High power and single frequency quantum. cascade lasers for gas sensing. Stéphane Blaser

Size: px
Start display at page:

Download "High power and single frequency quantum. cascade lasers for gas sensing. Stéphane Blaser"

Transcription

1 High power and single frequency quantum cascade lasers for gas sensing Stéphane Blaser Alpes Lasers: Yargo Bonetti Lubos Hvozdara Antoine Muller University of Neuchâtel: Marcella Giovannini Nicolas Hoyler Mattias Beck Jérome Faist

2 Outline Introduction Applications High power Fabry-Pérot devices High power pulsed DFB devices Cryogenic continuous-wave devices Reliability of the devices

3 Interband vs intersubband E E f E 12 k Interband transition - bipolar - photon energy limited by bandgap E g of material - Telecom, CD, DVD, E E 12 E f k Intersubband transition - unipolar, narrow gain - photon energy depends on layer thickness and can be tailored

4 Quantum cascade lasers Cascade -eache-emits N photons Active region / injector - active region population inversion which must be engineered -injector avoid fields domains and cools down the electrons τ32 > τ 21 T e >>T l τ 32 τ 21 T e ~T l active region relaxation / injection MBE - growth of thin layers - sharp interfaces

5 InP CW pulsed State of the art: QCL performances Atmospheric windows GaAs Peltier Temperature [K] Reststrahlen band LN Wavelength [µm] CW pulsed - Good Mid-IR coverage - Terahertz promising Data: Uni Neuchâtel Alpes Lasers Bell Labs Thales TU Vienna Northwestern Uni W. Schottky

6 Spectrum covered by Alpes Lasers dfb QCLs infrared UV 1 cm 1 cm 1 mm 1 µm 1 µm.8 µm.4 µm radio RADAR QCL Wavelength [µm] CCl2 O 2 NH3 F4 Si O3 N2 O CH4 C2 H 4 C5 H 1 O CCl2 O CO N2 O CO2 C2 H 4 O NH maser 3.1 THz p-ge laser 1 THz CO 2 laser High power QC lasers using new designs: Bound-to-continuum (patent n wo 2/19485A1) Two-phonon resonance (patent n wo 2/23686A1) Wavenumber [cm -1 ]

7 Applications: chemical sensing by optical spectroscopy Vibrational mode of molecules in Mid-IR Detection techniques: photo-acoustic TILDAS cavity ringdown Can be used for trace gas analysis, process control liquid detection spectroscopy Needs: high-power laser narrow linewidth (single mode) continuous-wave operation Talks in TDLS 3: Barry McManus: Trace Gas Instrumentation Using Pulsed Quantum Cascade Lasers Mark Zahniser: Trace Gas Measurements Using Pulsed Quantum Cascade Lasers Frank Tittel: Chemical Sensing with Quantum Cascade Lasers

8 Applications: chemical sensing by optical spectroscopy Typical applications: atmosphere diagnostics pollution monitoring non-invasive medical diagnostics detection of biological contaminants, drugs or explosives ammonia (NH 3 ) monitoring in process industry CO, NO, SO 2, SO 3 (e.g. in combustion processes) CH 4, HF, H 2 S, in petro-chemical processing facilities (e.g. gas leak detector) CO 2, O 3 for environment monitoring Large organic hydrocarbon molecules like benzene

9 Other applications Telecommunications Free-space optical data transmission for the last mile (high speed with no need for licence and better operation in fog, compared to λ = 1.55 µm) Terahertz field Astronomy Medical imaging Chemical detection Telecommunications for local area network (LAN) Talks yesterday: Ruedeger Koehler: Terahertz Quantum Cascade Lasers Daniel Hofstetter: Latest Progress on Intersubband Devices: Lasers and Detectors from the Near- to the Far-Infrared

10 High average power FP QCL: RT-HP-FP-15-X K, 6% 3K, 2% Voltage [V] Average power [W] Current [A].2.1 Characteristics Back-facet coated λ = 7.9 Average power: P = 15 mw threshold current density: j th = 3. ka/cm : P =.82 W (6% dc) j th =.75 ka/cm 2 P in CW: P = 3mW (j th =.78 ka/cm 2 )

11 Continuous-wave FP QCL on Peltier C -2 C -3 C Voltage [V] Average power [mw] CW Current [A] 1 Characteristics 1.5 mm-long, 12 µm-wide laser Buried-heterostructure Back-facet coating CW operation at λ 9.2 µm on C: Average power: P = 42 mw Threshold current density: j th = 3.8 ka/cm 2 typically designed for Free Space Optics data transmission

12 High average power DFB QCL: RT-HP-DFB-2-X Distributed feedback QC laser at 8.35µm with InP top cladding 1 35 Characteristics mm-long, 28µm-wide laser λ 8.35 C: Average power (2% dc): P = 32 mw (1.6 W peak power) threshold current density: j th = 2.9 ka/cm 2 Voltage C : P = 25 mw (1.25W peak power) j th = 3.8 ka/cm 2 Average power [mw] -3 C C 3 C Current [A]

13 High average power DFB QCL: RT-HP-DFB-2-X Current [A] Voltage [V] Average power [mw] -3 C C 3 C C, 14V 3 C, 12V 15 C, 14V 15 C, 12V C, 14V C, 12V C 3 C Characteristics λ 8.35 µm Single-mode operation at T C with SMSR 4 db (At high bias, single-mode operation with SMSR 2 db) 4 db Wavelength [µm]

14 Long-wavelength (λ 16.4µm) B2C DFB QCL: RT-P-DFB-1-X Laser based on a bound to continuum design, λ 16.4 µm Rochat et al., APL 79, 4271 (21) Current [A] DC voltage fed to LDD [V] Average power [mw] -3 C -15 C C 15 C 3 C 4 C 5 C Characteristics 3 mm-long, 44µm-wide laser λ 16.4 C: Average power (1.5% dc): P = 1.5 mw (1 mw peak power) Threshold current density: j th = 5.4 ka/cm C : P =.5 mw (33 mw peak power) j th = 7.9 ka/cm 2

