DBR LASER INTERCONNECT Simulation

Size: px
Start display at page:

Download "DBR LASER INTERCONNECT Simulation"

Transcription

1 DBR LASER INTERCONNECT Simulation High-Speed Circuits & Systems Lab. Dept. of Electrical and Electronic Engineering Optoelectronics (17/2) Page 1

2 Lumerical Solutions 3D Maxwell solver(fdtd) Modal analysis(mode) Hierarchical Simulation(INTERCONNECT) Please download 2016b version! Optoelectronics (17/2) Page 2

3 License setup Optoelectronics (17/2) Page 3

4 INTERCONNECT Window Element Library Schematic Editor Property & Results View Command Window Optoelectronics (17/2) Page 4

5 Fabry-Perot(FP) Laser Several Types of LASERs Optoelectronics (17/2) Page 5

6 Simulation Setup Optoelectronics (17/2) Page 6

7 Gain Medium(TWLM) Standards :Frequency, structure of laser Properties Recombination Gain :Gain curve shape Drag & Drop Mode1 :Loss, n g, facet reflectivity Optoelectronics (17/2) Page 7

8 Structure of laser(standard) Properties of TWLM Recombination A B C A: monomolecular B: bimolecular C: Auger Optoelectronics (17/2) Page 8

9 Gain shape Properties of TWLM,, Mode setting Γ Reflectivity Facet reflectivity can be used for Febry-Perot laser simulation Gain spectrum Optoelectronics (17/2) Page 9

10 DC source Gain spectrum and LI curve Optical power meter Simulate, and sweep setup! Sweep DC amplitude, save result of power Optoelectronics (17/2) Page 10

11 Gain spectrum Click run TWLM gain curve Right click and Visualize Click here and click object to view result FP Laser s gain spectrum Optoelectronics (17/2) Page 11

12 Sweep setup for LI curve Right click visualize OPWM Mode1 Power LI curve!!! To set output power as sweep output parameter, you have to run simulation first. Optoelectronics (17/2) Page 12

13 Febry-Perot Laser Schematic Optical Spectrum Analyzer (Frequency-domain result) 0.05 DC Source Analyzers Optical Optical Spectrum Analyzer Optical Oscilloscope (Time-domain result) Analyzers Optical Optical Oscilloscope Carrier density Oscilloscope (Time-domain result) Analyzers Electrical Oscilloscope Optoelectronics (17/2) Page 13

14 Gain spectrum FP Laser Simulation Results Same result Optoelectronics (17/2) Page 14

15 FP Laser Simulation Results OSA Optical Oscilloscope(Mode1) Electrical Oscilloscope Optoelectronics (17/2) Page 15

16 Distributed Bragg Reflector LASER Single-mode by Bragg grating structure Phase tuning region can be controlled with another DC bias Optoelectronics (17/2) Page 16

17 DBR Laser Schematic R=0 R=0.3 Bragg-grating Phase tuning Waveguide Gain medium Each response analysis is necessary Grating response, FP response(gain medium + waveguide + phase tuning) Optoelectronics (17/2) Page 17

18 Bragg Grating Optical Network Analyzer (Gain simulation) Optical Network Analyzer setup Bragg Grating setup Waveguide Gratings Bragg Grating Optoelectronics (17/2) Page 18

19 Bragg Grating Simulation Result Click ONA Result View Input1 Mode1 plot gain Optoelectronics (17/2) Page 19

20 DBR Laser DC=0 (No pumping) R=0 R=0.3 Bragg Grating Same models in previous simulations (Bragg grating instead of mirror) Optoelectronics (17/2) Page 20

21 Model Setup Waveguide setup Waveguide Straight waveguide Optical modulator setup Modulators Optical Optical Modulator Measured Double click, edit First row: Input source Second row: n eff changes TWLM setup Same as FP simulation, but two changes ONA setup Same as Bragg grating simulation (page 16.) Spontaneous factor should be zero to clearly verify response Optoelectronics (17/2) Page 21

22 Simulation Result Click ONA Result View Input1 Mode1 plot gain Optoelectronics (17/2) Page 22

23 DBR Laser with Pumping Schematic Optical Spectrum Analyzer Source for phase tuner DC = 0.05 (Pumping) Spontaneous factor should not be zero for stimulus of lasing (0.0001) Optoelectronics (17/2) Page 23

24 Simulation Result OSA Optical Oscilloscope(Mode1) Electrical Oscilloscope Optoelectronics (17/2) Page 24

25 Phase Tuned Simulation Change DC value of phase tuner Peak frequency can be tuned with phase tuning Optoelectronics (17/2) Page 25

