Simulation and Analysis of Single Mode Semiconductor Laser

Slides:



Advertisements
Similar presentations
ECE 8443 – Pattern Recognition EE 3512 – Signals: Continuous and Discrete Objectives: Response to a Sinusoidal Input Frequency Analysis of an RC Circuit.
Advertisements

Light Waves and Polarization Xavier Fernando Ryerson Communications Lab
Presentation Overview
In Search of the “Absolute” Optical Phase
EE 230: Optical Fiber Communication Lecture 9 From the movie Warriors of the Net Light Sources.
R. Hui Photonics for bio-imaging and bio- sensing Rongqing Hui Dept. Electrical Engineering & Computer Science, The University of Kansas, Lawrence Kansas.
8. Optical Modulation. Modulation Techniques Direct modulation of laser diode –Vary the current supply to the laser diode –Directly modulates the output.
Modulation formats for digital fiber transmission
EE-2027 SaS 06-07, L11 1/12 Lecture 11: Fourier Transform Properties and Examples 3. Basis functions (3 lectures): Concept of basis function. Fourier series.
LIGO-G E LIGO Laboratory1 Simulating the LIGO Laser Phase Change Resulting from Gravitational Waves Simulate GW generation and detection Make.
Simulations of All-Optical Multiple-Input AND- Gate Based on Four Wave Mixing in a Single Semiconductor Optical Amplifier H. Le Minh, Z. Ghassemlooy, Wai.
1 The Mathematics of Signal Processing - an Innovative Approach Peter Driessen Faculty of Engineering University of Victoria.
Shock Waves & Potentials
Lecture 38 Lasers Final Exam next week. LASER L ight A mplification by S timulated E mission of R adiation.
High-speed optical switching based on diffusive conduction in an optical waveguide with surface-normal optical control V. A. Sabnis, H. V. Demir, M. B.
Optical Amplifiers An Important Element of WDM Systems Xavier Fernando ADROIT Group Ryerson University.
1 ISIS-IPHOBAC SUMMER SCHOOL, May 17-18, 2007, Budapest, Hungary "Broadband Architectures and Functions" Photonic microwave signal processing Jianping.
February 2004 Charles A. DiMarzio, Northeastern University ECEG287 Optical Detection Course Notes Part 11: Coherent Detection Profs. Charles.
Graphs of the Sine and Cosine Functions Section 6.
Coherent System in Remote Antenna Application
Analysis of Phase Noise in a fiber-optic link
Fourier (1) Hany Ferdinando Dept. of Electrical Eng. Petra Christian University.
Prof. Brian L. Evans Dept. of Electrical and Computer Engineering The University of Texas at Austin EE445S Real-Time Digital Signal Processing Lab Fall.
CLIPPING DISTORTION IN LASER DIODE: MODEL, SIMULATIONS AND STATISTICS By: Omar Falou.
Gaussian Minimum Shift Keying GMSK Software Defined Radio EE 194SDR Spring 2006 Brad Gaynor.
Femto-second Measurements of Semiconductor Laser Diodes David Baxter
EE104: Lecture 5 Outline Review of Last Lecture Introduction to Fourier Transforms Fourier Transform from Fourier Series Fourier Transform Pair and Signal.
Fourier Analysis of Discrete-Time Systems
Lecture 17: The Discrete Fourier Series Instructor: Dr. Ghazi Al Sukkar Dept. of Electrical Engineering The University of Jordan
Fourier Analysis of Signals and Systems
SIMULINK-Tutorial 1 Class ECES-304 Presented by : Shubham Bhat.
Department of Mechanical Engineering, LSUSession VII MATLAB Tutorials Session VII Introduction to SIMULINK Rajeev Madazhy
Professor Walter W. Olson Department of Mechanical, Industrial and Manufacturing Engineering University of Toledo Linear Systems m k u x m k u x Fixed.
Simulation and Analysis of Single Mode Semiconductor Laser Course Project for EE8114 Electrical Engineering Dept. Ryerson University Grace FENG Course.
© The McGraw-Hill Companies, Inc McGraw-Hill 1 PRINCIPLES AND APPLICATIONS OF ELECTRICAL ENGINEERING THIRD EDITION G I O R G I O R I Z Z O N I 8.
ECE 8443 – Pattern Recognition ECE 3163 – Signals and Systems Objectives: Frequency Response Response of a Sinusoid DT MA Filter Filter Design DT WMA Filter.
Lecture 11: EE 221: Signals Analysis and Systems Instructor: Dr. Ghazi Al Sukkar Dept. of Electrical Engineering The University of Jordan
Simulink Continuous Library by Dr. Amin Danial Asham.
EE313 Linear Systems and Signals Fall 2010 Initial conversion of content to PowerPoint by Dr. Wade C. Schwartzkopf Prof. Brian L. Evans Dept. of Electrical.
Eeng360 1 Chapter 2 Linear Systems Topics:  Review of Linear Systems Linear Time-Invariant Systems Impulse Response Transfer Functions Distortionless.
Prof. Brian L. Evans Dept. of Electrical and Computer Engineering The University of Texas at Austin Lecture 3
Date of download: 6/22/2016 Copyright © 2016 SPIE. All rights reserved. Parallel structure of DQPSK transmitter. Figure Legend: From: Generation and transmission.
Development of Instrumentation for High-Precision Position Measurement Done by: Mohamed El-Jaam Sharief Saleh Asem Khattab Mahmoud Mesleh 1 Senior Design.
Switched-mode power supply charger
Recall-Lecture 5 DC Analysis Representation of diode into three models
Four wave mixing in submicron waveguides
Recall-Lecture 4 Current generated due to two main factors
Discussion today Over the next two class periods we will be designing a ring resonator based 2-channel wavelength division multiplexing (WDM) optical link.
by: Mrs. Aboli N. Moharil Assistant Professor, EXTC dept.
Integrated Semiconductor Modelocked Lasers
Modelling & Simulation of Semiconductor Devices
The Laplace Transform Prof. Brian L. Evans
EE Audio Signals and Systems
Description and Analysis of Systems
Discussion today Over the next two class periods we will be designing a ring resonator based 2-channel wavelength division multiplexing (WDM) optical link.
Subject Name: Optical Fiber Communication Subject Code: 10EC72
Chapter4 Bandpass Signalling Bandpass Filtering and Linear Distortion
High Power, Uncooled InGaAs Photodiodes with High Quantum Efficiency for 1.2 to 2.2 Micron Wavelength Coherent Lidars Shubhashish Datta and Abhay Joshi.
Sinusoidal response of circuits
Modeling in the Time Domain
EE-314 Signals and Linear Systems
State Space Method.
SuperKEKb X-Ray Monitor
Equalizing Average Source Power with Pattern Swapping
LECTURE 20: FOURIER ANALYSIS OF DT SYSTEMS
Digital Modulation Basics
Pump and probe technique
Dynamical Operation, Vector Control, DTC and Encoder-less Operation
Sinusoidal response of circuits
Presentation transcript:

Simulation and Analysis of Single Mode Semiconductor Laser Course Project for EE8114 Electrical Engineering Dept. Ryerson University Grace FENG

Outline of My Work Background Research on Fiber over Radio Close Study on the Simulink Based Semiconductor Laser Diode Model Repeat the Simulation Results from the Previous Work Build Simulation Functions to Analyze the Optical Response of the Laser Diode

Large-Signal Simulink Model Rate Equation for Carrier Density and Photon Density S.A. Javro & S.M. Kang “Transforming Tucker’s Linearized Laser Rate Equations to a Form that has a Single Solution Regime” Journal of Lightwave Technology, 1995

Large-Signal Simulink Model, Cont. Toby Schaer, Robert Rusnov, Stephen Eagle, Jay Jastrebski, Steven Albanese and Xavier Fernando “A Dynamic Simulation Model for Semiconductor Laser Diodes” CCECE 2003 – CCGEI 2003, Montreal, May/mai 2003

Operating Point Pumping Current (mA) Electron Density (m-3) Photon Density (m-3) 10mA 1.9531 * 1018 1.9221 * 1013 15mA 1.9571* 1018 1.7141 * 1014 STATE SPACE MODEL Using the operating point values to complete State Space Model, so that to enable simulation around operating point.

Small-Signal Simulink Model Current Input Rectanglur Pulse Amplitude = 1mA Photon Output State Space Model Implemented in Matlab Pumping Current (10mA, 15mA) Pulse Response when bias point of I = 10mA Pulse Response when bias point of I = 15mA

Sinusoidal Signal Response

Sinusoidal Signal Response, Cont. Amplitude of Input Signal Increased from 0.001mA to 1mA Stepped by 0.001mA Simulating System Response 100 Times Sampling the Input Amplitude each Time Sampling the Output Amplitude each Time Plot the Relationship between Input and Output Amplitude Analyze the Result

Sinusoidal Signal Response, Cont. Sample Phase Shift during Each Simulation Plot the Relationship between Input Amplitude with Output Phase Shift

Conclusion Small Input Eletronic Signal around Operating Point of a Laser Diode could Lead to Linear Optical Response in Terms of Amplitude Phase Shift in Optical Response around Operating Point Does Not Respond to Any Changes in Input Electronic Signal