15 Long-wavelength (λ 16.4µm) B2C DFB QCL: RT-P-DFB-1-X C, 21V -3 C, 27V -15 C, 21V -15 C, 27V C, 23V C, 28V 15 C, 24V 15 C, 29V 3 C, 26V 3 C, 3V 4 C, 27V 4 C, 32V 5 C, 28V 5 C, 32V Characteristics 3mm-long, 44µm-wide laser λ 16.4 µm single-mode emission: Side Mode Suppression Ratio > 25 db tuning range: cm -1 (16.51 µm) at 5 C to 61.3 cm -1 (16.38 µm) at -3 C Normalized intensity Wavenumbers [cm-1]

16 CW operation at λ 6.73µm: LN2-CW-DFB-1-X 1.2 Characteristics K 13K 12K 1K 8K mm-long, 23 µm-wide laser CW operation at λ 6.73 K: Average power P =.2 W Threshold current density: j th = 1. ka/cm 2 Voltage [V] Average power [W] Current [A]

17 CW operation at λ 6.73µm: LN2-CW-DFB-1-X K, 5mA 1K, 7mA 1K, 65mA 1K, 55mA 1K, 45mA 8K, 75mA 8K, 7mA 8K, 6mA 8K, 5mA 8K, 4mA Wavelength [µm] Characteristics 1.5 mm-long, 23 µm-wide laser CW operation at λ 6.73 µm single-mode emission: Side Mode Suppression Ratio > 3 db tuning range: cm -1 (6.744 µm) at 12K to cm -1 (6.722 µm) at 8K Normalized intensity Wavenumbers [cm -1 ]

18 Terahertz QC laser THz QC laser based on a bound to continuum design, λ 87 µm Structure grown at University of Neuchâtel (L. Ajili, G. Scalari, M. Beck and M. Giovannini) j [A/cm 2 ] Duty cycle 2.5% Jth=267 A/cm 2 1k 5k 7k 78k Characteristics THz QC laser: λ 87 µm 2.7mm-long, 2µm-wide laser back-facet K: Peak power (2.5% dc): P = 14 mw threshold current density: j th = 267 A/cm 2 Voltage [V] Peak power [mw] Emission energy [mev] Current[A] pulsed operation up to 78K CW operation up to 3 K

19 Reliability of the devices Lifetime measurement (partly with HR coating) ageing at 13 C and 2 % duty-cycle, monitor signal at 3 C (HR) c1 (HR) c11 (HR) c13 c14 c15 Normalized output power Time [hours] => lifetime of the devices > 4 years

20 Tuning Advantages of QCLs DFB Pulsed (CW) CW Pulsed FP CW Pulsed CW RT LN2 RT LN2 3 mw (4mW) mw 2 mw.8 W 2 mw < 33 MHz < 3.5 MHz 1-4 % 1-4 %.4 %.4 % N/A N/A Portable Linewidth Temp. cycling Power Temperature Type Duty-cycle

Room Temperature. from Alpes Lasers

Room Temperature. from Alpes Lasers Boston Electronics Corporation 91 Boylston Street, Brookline, Massachusetts 02445 USA (800)347-5445 or (617)566-3821 fax (617)731-0935 www.boselec.com boselec@boselec.com Room Temperature TUNABLE IR DIODE

More information

Continuous wave operation of quantum cascade lasers above room temperature

Continuous wave operation of quantum cascade lasers above room temperature Invited Paper Continuous wave operation of quantum cascade lasers above room temperature Mattias Beck *a, Daniel Hofstetter a,thierryaellen a,richardmaulini a,jérômefaist a,emiliogini b a Institute of

More information

MBE Growth of Terahertz Quantum Cascade Lasers Harvey Beere

MBE Growth of Terahertz Quantum Cascade Lasers Harvey Beere MBE Growth of Terahertz Quantum Cascade Lasers Harvey Beere Cavendish Laboratory J J Thomson Avenue Madingley Road Cambridge, CB3 0HE United Kingdom People involved Harvey Beere, Chris Worrall, Josh Freeman,

More information

The quantum cascade laser: a unifying concept for generating electromagnetic radiation from 3 to 300µm wavelength

The quantum cascade laser: a unifying concept for generating electromagnetic radiation from 3 to 300µm wavelength The quantum cascade laser: a unifying concept for generating electromagnetic radiation from 3 to 300µm wavelength C. Sirtori Matériaux et phénomènes quantiques, Université Paris 7 - Denis Diderot ALCATEL-THALES

More information

Introduction Fundamentals of laser Types of lasers Semiconductor lasers

Introduction Fundamentals of laser Types of lasers Semiconductor lasers ECE 5368 Introduction Fundamentals of laser Types of lasers Semiconductor lasers Introduction Fundamentals of laser Types of lasers Semiconductor lasers How many types of lasers? Many many depending on

More information

Surface-Emitting Single-Mode Quantum Cascade Lasers

Surface-Emitting Single-Mode Quantum Cascade Lasers Surface-Emitting Single-Mode Quantum Cascade Lasers M. Austerer, C. Pflügl, W. Schrenk, S. Golka, G. Strasser Zentrum für Mikro- und Nanostrukturen, Technische Universität Wien, Floragasse 7, A-1040 Wien

More information

Quantum cascade laser-based photoacoustic sensor for environmental pollution monitoring

Quantum cascade laser-based photoacoustic sensor for environmental pollution monitoring Quantum cascade laser-based photoacoustic sensor for environmental pollution monitoring Angela Elia, V. Spagnolo, C. Di Franco, P.M. Lugarà, G. Scamarcio Laboratorio Regionale CNR-INFM LIT 3 Dipartimento

More information

Advanced semiconductor lasers

Advanced semiconductor lasers Advanced semiconductor lasers Quantum cascade lasers Single mode lasers DFBs, VCSELs, etc. Quantum cascade laser Reminder: Semiconductor laser diodes Conventional semiconductor laser CB diode laser: material

More information

About Omics Group conferences

About Omics Group conferences About Omics Group OMICS Group International through its Open Access Initiative is committed to make genuine and reliable contributions to the scientific community. OMICS Group hosts over 400 leading-edge