26 Design Exercise 3 a) With Bragg-gating frequency as THz ( nm), simulate three different gain response simulation without phase tuning. Also, plot the optical spectrum with optical pumping. Compare & analyze the result with the simulation results obtained in the class. -Bragg-grating, FP, DBR simulation b) With phase tuning, find out DC source value for highest output power at THz ( nm). Explain how to get the value. Also, analyze the simulation results with theoretical background. Due date: 22 Dec. PM B629 Optoelectronics (17/2) Page 26

DBR LASER INTERCONNECT Simulation

DBR LASER INTERCONNECT Simulation DBR LASER INTERCONNECT Simulation High-Speed Circuits & Systems Lab. Dept. of Electrical and Electronic Engineering Optoelectronics (16/2) Page 1 Lumerical Solutions 3D Maxwell solver(fdtd) Modal analysis(mode)

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

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

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

Single-Frequency, 2-cm, Yb-Doped Silica-Fiber Laser

Single-Frequency, 2-cm, Yb-Doped Silica-Fiber Laser Single-Frequency, 2-cm, Yb-Doped Silica-Fiber Laser W. Guan and J. R. Marciante University of Rochester Laboratory for Laser Energetics The Institute of Optics Frontiers in Optics 2006 90th OSA Annual

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

CHAPTER 5 FINE-TUNING OF AN ECDL WITH AN INTRACAVITY LIQUID CRYSTAL ELEMENT

CHAPTER 5 FINE-TUNING OF AN ECDL WITH AN INTRACAVITY LIQUID CRYSTAL ELEMENT CHAPTER 5 FINE-TUNING OF AN ECDL WITH AN INTRACAVITY LIQUID CRYSTAL ELEMENT In this chapter, the experimental results for fine-tuning of the laser wavelength with an intracavity liquid crystal element

More information

GoToWebinar Housekeeping: attendee screen Lumerical Solutions, Inc.

GoToWebinar Housekeeping: attendee screen Lumerical Solutions, Inc. GoToWebinar Housekeeping: attendee screen 2012 Lumerical Solutions, Inc. GoToWebinar Housekeeping: your participation Open and hide your control panel Join audio: Choose Mic & Speakers to use VoIP Choose

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

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

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

Mode-locking and frequency beating in. compact semiconductor lasers. Michael J. Strain

Mode-locking and frequency beating in. compact semiconductor lasers. Michael J. Strain Mode-locking and frequency beating in Michael J. Strain Institute of Photonics Dept. of Physics University of Strathclyde compact semiconductor lasers Outline Pulsed lasers Mode-locking basics Semiconductor

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

Optical fiber-fault surveillance for passive optical networks in S-band operation window

Optical fiber-fault surveillance for passive optical networks in S-band operation window Optical fiber-fault surveillance for passive optical networks in S-band operation window Chien-Hung Yeh 1 and Sien Chi 2,3 1 Transmission System Department, Computer and Communications Research Laboratories,

More information

White Paper Laser Sources For Optical Transceivers. Giacomo Losio ProLabs Head of Technology

White Paper Laser Sources For Optical Transceivers. Giacomo Losio ProLabs Head of Technology White Paper Laser Sources For Optical Transceivers Giacomo Losio ProLabs Head of Technology September 2014 Laser Sources For Optical Transceivers Optical transceivers use different semiconductor laser

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

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

Agilent 81600B All-band Tunable Laser Source Technical Specifications December 2002

Agilent 81600B All-band Tunable Laser Source Technical Specifications December 2002 Agilent 81600B All-band Tunable Laser Source December 2002 The 81600B, the flagship product in Agilent s market-leading portfolio of tunable laser sources, sweeps the entire S, C and L- bands with just

More information

Chapter 1 Introduction

Chapter 1 Introduction Chapter 1 Introduction 1-1 Preface Telecommunication lasers have evolved substantially since the introduction of the early AlGaAs-based semiconductor lasers in the late 1970s suitable for transmitting

More information

Temporal coherence characteristics of a superluminescent diode system with an optical feedback mechanism

Temporal coherence characteristics of a superluminescent diode system with an optical feedback mechanism VI Temporal coherence characteristics of a superluminescent diode system with an optical feedback mechanism Fang-Wen Sheu and Pei-Ling Luo Department of Applied Physics, National Chiayi University, Chiayi

More information

Integrated into Nanowire Waveguides

Integrated into Nanowire Waveguides Supporting Information Widely Tunable Distributed Bragg Reflectors Integrated into Nanowire Waveguides Anthony Fu, 1,3 Hanwei Gao, 1,3,4 Petar Petrov, 1, Peidong Yang 1,2,3* 1 Department of Chemistry,

