. Blair February 15,

S. Blair February 15, S Blair February 15, 2012 66 32 Laser Diodes A semiconductor laser diode is basically an LED structure with mirrors for optical feedback This feedback causes photons to retrace their path back through

More information

Laser Types Two main types depending on time operation Continuous Wave (CW) Pulsed operation Pulsed is easier, CW more useful

Laser Types Two main types depending on time operation Continuous Wave (CW) Pulsed operation Pulsed is easier, CW more useful Main Requirements of the Laser Optical Resonator Cavity Laser Gain Medium of 2, 3 or 4 level types in the Cavity Sufficient means of Excitation (called pumping) eg. light, current, chemical reaction Population

More information

Semiconductor Quantum Dot Nanostructures and their Roles in the Future of Photonics

Semiconductor Quantum Dot Nanostructures and their Roles in the Future of Photonics 550 Brazilian Journal of Physics, vol. 34, no. 2B, June, 2004 Semiconductor Quantum Dot Nanostructures and their Roles in the Future of Photonics S. Fafard, K. Hinzer, and C. N. Allen Institute for Microstructural

More information

Near-Infrared Spectroscopy of Nitride Heterostructures EMILY FINAN ADVISOR: DR. OANA MALIS PURDUE UNIVERSITY REU PROGRAM AUGUST 2, 2012

Near-Infrared Spectroscopy of Nitride Heterostructures EMILY FINAN ADVISOR: DR. OANA MALIS PURDUE UNIVERSITY REU PROGRAM AUGUST 2, 2012 Near-Infrared Spectroscopy of Nitride Heterostructures EMILY FINAN ADVISOR: DR. OANA MALIS PURDUE UNIVERSITY REU PROGRAM AUGUST 2, 2012 Introduction Experimental Condensed Matter Research Study of large

More information

OPTICAL GAIN AND LASERS

OPTICAL GAIN AND LASERS OPTICAL GAIN AND LASERS 01-02-1 BY DAVID ROCKWELL DIRECTOR, RESEARCH & DEVELOPMENT fsona COMMUNICATIONS MARCH 6, 2001 OUTLINE 01-02-2 I. DEFINITIONS, BASIC CONCEPTS II. III. IV. OPTICAL GAIN AND ABSORPTION

More information

What Makes a Laser Light Amplification by Stimulated Emission of Radiation Main Requirements of the Laser Laser Gain Medium (provides the light

What Makes a Laser Light Amplification by Stimulated Emission of Radiation Main Requirements of the Laser Laser Gain Medium (provides the light What Makes a Laser Light Amplification by Stimulated Emission of Radiation Main Requirements of the Laser Laser Gain Medium (provides the light amplification) Optical Resonator Cavity (greatly increase

More information

MEASUREMENT of gain from amplified spontaneous

MEASUREMENT of gain from amplified spontaneous IEEE JOURNAL OF QUANTUM ELECTRONICS, VOL. 40, NO. 2, FEBRUARY 2004 123 Fourier Series Expansion Method for Gain Measurement From Amplified Spontaneous Emission Spectra of Fabry Pérot Semiconductor Lasers

More information

Characteristics of a Designed 1550 nm AlGaInAs/InP MQW VCSEL

Characteristics of a Designed 1550 nm AlGaInAs/InP MQW VCSEL INTERNATIONAL JOURNAL OF MULTIDISCIPLINARY SCIENCES AND ENGINEERING, VOL. 4, NO. 1, JANUARY 13 Characteristics of a Designed 155 nm AlGaInAs/InP MQW VCSEL Raja Rashidul Hasan and Rinku Basak Abstract The

More information

Synchronization of semiconductor laser arrays with 2D Bragg structures

Synchronization of semiconductor laser arrays with 2D Bragg structures Journal of Physics: Conference Series PAPER OPEN ACCESS Synchroniation of semiconductor laser arrays with D Bragg structures To cite this article: V R Baryshev and N S Ginburg 06 J. Phys.: Conf. Ser. 740

More information

Distributed Feedback Laser ECE 464. Tin Nguyen

Distributed Feedback Laser ECE 464. Tin Nguyen Distributed Feedbac Laser ECE 464 Tin Nguyen La Rosa, Spring 2008 Abstract In recent year, distributed feedbac laser was one of the hot topics that have been study for many years. It was introduced and

More information

Laser Types Two main types depending on time operation Continuous Wave (CW) Pulsed operation Pulsed is easier, CW more useful

Laser Types Two main types depending on time operation Continuous Wave (CW) Pulsed operation Pulsed is easier, CW more useful What Makes a Laser Light Amplification by Stimulated Emission of Radiation Main Requirements of the Laser Laser Gain Medium (provides the light amplification) Optical Resonator Cavity (greatly increase

More information

Nanostrutture a confinamento quantistico elettronico: i quantum dot

Nanostrutture a confinamento quantistico elettronico: i quantum dot Nanostrutture a confinamento quantistico elettronico: i quantum dot Massimo De Vittorio National Nanotechnology Laboratories of CNR-INFM ISUFI - Università del Salento massimo.devittorio@unile.it Outline