More information

Lecture 6 Fiber Optical Communication Lecture 6, Slide 1

Lecture 6 Fiber Optical Communication Lecture 6, Slide 1 Lecture 6 Optical transmitters Photon processes in light matter interaction Lasers Lasing conditions The rate equations CW operation Modulation response Noise Light emitting diodes (LED) Power Modulation

More information

AMELIORATION DES PERFORMANCES DES LASERS A CASCADE QUANTIQUE - ETUDE DU CONFINEMENT OPTIQUE ET DES PROPRIETES THERMIQUES

AMELIORATION DES PERFORMANCES DES LASERS A CASCADE QUANTIQUE - ETUDE DU CONFINEMENT OPTIQUE ET DES PROPRIETES THERMIQUES AMELIORATION DES PERFORMANCES DES LASERS A CASCADE QUANTIQUE - ETUDE DU CONFINEMENT OPTIQUE ET DES PROPRIETES THERMIQUES Jean-Yves Bengloan To cite this version: Jean-Yves Bengloan. AMELIORATION DES PERFORMANCES

More information

Optodevice Data Book ODE I. Rev.9 Mar Opnext Japan, Inc.

Optodevice Data Book ODE I. Rev.9 Mar Opnext Japan, Inc. Optodevice Data Book ODE-408-001I Rev.9 Mar. 2003 Opnext Japan, Inc. Section 1 Operating Principles 1.1 Operating Principles of Laser Diodes (LDs) and Infrared Emitting Diodes (IREDs) 1.1.1 Emitting Principles

More information

Introduction to Optoelectronic Devices

Introduction to Optoelectronic Devices Introduction to Optoelectronic Devices Dr. Jing Bai Assistant Professor Department of Electrical and Computer Engineering University of Minnesota Duluth October 30th, 2012 1 Outline What is the optoelectronics?

More information

Lecture 18: Photodetectors

Lecture 18: Photodetectors Lecture 18: Photodetectors Contents 1 Introduction 1 2 Photodetector principle 2 3 Photoconductor 4 4 Photodiodes 6 4.1 Heterojunction photodiode.................... 8 4.2 Metal-semiconductor photodiode................

More information

Sub 300 nm Wavelength III-Nitride Tunnel-Injected Ultraviolet LEDs

Sub 300 nm Wavelength III-Nitride Tunnel-Injected Ultraviolet LEDs Sub 300 nm Wavelength III-Nitride Tunnel-Injected Ultraviolet LEDs Yuewei Zhang, Sriram Krishnamoorthy, Fatih Akyol, Sadia Monika Siddharth Rajan ECE, The Ohio State University Andrew Allerman, Michael

More information

Functional Materials. Optoelectronic devices

Functional Materials. Optoelectronic devices Functional Materials Lecture 2: Optoelectronic materials and devices (inorganic). Photonic materials Optoelectronic devices Light-emitting diode (LED) displays Photodiode and Solar cell Photoconductive

More information

Luminous Equivalent of Radiation

Luminous Equivalent of Radiation Intensity vs λ Luminous Equivalent of Radiation When the spectral power (p(λ) for GaP-ZnO diode has a peak at 0.69µm) is combined with the eye-sensitivity curve a peak response at 0.65µm is obtained with

More information

Active mode locking of quantum cascade lasers operating in external ring. cavity

Active mode locking of quantum cascade lasers operating in external ring. cavity Active mode locking of quantum cascade lasers operating in external ring cavity D.G. Revin* 1, M. Hemingway 1, Y. Wang 2, J.W. Cockburn 1, A. Belyanin 2 1 Physics and Astronomy Department, The University

More information

A continuous-wave Raman silicon laser

A continuous-wave Raman silicon laser A continuous-wave Raman silicon laser Haisheng Rong, Richard Jones,.. - Intel Corporation Ultrafast Terahertz nanoelectronics Lab Jae-seok Kim 1 Contents 1. Abstract 2. Background I. Raman scattering II.

More information

Abstract submitted to SPIE Photonics West 2017, San Francisco, CA. For publisher s version please see:

Abstract submitted to SPIE Photonics West 2017, San Francisco, CA. For publisher s version please see: Multi-heterodyne spectroscopy using Fabry-Perot interband cascade lasers for trace gas detection a feasibility assessment C. L. Patrick a, L.A. Sterczewski ac, J. Westberg a, W. W. Bewley b, C. D. Merritt

More information

LASER Transmitters 1 OBJECTIVE 2 PRE-LAB

LASER Transmitters 1 OBJECTIVE 2 PRE-LAB LASER Transmitters 1 OBJECTIVE Investigate the L-I curves and spectrum of a FP Laser and observe the effects of different cavity characteristics. Learn to perform parameter sweeps in OptiSystem. 2 PRE-LAB

More information

Widely tunable mode-hop free external cavity quantum cascade laser for high resolution spectroscopic applications

Widely tunable mode-hop free external cavity quantum cascade laser for high resolution spectroscopic applications Appl. Phys. B 81, 769 777 (2005) DOI: 10.1007/s00340-005-1965-4 Applied Physics B Lasers and Optics g. wysocki 1, r.f. curl 1 f.k. tittel 1 r. maulini 2 j.m. bulliard 2 j. faist 2 Widely tunable mode-hop

More information

High brightness semiconductor lasers M.L. Osowski, W. Hu, R.M. Lammert, T. Liu, Y. Ma, S.W. Oh, C. Panja, P.T. Rudy, T. Stakelon and J.E.