More information

Waveguide Bragg Gratings and Resonators LUMERICAL SOLUTIONS INC

Waveguide Bragg Gratings and Resonators LUMERICAL SOLUTIONS INC Waveguide Bragg Gratings and Resonators JUNE 2016 1 Outline Introduction Waveguide Bragg gratings Background Simulation challenges and solutions Photolithography simulation Initial design with FDTD Band

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

Air Cavity Dominant VCSELs with a Wide Wavelength Sweep

Air Cavity Dominant VCSELs with a Wide Wavelength Sweep Air Cavity Dominant VCSELs with a Wide Wavelength Sweep KEVIN T. COOK, 1 PENGFEI QIAO, 1 JIPENG QI, 1 LARRY A. COLDREN, 2 AND CONNIE J. CHANG-HASNAIN 1,* 1 Department of Electical Engineering and Computer

More information

Analysis of Self-Pulsation in Distributed Bragg Reflector Laser based on Four-Wave Mixing

Analysis of Self-Pulsation in Distributed Bragg Reflector Laser based on Four-Wave Mixing Analysis of Self-Pulsation in Distributed Bragg Reflector Laser based on Four-Wave Mixing P. Landais 1, J. Renaudier 2, P. Gallion 2 and G.-H.Duan 3 1 School of Electronic Engineering, Dublin City University,

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION Room-temperature InP distributed feedback laser array directly grown on silicon Zhechao Wang, Bin Tian, Marianna Pantouvaki, Weiming Guo, Philippe Absil, Joris Van Campenhout, Clement Merckling and Dries

More information

Simulation of a DBR Edge Emitting Laser with External Air Gap Tuning Mirror

Simulation of a DBR Edge Emitting Laser with External Air Gap Tuning Mirror Engineered Excellence A Journal for Process and Device Engineers Simulation of a DBR Edge Emitting Laser with External Air Gap Tuning Mirror Abstract A methodology for simulating an edge emitting laser

More information

DBR based passively mode-locked 1.5m semiconductor laser with 9 nm tuning range Moskalenko, V.; Williams, K.A.; Bente, E.A.J.M.

DBR based passively mode-locked 1.5m semiconductor laser with 9 nm tuning range Moskalenko, V.; Williams, K.A.; Bente, E.A.J.M. DBR based passively mode-locked 1.5m semiconductor laser with 9 nm tuning range Moskalenko, V.; Williams, K.A.; Bente, E.A.J.M. Published in: Proceedings of the 20th Annual Symposium of the IEEE Photonics

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

VCSELs and Optical Interconnects

VCSELs and Optical Interconnects VCSELs and Optical Interconnects Anders Larsson Chalmers University of Technology ADOPT Winter School on Optics and Photonics February 4-7, 6 Outline Part VCSEL basics - Physics and design - Static and

More information

Suppression of Stimulated Brillouin Scattering

Suppression of Stimulated Brillouin Scattering Suppression of Stimulated Brillouin Scattering 42 2 5 W i de l y T u n a b l e L a s e r T ra n s m i t te r www.lumentum.com Technical Note Introduction This technical note discusses the phenomenon and

More information

Tunable vertical-cavity SOAs: a unique combination of tunable filtering and optical gain

Tunable vertical-cavity SOAs: a unique combination of tunable filtering and optical gain Tunable vertical-cavity SOAs: a unique combination of tunable filtering and optical gain Garrett D. Cole Materials Dept., University of California, Santa Barbara, Santa Barbara, CA 93106-5050 ABSTRACT

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

InP-based Waveguide Photodetector with Integrated Photon Multiplication

InP-based Waveguide Photodetector with Integrated Photon Multiplication InP-based Waveguide Photodetector with Integrated Photon Multiplication D.Pasquariello,J.Piprek,D.Lasaosa,andJ.E.Bowers Electrical and Computer Engineering Department University of California, Santa Barbara,

More information

3 General Principles of Operation of the S7500 Laser

3 General Principles of Operation of the S7500 Laser Application Note AN-2095 Controlling the S7500 CW Tunable Laser 1 Introduction This document explains the general principles of operation of Finisar s S7500 tunable laser. It provides a high-level description

More information

Optical Amplifiers (Chapter 6)

Optical Amplifiers (Chapter 6) Optical Amplifiers (Chapter 6) General optical amplifier theory Semiconductor Optical Amplifier (SOA) Raman Amplifiers Erbium-doped Fiber Amplifiers (EDFA) Read Chapter 6, pp. 226-266 Loss & dispersion

More information

Swept Wavelength Testing:

Swept Wavelength Testing: Application Note 13 Swept Wavelength Testing: Characterizing the Tuning Linearity of Tunable Laser Sources In a swept-wavelength measurement system, the wavelength of a tunable laser source (TLS) is swept