More information

Nanophysics: Main trends

Nanophysics: Main trends Nano-opto-electronics Nanophysics: Main trends Nanomechanics Main issues Light interaction with small structures Molecules Nanoparticles (semiconductor and metallic) Microparticles Photonic crystals Nanoplasmonics

More information

LASER. Light Amplification by Stimulated Emission of Radiation

LASER. Light Amplification by Stimulated Emission of Radiation LASER Light Amplification by Stimulated Emission of Radiation Energy Level, Definitions The valence band is the highest filled band The conduction band is the next higher empty band The energy gap has

More information

EE 6313 Homework Assignments

EE 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 information

B 2 P 2, which implies that g B should be

B 2 P 2, which implies that g B should be Enhanced Summary of G.P. Agrawal Nonlinear Fiber Optics (3rd ed) Chapter 9 on SBS Stimulated Brillouin scattering is a nonlinear three-wave interaction between a forward-going laser pump beam P, a forward-going

More information

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

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

More information

Reflectivity and photoluminescence studies in Bragg reflectors with absorbing layers

Reflectivity and photoluminescence studies in Bragg reflectors with absorbing layers INSTITUTE OF PHYSICS PUBLISHING SEMICONDUCTOR SCIENCE AND TECHNOLOGY Semicond. Sci. Technol. 16 (2001) 548 552 www.iop.org/journals/ss PII: S0268-1242(01)16119-5 Reflectivity and photoluminescence studies

More information

Lasers... the optical cavity

Lasers... the optical cavity Lasers... the optical cavity history principle, intuitive aspects, characteristics 2 levels systems Ti: Helium Al2O3 - Neon model-locked laser laser VCSEL bragg mirrors cleaved facets 13 ptical and/or

More information

Fiber Lasers. Chapter Basic Concepts

Fiber Lasers. Chapter Basic Concepts Chapter 5 Fiber Lasers A fiber amplifier can be converted into a laser by placing it inside a cavity designed to provide optical feedback. Such lasers are called fiber lasers, and this chapter is devoted

More information

Modeling of Kerr non-linear photonic components with mode expansion

Modeling of Kerr non-linear photonic components with mode expansion Modeling of Kerr non-linear photonic components with mode expansion Björn Maes (bjorn.maes@intec.ugent.be), Peter Bienstman and Roel Baets Department of Information Technology, Ghent University IMEC, St.-Pietersnieuwstraat

More information

Laser Diodes. Revised: 3/14/14 14: , Henry Zmuda Set 6a Laser Diodes 1

Laser 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 information

Lecture 2. Electron states and optical properties of semiconductor nanostructures

Lecture 2. Electron states and optical properties of semiconductor nanostructures Lecture Electron states and optical properties of semiconductor nanostructures Bulk semiconductors Band gap E g Band-gap slavery: only light with photon energy equal to band gap can be generated. Very

More information

QUESTION BANK IN PHYSICS

QUESTION BANK IN PHYSICS QUESTION BANK IN PHYSICS LASERS. Name some properties, which make laser light different from ordinary light. () {JUN 5. The output power of a given laser is mw and the emitted wavelength is 630nm. Calculate

More information

Crosslight Software Overview, New Features & Updates. Dr. Peter Mensz

Crosslight Software Overview, New Features & Updates. Dr. Peter Mensz 1 Crosslight Software Overview, New Features & Updates Dr. Peter Mensz 2 Device Simulators Lastip/Pics3d Laser diode FEM models in 2D/3D Apsys 2D and 3D Any other compound semiconductors device FEM models,

More information

Appendix. Photonic crystal lasers: future integrated devices

Appendix. Photonic crystal lasers: future integrated devices 91 Appendix Photonic crystal lasers: future integrated devices 5.1 Introduction The technology of photonic crystals has produced a large variety of new devices. However, photonic crystals have not been

More information

School of Electrical and Computer Engineering, Cornell University. ECE 5330: Semiconductor Optoelectronics. Fall 2014

School of Electrical and Computer Engineering, Cornell University. ECE 5330: Semiconductor Optoelectronics. Fall 2014 School of Electrical and Computer Engineering, Cornell University ECE 5330: Semiconductor Optoelectronics Fall 014 Homework 7 Due on Nov. 06, 014 Suggested Readings: i) Study lecture notes. ii) Study Coldren

More information

Polarization-Resolved Output Characteristics of InAlGaAs VCSELs under Anisotropic Strain

Polarization-Resolved Output Characteristics of InAlGaAs VCSELs under Anisotropic Strain Polarization-Resolved Output Characteristics of InAlGaAs VCSELs under Anisotropic Strain Andrea Kroner and Johannes Michael Ostermann We present a setup that enables direct examination of the correlation

More information

Designing a high speed 1310nm AlGaInAs/AlGaInAs VCSEL using MgO/Si top DBR and GaInAsP/InP bottom DBR

Designing a high speed 1310nm AlGaInAs/AlGaInAs VCSEL using MgO/Si top DBR and GaInAsP/InP bottom DBR American Journal of Optics and Photonics 014; (3): 37-44 Published online July 0, 014 (http://www.sciencepublishinggroup.com/j/ajop) doi: 10.11648/j.ajop.014003.14 ISSN: 330-8486 (Print); ISSN: 330-8494

More information