High brightness semiconductor lasers M.L. Osowski, W. Hu, R.M. Lammert, T. Liu, Y. Ma, S.W. Oh, C. Panja, P.T. Rudy, T. Stakelon and J.E. QPC Lasers, Inc. 2007 SPIE Photonics West Paper: Mon Jan 22, 2007, 1:20 pm, LASE Conference 6456, Session 3 High brightness semiconductor lasers M.L. Osowski, W. Hu, R.M. Lammert, T. Liu, Y. Ma, S.W. Oh,

More information

A Phase-Locked Terahertz Quantum Cascade Laser

A Phase-Locked Terahertz Quantum Cascade Laser A Phase-Locked Terahertz Quantum Cascade Laser A.L. Betz, R.T. Boreiko Center for Astrophysics & Space Astronomy, UCB 593, University of Colorado, Boulder, CO 80309 B. S. Williams, S. Kumar, and Q. Hu

More information

Distributed-feedback quantum cascade laser emitting at 3.2 μm

Distributed-feedback quantum cascade laser emitting at 3.2 μm Distributed-feedback quantum cascade laser emitting at 3.2 μm Johanna M. Wolf,, Alfredo Bismuto, 2 Mattias Beck and Jérôme Faist Institute for Quantum Electronics, ETH-Zurich, CH-893 Zurich, Switzerland

More information

High Power AlGaInAs/InP Widely Wavelength Tunable Laser

High Power AlGaInAs/InP Widely Wavelength Tunable Laser Special Issue Optical Communication High Power AlGaInAs/InP Widely Wavelength Tunable Laser Norihiro Iwai* 1, Masaki Wakaba* 1, Kazuaki Kiyota* 3, Tatsuro Kurobe* 1, Go Kobayashi* 4, Tatsuya Kimoto* 3,

More information

Optoelectronics ELEC-E3210

Optoelectronics ELEC-E3210 Optoelectronics ELEC-E3210 Lecture 4 Spring 2016 Outline 1 Lateral confinement: index and gain guiding 2 Surface emitting lasers 3 DFB, DBR, and C3 lasers 4 Quantum well lasers 5 Mode locking P. Bhattacharya:

More information

AIR-COUPLED PHOTOCONDUCTIVE ANTENNAS

AIR-COUPLED PHOTOCONDUCTIVE ANTENNAS AIR-COUPLED PHOTOCONDUCTIVE ANTENNAS Report: Air-Coupled Photoconductive Antennas In this paper, we present air-coupled terahertz photoconductive antenna (THz-PCAs) transmitters and receivers made on high-resistive

More information

Long wavelength electrically pumped GaSb-based Buried Tunnel Junction VCSELs

Long wavelength electrically pumped GaSb-based Buried Tunnel Junction VCSELs Available online at www.sciencedirect.com Physics Physics Procedia Procedia 3 (2010) 00 (2009) 1155 1159 000 000 www.elsevier.com/locate/procedia 14 th International Conference on Narrow Gap Semiconductors

More information

NGS-13, Guildford UK, July 2007

NGS-13, Guildford UK, July 2007 NGS-1, Guildford UK, July 7 Semiconductor light emitters for mid-ir spectral region -based Quantum Cascade Room temperature operated type-i QW -based light emitters with wavelength up to.4um L. Shterengas,

More information

Photomixing THz Spectrometer Review

Photomixing THz Spectrometer Review Photomixing THz Spectrometer Review Joseph R. Demers, PhD 9/29/2015 Leveraging Telecom Manufacturing Techniques to Improve THz Technology Terahertz Spectrum THz radiation was difficult to produce and detect

More information

Review of Semiconductor Physics

Review of Semiconductor Physics Review of Semiconductor Physics k B 1.38 u 10 23 JK -1 a) Energy level diagrams showing the excitation of an electron from the valence band to the conduction band. The resultant free electron can freely

More information

Basic concepts. Optical Sources (b) Optical Sources (a) Requirements for light sources (b) Requirements for light sources (a)

Basic concepts. Optical Sources (b) Optical Sources (a) Requirements for light sources (b) Requirements for light sources (a) Optical Sources (a) Optical Sources (b) The main light sources used with fibre optic systems are: Light-emitting diodes (LEDs) Semiconductor lasers (diode lasers) Fibre laser and other compact solid-state

More information

This article appeared in a journal published by Elsevier. The attached copy is furnished to the author for internal non-commercial research and

This article appeared in a journal published by Elsevier. The attached copy is furnished to the author for internal non-commercial research and This article appeared in a journal published by Elsevier. The attached copy is furnished to the author for internal non-commercial research and education use, including for instruction at the authors institution

More information

Ph 77 ADVANCED PHYSICS LABORATORY ATOMIC AND OPTICAL PHYSICS

Ph 77 ADVANCED PHYSICS LABORATORY ATOMIC AND OPTICAL PHYSICS Ph 77 ADVANCED PHYSICS LABORATORY ATOMIC AND OPTICAL PHYSICS Diode Laser Characteristics I. BACKGROUND Beginning in the mid 1960 s, before the development of semiconductor diode lasers, physicists mostly

More information

ECE 340 Lecture 29 : LEDs and Lasers Class Outline:

ECE 340 Lecture 29 : LEDs and Lasers Class Outline: ECE 340 Lecture 29 : LEDs and Lasers Class Outline: Light Emitting Diodes Lasers Semiconductor Lasers Things you should know when you leave Key Questions What is an LED and how does it work? How does a

More information

Recent Results from Broadly Tunable External Cavity Quantum Cascade Lasers

Recent Results from Broadly Tunable External Cavity Quantum Cascade Lasers Recent Results from Broadly Tunable External Cavity Quantum Cascade Lasers By Dave Caffey 1, Michael B. Radunsky 1,*, Vince Cook 1, Miles Weida 1, Peter R. Buerki 1, Sam Crivello 1 and Timothy Day 1 ABSTRACT

More information

Key Questions. What is an LED and how does it work? How does a laser work? How does a semiconductor laser work? ECE 340 Lecture 29 : LEDs and Lasers

Key Questions. What is an LED and how does it work? How does a laser work? How does a semiconductor laser work? ECE 340 Lecture 29 : LEDs and Lasers Things you should know when you leave Key Questions ECE 340 Lecture 29 : LEDs and Class Outline: What is an LED and how does it How does a laser How does a semiconductor laser How do light emitting diodes

More information

Semiconductor Lasers Semiconductors were originally pumped by lasers or e-beams First diode types developed in 1962: Create a pn junction in