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

Experimental Physics. Experiment C & D: Pulsed Laser & Dye Laser. Course: FY12. Project: The Pulsed Laser. Done by: Wael Al-Assadi & Irvin Mangwiza

Experimental Physics. Experiment C & D: Pulsed Laser & Dye Laser. Course: FY12. Project: The Pulsed Laser. Done by: Wael Al-Assadi & Irvin Mangwiza Experiment C & D: Course: FY1 The Pulsed Laser Done by: Wael Al-Assadi Mangwiza 8/1/ Wael Al Assadi Mangwiza Experiment C & D : Introduction: Course: FY1 Rev. 35. Page: of 16 1// In this experiment we

More information

Agilent 81980/ 81940A, Agilent 81989/ 81949A, Agilent 81944A Compact Tunable Laser Sources

Agilent 81980/ 81940A, Agilent 81989/ 81949A, Agilent 81944A Compact Tunable Laser Sources Agilent 81980/ 81940A, Agilent 81989/ 81949A, Agilent 81944A Compact Tunable Laser Sources December 2004 Agilent s Series 819xxA high-power compact tunable lasers enable optical device characterization

More information

Photonic Generation of Millimeter-Wave Signals With Tunable Phase Shift

Photonic Generation of Millimeter-Wave Signals With Tunable Phase Shift Photonic Generation of Millimeter-Wave Signals With Tunable Phase Shift Volume 4, Number 3, June 2012 Weifeng Zhang, Student Member, IEEE Jianping Yao, Fellow, IEEE DOI: 10.1109/JPHOT.2012.2199481 1943-0655/$31.00

More information

Gain Measurements of Fabry-Pérot InP/InGaAsP Lasers. using an Ultra High Resolution Spectrometer

Gain Measurements of Fabry-Pérot InP/InGaAsP Lasers. using an Ultra High Resolution Spectrometer Gain Measurements of Fabry-Pérot InP/InGaAsP Lasers using an Ultra High Resolution Spectrometer Y. Barbarin, E.A.J.M Bente, G. Servanton, L. Mussard, Y.S. Oei, R. Nötzel and M.K. Smit COBRA, Eindhoven

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

Revised: Summer 2010

Revised: Summer 2010 EE 2274 PRE-LAB EXPERIMENT 5 DIODE OR GATE & CLIPPING CIRCUIT COMPLETE PRIOR TO COMING TO LAB Part I: 1. Design a diode, Figure 1 OR gate in which the maximum input current,, Iin is less than 5mA. Show

More information

LASER DIODE MODULATION AND NOISE

LASER DIODE MODULATION AND NOISE > 5' O ft I o Vi LASER DIODE MODULATION AND NOISE K. Petermann lnstitutfiir Hochfrequenztechnik, Technische Universitdt Berlin Kluwer Academic Publishers i Dordrecht / Boston / London KTK Scientific Publishers

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

RADIO-OVER-FIBER TRANSPORT SYSTEMS BASED ON DFB LD WITH MAIN AND 1 SIDE MODES INJECTION-LOCKED TECHNIQUE

RADIO-OVER-FIBER TRANSPORT SYSTEMS BASED ON DFB LD WITH MAIN AND 1 SIDE MODES INJECTION-LOCKED TECHNIQUE Progress In Electromagnetics Research Letters, Vol. 7, 25 33, 2009 RADIO-OVER-FIBER TRANSPORT SYSTEMS BASED ON DFB LD WITH MAIN AND 1 SIDE MODES INJECTION-LOCKED TECHNIQUE H.-H. Lu, C.-Y. Li, C.-H. Lee,

More information

IST IP NOBEL "Next generation Optical network for Broadband European Leadership"

IST IP NOBEL Next generation Optical network for Broadband European Leadership DBR Tunable Lasers A variation of the DFB laser is the distributed Bragg reflector (DBR) laser. It operates in a similar manner except that the grating, instead of being etched into the gain medium, is

More information

THE EFFECT OF COUPLING COEFFICIENT VARIATIONS ON AN ALL OPTICAL FLIP FLOP PERFORMANCE BASED ON GAIN CLAMPED SEMICONDUCTOR OPTICAL AMPLIFIER

THE EFFECT OF COUPLING COEFFICIENT VARIATIONS ON AN ALL OPTICAL FLIP FLOP PERFORMANCE BASED ON GAIN CLAMPED SEMICONDUCTOR OPTICAL AMPLIFIER Indian J.Sci.Res. 5(2) : 9599, 2014 THE EFFECT OF COUPLING COEFFICIENT VARIATIONS ON AN ALL OPTICAL FLIP FLOP PERFORMANCE BASED ON GAIN CLAMPED SEMICONDUCTOR OPTICAL AMPLIFIER a b1 SHARAREH BASHIRAZAMI

More information

SEMICONDUCTOR lasers and amplifiers are important

SEMICONDUCTOR lasers and amplifiers are important 240 JOURNAL OF LIGHTWAVE TECHNOLOGY, VOL. 28, NO. 3, FEBRUARY 1, 2010 Temperature-Dependent Saturation Characteristics of Injection Seeded Fabry Pérot Laser Diodes/Reflective Optical Amplifiers Hongyun

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

InP-based Waveguide Photodetector with Integrated Photon Multiplication

InP-based Waveguide Photodetector with Integrated Photon Multiplication InP-based Waveguide Photodetector with Integrated Photon Multiplication D.Pasquariello,J.Piprek,D.Lasaosa,andJ.E.Bowers Electrical and Computer Engineering Department University of California, Santa Barbara,

More information

Application Instruction 002. Superluminescent Light Emitting Diodes: Device Fundamentals and Reliability

Application Instruction 002. Superluminescent Light Emitting Diodes: Device Fundamentals and Reliability I. Introduction II. III. IV. SLED Fundamentals SLED Temperature Performance SLED and Optical Feedback V. Operation Stability, Reliability and Life VI. Summary InPhenix, Inc., 25 N. Mines Road, Livermore,

More information

Photonics and Optical Communication

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

More information

EE 210 Lab Exercise #3 Introduction to PSPICE

EE 210 Lab Exercise #3 Introduction to PSPICE EE 210 Lab Exercise #3 Introduction to PSPICE Appending 4 in your Textbook contains a short tutorial on PSPICE. Additional information, tutorials and a demo version of PSPICE can be found at the manufacturer

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

Cost-effective wavelength-tunable fiber laser using self-seeding Fabry-Perot laser diode

Cost-effective wavelength-tunable fiber laser using self-seeding Fabry-Perot laser diode Cost-effective wavelength-tunable fiber laser using self-seeding Fabry-Perot laser diode Chien Hung Yeh, 1* Fu Yuan Shih, 2 Chia Hsuan Wang, 3 Chi Wai Chow, 3 and Sien Chi 2, 3 1 Information and Communications

More information

Elements of Optical Networking

Elements of Optical Networking Bruckner Elements of Optical Networking Basics and practice of optical data communication With 217 Figures, 13 Tables and 93 Exercises Translated by Patricia Joliet VIEWEG+ TEUBNER VII Content Preface

More information

Testing with Femtosecond Pulses

Testing with Femtosecond Pulses Testing with Femtosecond Pulses White Paper PN 200-0200-00 Revision 1.3 January 2009 Calmar Laser, Inc www.calmarlaser.com Overview Calmar s femtosecond laser sources are passively mode-locked fiber lasers.

More information

Application of optical system simulation software in a fiber optic telecommunications program

Application of optical system simulation software in a fiber optic telecommunications program Rochester Institute of Technology RIT Scholar Works Presentations and other scholarship 2004 Application of optical system simulation software in a fiber optic telecommunications program Warren Koontz

More information

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Electrical Engineering and Computer Science

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Electrical Engineering and Computer Science Student Name Date MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Electrical Engineering and Computer Science 6.161 Modern Optics Project Laboratory Laboratory Exercise No. 6 Fall 2010 Solid-State

More information

Performance Limitations of WDM Optical Transmission System Due to Cross-Phase Modulation in Presence of Chromatic Dispersion

Performance Limitations of WDM Optical Transmission System Due to Cross-Phase Modulation in Presence of Chromatic Dispersion Performance Limitations of WDM Optical Transmission System Due to Cross-Phase Modulation in Presence of Chromatic Dispersion M. A. Khayer Azad and M. S. Islam Institute of Information and Communication

More information

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

R. J. Jones College of Optical Sciences OPTI 511L Fall 2017 R. J. Jones College of Optical Sciences OPTI 511L Fall 2017 Active Modelocking of a Helium-Neon Laser The generation of short optical pulses is important for a wide variety of applications, from time-resolved

More information

Strong Optical Injection Locking of Edge-Emitting Lasers and Its Applications

Strong Optical Injection Locking of Edge-Emitting Lasers and Its Applications Strong Optical Injection Locking of Edge-Emitting Lasers and Its Applications Hyuk-Kee Sung Electrical Engineering and Computer Sciences University of California at Berkeley Technical Report No. UCB/EECS-2006-107

More information

Lab Reference Manual. ECEN 326 Electronic Circuits. Texas A&M University Department of Electrical and Computer Engineering