Semiconductor Lasers Semiconductors were originally pumped by lasers or e-beams First diode types developed in 1962: Create a pn junction in Semiconductor Lasers Semiconductors were originally pumped by lasers or e-beams First diode types developed in 1962: Create a pn junction in semiconductor material Pumped now with high current density

More information

arxiv: v1 [physics.optics] 8 Dec 2017

arxiv: v1 [physics.optics] 8 Dec 2017 Watt-level widely tunable single-mode emission by injection-locking of a multimode Fabry-Perot quantum cascade laser Paul Chevalier, 1 Marco Piccardo, 1 Sajant Anand, 1, 2 Enrique A. Mejia, 1, 3 Yongrui

More information

Semiconductor Optical Communication Components and Devices Lecture 18: Introduction to Diode Lasers - I

Semiconductor Optical Communication Components and Devices Lecture 18: Introduction to Diode Lasers - I Semiconductor Optical Communication Components and Devices Lecture 18: Introduction to Diode Lasers - I Prof. Utpal Das Professor, Department of lectrical ngineering, Laser Technology Program, Indian Institute

More information

Optical MEMS in Compound Semiconductors Advanced Engineering Materials, Cal Poly, SLO November 16, 2007

Optical MEMS in Compound Semiconductors Advanced Engineering Materials, Cal Poly, SLO November 16, 2007 Optical MEMS in Compound Semiconductors Advanced Engineering Materials, Cal Poly, SLO November 16, 2007 Outline Brief Motivation Optical Processes in Semiconductors Reflectors and Optical Cavities Diode

More information

Novel Integrable Semiconductor Laser Diodes

Novel Integrable Semiconductor Laser Diodes Novel Integrable Semiconductor Laser Diodes J.J. Coleman University of Illinois 1998-1999 Distinguished Lecturer Series IEEE Lasers and Electro-Optics Society Definition of the Problem Why aren t conventional

More information

GaSb based high power single spatial mode and distributed feedback lasers at 2.0 μm

GaSb based high power single spatial mode and distributed feedback lasers at 2.0 μm GaSb based high power single spatial mode and distributed feedback lasers at 2.0 μm Clifford Frez 1, Kale J. Franz 1, Alexander Ksendzov, 1 Jianfeng Chen 2, Leon Sterengas 2, Gregory L. Belenky 2, Siamak

More information

High-frequency tuning of high-powered DFB MOPA system with diffraction limited power up to 1.5W

High-frequency tuning of high-powered DFB MOPA system with diffraction limited power up to 1.5W High-frequency tuning of high-powered DFB MOPA system with diffraction limited power up to 1.5W Joachim Sacher, Richard Knispel, Sandra Stry Sacher Lasertechnik GmbH, Hannah Arendt Str. 3-7, D-3537 Marburg,

More information

DIODE LASER SPECTROSCOPY (160309)

DIODE LASER SPECTROSCOPY (160309) DIODE LASER SPECTROSCOPY (160309) Introduction The purpose of this laboratory exercise is to illustrate how we may investigate tiny energy splittings in an atomic system using laser spectroscopy. As an

More information

Tapered Amplifiers. For Amplification of Seed Sources or for External Cavity Laser Setups. 750 nm to 1070 nm COHERENT.COM DILAS.

Tapered Amplifiers. For Amplification of Seed Sources or for External Cavity Laser Setups. 750 nm to 1070 nm COHERENT.COM DILAS. Tapered Amplifiers For Amplification of Seed Sources or for External Cavity Laser Setups 750 nm to 1070 nm COHERENT.COM DILAS.COM Welcome DILAS Semiconductor is now part of Coherent Inc. With operations

More information

Modulation of light. Direct modulation of sources Electro-absorption (EA) modulators

Modulation of light. Direct modulation of sources Electro-absorption (EA) modulators Modulation of light Direct modulation of sources Electro-absorption (EA) modulators Why Modulation A communication link is established by transmission of information reliably Optical modulation is embedding

More information

Figure 1. Schematic diagram of a Fabry-Perot laser.

Figure 1. Schematic diagram of a Fabry-Perot laser. Figure 1. Schematic diagram of a Fabry-Perot laser. Figure 1. Shows the structure of a typical edge-emitting laser. The dimensions of the active region are 200 m m in length, 2-10 m m lateral width and

More information

Lecture 5: Introduction to Lasers

Lecture 5: Introduction to Lasers Lecture 5: Introduction to Lasers http://en.wikipedia.org/wiki/laser History of the Laser v Invented in 1958 by Charles Townes (Nobel prize in Physics 1964) and Arthur Schawlow of Bell Laboratories v Was

More information

High Efficiency, Low Power-Consumption DFB Quantum Cascade Lasers Without Lateral Regrowth

High Efficiency, Low Power-Consumption DFB Quantum Cascade Lasers Without Lateral Regrowth Jia et al. Nanoscale Research Letters (2017) 12:281 DOI 10.1186/s11671-017-2064-2 NANO EXPRESS High Efficiency, Low Power-Consumption DFB Quantum Cascade Lasers Without Lateral Regrowth Zhi-Wei Jia 1,2,

More information

High-Speed Directly Modulated Lasers

High-Speed Directly Modulated Lasers High-Speed Directly Modulated Lasers Tsuyoshi Yamamoto Fujitsu Laboratories Ltd. Some parts of the results in this presentation belong to Next-generation High-efficiency Network Device Project, which Photonics

More information

Ultra-sensitive, room-temperature THz detector using nonlinear parametric upconversion

Ultra-sensitive, room-temperature THz detector using nonlinear parametric upconversion 15 th Coherent Laser Radar Conference Ultra-sensitive, room-temperature THz detector using nonlinear parametric upconversion M. Jalal Khan Jerry C. Chen Z-L Liau Sumanth Kaushik Ph: 781-981-4169 Ph: 781-981-3728

More information

Progress on High Power Single Frequency Fiber Amplifiers at 1mm, 1.5mm and 2mm

Progress on High Power Single Frequency Fiber Amplifiers at 1mm, 1.5mm and 2mm Nufern, East Granby, CT, USA Progress on High Power Single Frequency Fiber Amplifiers at 1mm, 1.5mm and 2mm www.nufern.com Examples of Single Frequency Platforms at 1mm and 1.5mm and Applications 2 Back-reflection

More information

R. J. Jones Optical Sciences OPTI 511L Fall 2017

R. J. Jones Optical Sciences OPTI 511L Fall 2017 R. J. Jones Optical Sciences OPTI 511L Fall 2017 Semiconductor Lasers (2 weeks) Semiconductor (diode) lasers are by far the most widely used lasers today. Their small size and properties of the light output

More information

Semiconductor Lasers Semiconductors were originally pumped by lasers or e-beams First diode types developed in 1962: Create a pn junction in

Semiconductor Lasers Semiconductors were originally pumped by lasers or e-beams First diode types developed in 1962: Create a pn junction in Semiconductor Lasers Semiconductors were originally pumped by lasers or e-beams First diode types developed in 1962: Create a pn junction in semiconductor material Pumped now with high current density

More information

Wavelength switching using multicavity semiconductor laser diodes

Wavelength switching using multicavity semiconductor laser diodes Wavelength switching using multicavity semiconductor laser diodes A. P. Kanjamala and A. F. J. Levi Department of Electrical Engineering University of Southern California Los Angeles, California 989-1111

More information

THz quantum cascade lasers with wafer bonded active regions

THz quantum cascade lasers with wafer bonded active regions THz quantum cascade lasers with wafer bonded active regions M. Brandstetter, 1, C. Deutsch, 1 A. Benz, 1 G. D. Cole, 2 H. Detz, 3 A. M. Andrews, 3 W. Schrenk, 3 G. Strasser, 3 and K. Unterrainer 1 1 Photonics

More information

Coupling terahertz radiation between sub-wavelength metal-metal waveguides and free space using monolithically integrated horn antennae

Coupling terahertz radiation between sub-wavelength metal-metal waveguides and free space using monolithically integrated horn antennae Coupling terahertz radiation between sub-wavelength metal-metal waveguides and free space using monolithically integrated horn antennae J. Lloyd-Hughes, G. Scalari, A. van Kolck, M. Fischer, M. Beck and

More information

High resolution cavity-enhanced absorption spectroscopy with a mode comb.

High resolution cavity-enhanced absorption spectroscopy with a mode comb. CRDS User meeting Cork University, sept-2006 High resolution cavity-enhanced absorption spectroscopy with a mode comb. T. Gherman, S. Kassi, J. C. Vial, N. Sadeghi, D. Romanini Laboratoire de Spectrométrie

More information

Investigation of the tapered waveguide structures for terahertz quantum cascade lasers

Investigation of the tapered waveguide structures for terahertz quantum cascade lasers Invited Paper Investigation of the tapered waveguide structures for terahertz quantum cascade lasers T. H. Xu, and J. C. Cao * Key Laboratory of Terahertz Solid-State Technology, Shanghai Institute of

More information

Intersubband spectroscopy of electron tunneling in GaN/AlN coupled quantum wells

Intersubband spectroscopy of electron tunneling in GaN/AlN coupled quantum wells Intersubband spectroscopy of electron tunneling in GaN/AlN coupled quantum wells N. Kheirodin, L. Nevou, M. Tchernycheva, F. H. Julien, A. Lupu, P. Crozat, L. Meignien, E. Warde, L.Vivien Institut d Electronique

More information

UNMATCHED OUTPUT POWER AND TUNING RANGE

UNMATCHED OUTPUT POWER AND TUNING RANGE ARGOS MODEL 2400 SF SERIES TUNABLE SINGLE-FREQUENCY MID-INFRARED SPECTROSCOPIC SOURCE UNMATCHED OUTPUT POWER AND TUNING RANGE One of Lockheed Martin s innovative laser solutions, Argos TM Model 2400 is

More information

S Optical Networks Course Lecture 2: Essential Building Blocks

S Optical Networks Course Lecture 2: Essential Building Blocks S-72.3340 Optical Networks Course Lecture 2: Essential Building Blocks Edward Mutafungwa Communications Laboratory, Helsinki University of Technology, P. O. Box 2300, FIN-02015 TKK, Finland Tel: +358 9

More information

Laser Diode. Photonic Network By Dr. M H Zaidi

Laser Diode. Photonic Network By Dr. M H Zaidi Laser Diode Light emitters are a key element in any fiber optic system. This component converts the electrical signal into a corresponding light signal that can be injected into the fiber. The light emitter

More information

Recent Advances in Infrared Semiconductor Laser based Chemical Sensing Technologies

Recent Advances in Infrared Semiconductor Laser based Chemical Sensing Technologies Recent Advances in Infrared Semiconductor Laser based Chemical Sensing Technologies F.K. Tittel, R.F. Curl, L. Dong, J.H. Doty, A.A. Kosterev, R. Lewicki, D. Thomazy, and G.Wysocki Abstract Recent advances

More information

Graded P-AlGaN Superlattice for Reduced Electron Leakage in Tunnel- Injected UVC LEDs

Graded P-AlGaN Superlattice for Reduced Electron Leakage in Tunnel- Injected UVC LEDs Graded P-AlGaN Superlattice for Reduced Electron Leakage in Tunnel- Injected UVC LEDs Yuewei Zhang, Sriram Krishnamoorthy, Fatih Akyol, Zane Jamal-Eddine Siddharth Rajan ECE, The Ohio State University

More information

VCSELs for gas sensing

VCSELs for gas sensing Long-wavelength VCSELs for gas sensing A. Sirbu*, A.Caliman *, V.Iakovlev ", A. Mereuta *, G. Suruceanu " and E. Kapon *" * Laboratory of Physics of Nanostructures, EPFL, 1015 Lausanne, Switzerland " BeamExpress,

More information

Thermal management and thermal properties of high-brightness diode lasers

Thermal management and thermal properties of high-brightness diode lasers Thermal management and thermal properties of high-brightness diode lasers Jens W. Tomm Max-Born-Institut für Nichtlineare Optik und Kurzzeitspektroskopie Berlin Max-Born-Str. 2 A, D-12489 Berlin, Germany