Lab Reference Manual. ECEN 326 Electronic Circuits. Texas A&M University Department of Electrical and Computer Engineering Lab Reference Manual ECEN 326 Electronic Circuits Texas A&M University Department of Electrical and Computer Engineering Contents 1. Circuit Analysis in PSpice 3 1.1 Transient and DC Analysis 3 1.2 Measuring

More information

Modifying Bragg Grating Interrogation System and Studying Corresponding Problems

Modifying Bragg Grating Interrogation System and Studying Corresponding Problems Modifying Bragg Grating Interrogation System and Studying Corresponding Problems 1998 Abstract An improved fiber Bragg grating (FBG) interrogation system is described. The system utilises time domain multiplexing

More information

Measurements of linewidth variations within external-cavity modes of a grating-cavity laser

Measurements of linewidth variations within external-cavity modes of a grating-cavity laser 15 March 2002 Optics Communications 203 (2002) 295 300 www.elsevier.com/locate/optcom Measurements of linewidth variations within external-cavity modes of a grating-cavity laser G. Genty a, *, M. Kaivola

More information

Optical Amplifiers Photonics and Integrated Optics (ELEC-E3240) Zhipei Sun Photonics Group Department of Micro- and Nanosciences Aalto University

Optical Amplifiers Photonics and Integrated Optics (ELEC-E3240) Zhipei Sun Photonics Group Department of Micro- and Nanosciences Aalto University Photonics Group Department of Micro- and Nanosciences Aalto University Optical Amplifiers Photonics and Integrated Optics (ELEC-E3240) Zhipei Sun Last Lecture Topics Course introduction Ray optics & optical

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

Technical Brief #2. Depolarizers

Technical Brief #2. Depolarizers Technical Brief #2 Depolarizers What is a depolarizer?...2 Principle of operation...2 Source coherence function dependence...2 Depolarizer realization...3 Input linear polarization state definition...4

More information

MICROWAVE photonics is an interdisciplinary area

MICROWAVE photonics is an interdisciplinary area 314 JOURNAL OF LIGHTWAVE TECHNOLOGY, VOL. 27, NO. 3, FEBRUARY 1, 2009 Microwave Photonics Jianping Yao, Senior Member, IEEE, Member, OSA (Invited Tutorial) Abstract Broadband and low loss capability of

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

A Cascaded Incoherent Spectrum Sliced Transversal Photonic Microwave Filters-An Analysis

A Cascaded Incoherent Spectrum Sliced Transversal Photonic Microwave Filters-An Analysis A Cascaded Incoherent Spectrum Sliced Transversal Photonic Microwave Filters-An Analysis R. K. JEYACHITRA 1 DR. (MRS.) R. SUKANESH 2 1. Assistant Professor, Department of Electronics and Communication

More information

Multiply Resonant EOM for the LIGO 40-meter Interferometer

Multiply Resonant EOM for the LIGO 40-meter Interferometer LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY - LIGO - CALIFORNIA INSTITUTE OF TECHNOLOGY MASSACHUSETTS INSTITUTE OF TECHNOLOGY LIGO-XXXXXXX-XX-X Date: 2009/09/25 Multiply Resonant EOM for the LIGO

More information

ASE Suppression in a Diode-Pumped Nd:YLF Regenerative Amplifier Using a Volume Bragg Grating

ASE Suppression in a Diode-Pumped Nd:YLF Regenerative Amplifier Using a Volume Bragg Grating ASE Suppression in a Diode-Pumped Nd:YLF Regenerative Amplifier Using a Volume Bragg Grating Spectral density (db) 0 10 20 30 40 Mirror VBG 1053.0 1053.3 1053.6 Wavelength (nm) Frontiers in Optics 2007/Laser

More information

Spatial Investigation of Transverse Mode Turn-On Dynamics in VCSELs

Spatial Investigation of Transverse Mode Turn-On Dynamics in VCSELs Spatial Investigation of Transverse Mode Turn-On Dynamics in VCSELs Safwat W.Z. Mahmoud Data transmission experiments with single-mode as well as multimode 85 nm VCSELs are carried out from a near-field

More information

Field Optical Spectrum Analyser

Field Optical Spectrum Analyser NEWSLETTER JANUARY 2004 5 Field Optical Spectrum Analyser There is a growing number of applications in today's telecom world involving fibre optic communications using more than one wavelength on the same

More information

S-band gain-clamped grating-based erbiumdoped fiber amplifier by forward optical feedback technique

S-band gain-clamped grating-based erbiumdoped fiber amplifier by forward optical feedback technique S-band gain-clamped grating-based erbiumdoped fiber amplifier by forward optical feedback technique Chien-Hung Yeh 1, *, Ming-Ching Lin 3, Ting-Tsan Huang 2, Kuei-Chu Hsu 2 Cheng-Hao Ko 2, and Sien Chi