More information

HIGH BANDWIDTH DFB LASERS

HIGH BANDWIDTH DFB LASERS HIGH BANDWIDTH DFB LASERS 7-pin k-package AA71 SERIES The AA71 distributed feedback laser (DFB) is an InGaAsP/InP multi-quantum well laser diode. The module is ideal in applications where high bandwidth,

More information

of-the-art Terahertz astronomy detectors Dr. Ir. Gert de Lange

of-the-art Terahertz astronomy detectors Dr. Ir. Gert de Lange State-of of-the-art Terahertz astronomy detectors Dr. Ir. Gert de Lange Outline Introduction SRON Origin, interest and challenges in (space) THz radiation Technology Heterodyne mixers Local oscillators

More information

Investigation of InGaAsP/InP DFB and FP Laser Diodes Noise Characteristic

Investigation of InGaAsP/InP DFB and FP Laser Diodes Noise Characteristic ISSN 9 MATERIALS SCIENCE (MEDŽIAGOTYRA). Vol., No. 4. 4 Investigation of InGaAsP/InP DFB and FP Laser Diodes Noise Characteristic Jonas MATUKAS, Vilius PALENSKIS, Sandra PRALGAUSKAITĖ, Emilis ŠERMUKŠNIS

More information

Lecture 4 Fiber Optical Communication Lecture 4, Slide 1

Lecture 4 Fiber Optical Communication Lecture 4, Slide 1 Lecture 4 Optical transmitters Photon processes in light matter interaction Lasers Lasing conditions The rate equations CW operation Modulation response Noise Light emitting diodes (LED) Power Modulation

More information

Wavelength modulation spectroscopy based on quasi-continuous-wave diode lasers

Wavelength modulation spectroscopy based on quasi-continuous-wave diode lasers Wavelength modulation spectroscopy based on quasi-continuous-wave diode lasers Rubin Qi ( Í), Zhenhui Du ( ï), Dongyu Gao (Ôü ), Jinyi Li (Ó þ), and Kexin Xu (Å ) State Key Laboratory of Precision Measuring

More information

Lecture 4 INTEGRATED PHOTONICS

Lecture 4 INTEGRATED PHOTONICS Lecture 4 INTEGRATED PHOTONICS What is photonics? Photonic applications use the photon in the same way that electronic applications use the electron. Devices that run on light have a number of advantages

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION Electrically pumped continuous-wave III V quantum dot lasers on silicon Siming Chen 1 *, Wei Li 2, Jiang Wu 1, Qi Jiang 1, Mingchu Tang 1, Samuel Shutts 3, Stella N. Elliott 3, Angela Sobiesierski 3, Alwyn

More information

NIST EUVL Metrology Programs

NIST EUVL Metrology Programs NIST EUVL Metrology Programs S.Grantham, C. Tarrio, R.E. Vest, Y. Barad, S. Kulin, K. Liu and T.B. Lucatorto National Institute of Standards and Technology (NIST) Gaithersburg, MD USA L. Klebanoff and

More information

TECHNICAL BRIEF O K I L A S E R D I O D E P R O D U C T S. OKI Laser Diodes

TECHNICAL BRIEF O K I L A S E R D I O D E P R O D U C T S. OKI Laser Diodes TECHNICAL BRIEF O K I L A S E R D I O D E P R O D U C T S OKI Laser Diodes June 1995 OKI Laser Diodes INTRODUCTION This technical brief presents an overview of OKI laser diode and edge emitting light emitting

More information

Innovative and World Leading Laser Solutions from VERTILAS GmbH. Lasers with High Performance and Ultra Low Power Consumption for Green Photonics

Innovative and World Leading Laser Solutions from VERTILAS GmbH. Lasers with High Performance and Ultra Low Power Consumption for Green Photonics Lasers for Green Photonics Innovative and World Leading Laser Solutions from VERTILAS GmbH Lasers with High Performance and Ultra Low Power Consumption for Green Photonics VERTILAS GmbH, headquartered

More information

USAF Applications for Quantum Cascade Lasers. Dr. Thomas R. Nelson AFRL/Sensors Directorate 6 September 2006

USAF Applications for Quantum Cascade Lasers. Dr. Thomas R. Nelson AFRL/Sensors Directorate 6 September 2006 USAF Applications for Quantum Cascade Lasers Dr. Thomas R. Nelson AFRL/Sensors Directorate 6 September 2006 Outline Brief AFRL overview THz QCL application areas Mid-IR QCL application areas Overview of

More information

Examination Optoelectronic Communication Technology. April 11, Name: Student ID number: OCT1 1: OCT 2: OCT 3: OCT 4: Total: Grade:

Examination Optoelectronic Communication Technology. April 11, Name: Student ID number: OCT1 1: OCT 2: OCT 3: OCT 4: Total: Grade: Examination Optoelectronic Communication Technology April, 26 Name: Student ID number: OCT : OCT 2: OCT 3: OCT 4: Total: Grade: Declaration of Consent I hereby agree to have my exam results published on

More information

Lecture 1: Course Overview. Rajeev J. Ram

Lecture 1: Course Overview. Rajeev J. Ram Lecture 1: Course Overview Rajeev J. Ram Office: 36-491 Telephone: X3-4182 Email: rajeev@mit.edu Syllabus Basic concepts Advanced concepts Background: p-n junctions Photodetectors Modulators Optical amplifiers

More information

OCIS codes: ( ) Lasers and laser optics; ( ) Spectroscopy.

OCIS codes: ( ) Lasers and laser optics; ( ) Spectroscopy. Time-resolved spectral characterization of ring cavity surface emitting and ridge-type distributed feedback quantum cascade lasers by step-scan FT-IR spectroscopy Markus Brandstetter, 1,4 Andreas Genner,

More information

EYP-DFB BFY02-0x0x

EYP-DFB BFY02-0x0x 102 26.06.2014 DATA SHEET Revision 1.02 26.06.2014 page 1 from 5 General Product Information Product Application 760 nm DFB Laser with hermetic Butterfly Housing Spectroscopy Monitor Diode, Thermoelectric

More information

EE 230: Optical Fiber Communication Transmitters

EE 230: Optical Fiber Communication Transmitters EE 230: Optical Fiber Communication Transmitters From the movie Warriors of the Net Laser Diode Structures Most require multiple growth steps Thermal cycling is problematic for electronic devices Fabry

More information

A Narrow-Band Tunable Diode Laser System with Grating Feedback

A Narrow-Band Tunable Diode Laser System with Grating Feedback A Narrow-Band Tunable Diode Laser System with Grating Feedback S.P. Spirydovich Draft Abstract The description of diode laser was presented. The tuning laser system was built and aligned. The free run

More information

Phase-locked array of quantum cascade lasers with an

Phase-locked array of quantum cascade lasers with an Phase-locked array of quantum cascade lasers with an intracavity spatial filter Lei Wang 1, Jinchuan Zhang 1 *, Zhiwei Jia 1, Yue Zhao 1, Chuanwei Liu 1, Yinghui Liu 1, Shenqiang Zhai 1, Zhuo Ning 1, Fengqi

More information

Analysis of optical signal propagation through free space optical medium

Analysis of optical signal propagation through free space optical medium Analysis of optical signal propagation through free space optical medium Sathyasree J 1, Sivaranjani A 2, Ashok P 3 1,2 UG Student, Department of Electronics and Communication Engineering, Prince Shri

More information

Recent advances in high-performance 2.X µm Vertical External Cavity Surface Emitting Laser (VECSEL)

Recent advances in high-performance 2.X µm Vertical External Cavity Surface Emitting Laser (VECSEL) Recent advances in high-performance 2.X µm Vertical External Cavity Surface Emitting Laser (VECSEL) Joachim Wagner*, M. Rattunde, S. Kaspar, C. Manz, A. Bächle Fraunhofer-Institut für Angewandte Festkörperphysik

More information

# 27. Intensity Noise Performance of Semiconductor Lasers

# 27. Intensity Noise Performance of Semiconductor Lasers # 27 Intensity Noise Performance of Semiconductor Lasers Test report: Intensity noise performance of semiconductor lasers operated by the LDX-3232 current source Dr. Tobias Gensty Prof. Dr. Wolfgang Elsässer

More information

HIGH POWER DFB LASERS

HIGH POWER DFB LASERS HIGH POWER DFB LASERS Single frequency lasers in 14-pin butterfly package AA1401 SERIES INCLUDING AA1402, AA1406, AA1408, and AA1415 The Gooch & Housego high power distributed feedback laser (DFB) is an

More information

VERTICAL CAVITY SURFACE EMITTING LASER

VERTICAL CAVITY SURFACE EMITTING LASER VERTICAL CAVITY SURFACE EMITTING LASER Nandhavel International University Bremen 1/14 Outline Laser action, optical cavity (Fabry Perot, DBR and DBF) What is VCSEL? How does VCSEL work? How is it different

More information

Intracavity laser absorption spectroscopy using mid-ir quantum cascade laser

Intracavity laser absorption spectroscopy using mid-ir quantum cascade laser Intracavity laser absorption spectroscopy using mid-ir quantum cascade laser G. Medhi a, A. V. Muravjov b, H. Saxena b, C. J. Fredricksen a, T. Brusentsova a, R. E. Peale a, O. Edwards b a Department of

More information

Terahertz Quantum Cascade Lasers and Electronics

Terahertz Quantum Cascade Lasers and Electronics Terahertz Quantum Cascade Lasers and Electronics Academic and Research Staff Professor Qing Hu Graduate Students Hans Callebaut, Erik Duerr, Steve Kohen, Kostas Konistis, Sushil Kumar, Juan Montoya, Ben

More information

Near/Mid-Infrared Heterogeneous Si Photonics

Near/Mid-Infrared Heterogeneous Si Photonics PHOTONICS RESEARCH GROUP Near/Mid-Infrared Heterogeneous Si Photonics Zhechao Wang, PhD Photonics Research Group Ghent University / imec, Belgium ICSI-9, Montreal PHOTONICS RESEARCH GROUP 1 Outline Ge-on-Si

More information

Si and InP Integration in the HELIOS project

Si and InP Integration in the HELIOS project Si and InP Integration in the HELIOS project J.M. Fedeli CEA-LETI, Grenoble ( France) ECOC 2009 1 Basic information about HELIOS HELIOS photonics ELectronics functional Integration on CMOS www.helios-project.eu

More information

Narrow line diode laser stacks for DPAL pumping

Narrow line diode laser stacks for DPAL pumping Narrow line diode laser stacks for DPAL pumping Tobias Koenning David Irwin, Dean Stapleton, Rajiv Pandey, Tina Guiney, Steve Patterson DILAS Diode Laser Inc. Joerg Neukum Outline Company overview Standard

More information

940nm Single-Mode VCSEL Part number code: 940S-0000-X001

940nm Single-Mode VCSEL Part number code: 940S-0000-X001 940nm Single-Mode VCSEL Part number code: 940S-0000-X001 PRODUCT DESCRIPTION A single transverse mode 940nm VCSEL, with linear polarized emission. Features include low power consumption, linear polarization

More information

Visible Superluminescent LEDs for Smart Lighting

Visible Superluminescent LEDs for Smart Lighting Visible Superluminescent LEDs for Smart Lighting M. Duelk, M.Rossetti, A. Castiglia, M. Malinverni, N. Matuschek, C. Vélez EXALOS AG, 8952 Schlieren, Switzerland J.-F. Carlin, N. Grandjean Ecole Polytechnique

More information

sensors ISSN by MDPI

sensors ISSN by MDPI Sensors 2006, 6, 1411-1419 Review sensors ISSN 1424-8220 2006 by MDPI http://www.mdpi.org/sensors Photoacoustic Spectroscopy with Quantum Cascade Lasers for Trace Gas Detection Angela Elia *, Cinzia Di

More information