More information

PERFORMANCE OF PHOTODIGM S DBR SEMICONDUCTOR LASERS FOR PICOSECOND AND NANOSECOND PULSING APPLICATIONS

PERFORMANCE OF PHOTODIGM S DBR SEMICONDUCTOR LASERS FOR PICOSECOND AND NANOSECOND PULSING APPLICATIONS PERFORMANCE OF PHOTODIGM S DBR SEMICONDUCTOR LASERS FOR PICOSECOND AND NANOSECOND PULSING APPLICATIONS By Jason O Daniel, Ph.D. TABLE OF CONTENTS 1. Introduction...1 2. Pulse Measurements for Pulse Widths

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

Degradation analysis in asymmetric sampled grating distributed feedback laser diodes

Degradation analysis in asymmetric sampled grating distributed feedback laser diodes Microelectronics Journal 8 (7) 74 74 www.elsevier.com/locate/mejo Degradation analysis in asymmetric sampled grating distributed feedback laser diodes Han Sung Joo, Sang-Wan Ryu, Jeha Kim, Ilgu Yun Semiconductor

More information

40 GHz Dual Mode-Locked Widely-Tunable Sampled-Grating DBR Laser

40 GHz Dual Mode-Locked Widely-Tunable Sampled-Grating DBR Laser 40 GHz Dual Mode-Locked Widely-Tunable Sampled-Grating DBR Laser L.A. Johansson, Zhaoyang Hu, D.J. Blumenthal and L.A. Coldren Department of Electrical and Computer Engineering, University of California,

More information

FFP-C Fiber Fabry-Perot Controller OPERATING INSTRUCTIONS. Version 1.0 MICRON OPTICS, INC.

FFP-C Fiber Fabry-Perot Controller OPERATING INSTRUCTIONS. Version 1.0 MICRON OPTICS, INC. FFP-C Fiber Fabry-Perot Controller OPERATING INSTRUCTIONS Version 1.0 MICRON OPTICS, INC. 1852 Century Place NE Atlanta, GA 30345 USA Tel (404) 325-0005 Fax (404) 325-4082 www.micronoptics.com Page 2 Table

More information

Intensity-demodulated fiber-ring laser sensor system for acoustic emission detection

Intensity-demodulated fiber-ring laser sensor system for acoustic emission detection University of Nebraska - Lincoln DigitalCommons@University of Nebraska - Lincoln Faculty Publications from the Department of Electrical and Computer Engineering Electrical & Computer Engineering, Department

More information

External-Cavity Tapered Semiconductor Ring Lasers

External-Cavity Tapered Semiconductor Ring Lasers External-Cavity Tapered Semiconductor Ring Lasers Frank Demaria Laser operation of a tapered semiconductor amplifier in a ring-oscillator configuration is presented. In first experiments, 1.75 W time-average

More information

Doppler-Free Spetroscopy of Rubidium

Doppler-Free Spetroscopy of Rubidium Doppler-Free Spetroscopy of Rubidium Pranjal Vachaspati, Sabrina Pasterski MIT Department of Physics (Dated: April 17, 2013) We present a technique for spectroscopy of rubidium that eliminates doppler

More information

Experiment No.15 DC-DC Converters

Experiment No.15 DC-DC Converters Experiment No.15 DC-DC Converters Experiment aim The aim of Experiment is to analyze the operation (Switching) of DC-DC converter with resistive load. Apparatus 1. Power electronic trainer 2. Connection

More information

Introduction Fundamental of optical amplifiers Types of optical amplifiers

Introduction Fundamental of optical amplifiers Types of optical amplifiers ECE 6323 Introduction Fundamental of optical amplifiers Types of optical amplifiers Erbium-doped fiber amplifiers Semiconductor optical amplifier Others: stimulated Raman, optical parametric Advanced application:

More information

Tunable semiconductor lasers for telecommunications applications

Tunable semiconductor lasers for telecommunications applications Tunable semiconductor lasers for telecommunications applications H. Debrégeas-Sillard, A. Plais, A. Vuong, Th. Fillion, D. Locatelli, J. Decobert, D. Herrati, P. Doussière*, J. Jacquet Alcatel CIT OPTO+,

More information

Synchronization in Chaotic Vertical-Cavity Surface-Emitting Semiconductor Lasers

Synchronization in Chaotic Vertical-Cavity Surface-Emitting Semiconductor Lasers Synchronization in Chaotic Vertical-Cavity Surface-Emitting Semiconductor Lasers Natsuki Fujiwara and Junji Ohtsubo Faculty of Engineering, Shizuoka University, 3-5-1 Johoku, Hamamatsu, 432-8561 Japan

More information

Chad A. Husko 1,, Sylvain Combrié 2, Pierre Colman 2, Jiangjun Zheng 1, Alfredo De Rossi 2, Chee Wei Wong 1,

Chad A. Husko 1,, Sylvain Combrié 2, Pierre Colman 2, Jiangjun Zheng 1, Alfredo De Rossi 2, Chee Wei Wong 1, SOLITON DYNAMICS IN THE MULTIPHOTON PLASMA REGIME Chad A. Husko,, Sylvain Combrié, Pierre Colman, Jiangjun Zheng, Alfredo De Rossi, Chee Wei Wong, Optical Nanostructures Laboratory, Columbia University

More information

Numerical analysis of a swift, high resolution wavelength monitor designed as a Generic Lightwave Integrated Chip (GLIC)

Numerical analysis of a swift, high resolution wavelength monitor designed as a Generic Lightwave Integrated Chip (GLIC) Numerical analysis of a swift, high resolution wavelength monitor designed as a Generic Lightwave Integrated Chip (GLIC) John Ging and Ronan O Dowd Optoelectronics Research Centre University College Dublin,

More information

Optical Gain Experiment Manual

Optical Gain Experiment Manual Optical Gain Experiment Manual Table of Contents Purpose 1 Scope 1 1. Background Theory 1 1.1 Absorption, Spontaneous Emission and Stimulated Emission... 2 1.2 Direct and Indirect Semiconductors... 3 1.3

More information

Trends in Optical Transceivers:

Trends in Optical Transceivers: Trends in Optical Transceivers: Light sources for premises networks Peter Ronco Corning Optical Fiber Asst. Product Line Manager Premises Fibers January 24, 2006 Outline: Introduction: Transceivers and

More information

Design of InGaAs/InP 1.55μm vertical cavity surface emitting lasers (VCSEL)

Design of InGaAs/InP 1.55μm vertical cavity surface emitting lasers (VCSEL) Design of InGaAs/InP 1.55μm vertical cavity surface emitting lasers (VCSEL) J.-M. Lamy, S. Boyer-Richard, C. Levallois, C. Paranthoën, H. Folliot, N. Chevalier, A. Le Corre, S. Loualiche UMR FOTON 6082

More information

EE 2274 DIODE OR GATE & CLIPPING CIRCUIT

EE 2274 DIODE OR GATE & CLIPPING CIRCUIT EE 2274 DIODE OR GATE & CLIPPING CIRCUIT Prelab Part I: Wired Diode OR Gate LTspice use 1N4002 1. Design a diode OR gate, Figure 1 in which the maximum current thru R1 I R1 = 9mA assume Vin = 5Vdc. Design

More information

Optoelectronics EE/OPE 451, OPT 444 Fall 2009 Section 1: T/Th 9:30-10:55 PM

Optoelectronics EE/OPE 451, OPT 444 Fall 2009 Section 1: T/Th 9:30-10:55 PM Optoelectronics EE/OPE 451, OPT 444 Fall 009 Section 1: T/Th 9:30-10:55 PM John D. Williams, Ph.D. Department of Electrical and Computer Engineering 406 Optics Building - UAHuntsville, Huntsville, AL 35899

More information

LW Technology. Passive Components. LW Technology (Passive Components).PPT - 1 Copyright 1999, Agilent Technologies

LW Technology. Passive Components. LW Technology (Passive Components).PPT - 1 Copyright 1999, Agilent Technologies LW Technology Passive Components LW Technology (Passive Components).PPT - 1 Patchcords Jumper cables to connect devices and instruments Adapter cables to connect interfaces using different connector styles

More information

Tunable single frequency fiber laser based on FP-LD injection locking

Tunable single frequency fiber laser based on FP-LD injection locking Tunable single frequency fiber laser based on FP-LD injection locking Aiqin Zhang, Xinhuan Feng, * Minggui Wan, Zhaohui Li, and Bai-ou Guan Institute of Photonics Technology, Jinan University, Guangzhou,

More information

Spectrally Compact Optical Subcarrier Multiplexing with 42.6 Gbit/s AM-PSK Payload and 2.5Gbit/s NRZ Labels

Spectrally Compact Optical Subcarrier Multiplexing with 42.6 Gbit/s AM-PSK Payload and 2.5Gbit/s NRZ Labels Spectrally Compact Optical Subcarrier Multiplexing with 42.6 Gbit/s AM-PSK Payload and 2.5Gbit/s NRZ Labels A.K. Mishra (1), A.D. Ellis (1), D. Cotter (1),F. Smyth (2), E. Connolly (2), L.P. Barry (2)

More information