Characterization of fiber amplifiers Lecture-5. EDFA architecture Figure: EDFA architecture Characterization of DFA.

Slides:



Advertisements
Similar presentations
High power (130 mW) 40 GHz 1.55 μm mode-locked DBR lasers with integrated optical amplifiers J. Akbar, L. Hou, M. Haji,, M. J. Strain, P. Stolarz, J. H.
Advertisements

EE 230: Optical Fiber Communication Lecture 17
Simultaneously Stokes and anti-Stokes Raman amplification in silica fiber Victor G. Bespalov Russian Research Center "S. I. Vavilov State Optical Institute"
Low Noise Amplifier (LNA) Presented By Mohammad Jameel NDG on FSMFPGA Based System Design1.
Presentation Overview
Waveguides Part 2 Rectangular Waveguides Dielectric Waveguide
S Digital Communication Systems Fiber-optic Communications - Supplementary.
Combined Stokes-anti-Stokes Raman amplification in fiber Victor G. Bespalov All Russian Research Center "S. I. Vavilov State Optical Institute" Nikolai.
Building a Continuous Wave Erbium Doped Fiber Laser and Amplifier Ben Baker Kristen Norton.
May Chuck DiMarzio, Northeastern University ECE-1466 Modern Optics Course Notes Part 9 Prof. Charles A. DiMarzio Northeastern University.
CHAPTER 6 OPTICAL AMPLIFIERS
Optical Fibre Communication Systems
Lecture: 10 New Trends in Optical Networks
Bulk Scintillator Light Yield  We have prepared samples of bulk scintillator in order to study optimization for the MICE Fiber Tracker  pT(1.25%) + 3HF(.1-1%)
Matt Ruby & Colin Diehl High Power Double-Clad Fiber Laser.
P449. p450 Figure 15-1 p451 Figure 15-2 p453 Figure 15-2a p453.
EE 230: Optical Fiber Communication Lecture 7 From the movie Warriors of the Net Optical Amplifiers-the Basics.
1 Optical Fibre Amplifiers. 2 Introduction to Optical Amplifiers Raman Fibre Amplifier Brillouin Fibre Amplifier Doped Fibre Amplifier.
EE 230: Optical Fiber Communication Lecture 17 From the movie Warriors of the Net System Considerations.
Lecture 8 Optical Fiber Amplifier – noise and BER Last lecture Introduction to Fiber Optical Amplifier – types and applications Erbium-doped fiber.
EE 230: Optical Fiber Communication From the movie Warriors of the Net Lecture 8 Fiber Amplifiers.
Ch 6: Optical Sources Variety of sources Variety of sources LS considerations: LS considerations: Wavelength Wavelength  Output power Output power Modulation.
May be regarded as a form of electromagnetic radiation, consisting of interdependent, mutually perpendicular transverse oscillations of an electric and.
Lecture 9 Optical Fiber Amplifier – PDL, Transient, Cross-talk Last Lecture Amplifier Noise OSNR and BER System Applications.
1 Lecture 7b DWDM 1. Introduction 2. Principles of Wavelength Division Multiplexing 3. WDM System Components 4. Wavelength-Independent Coupler 5. Construction.
Introduction to Space Systems and Spacecraft Design Space Systems Design Communications - Decibel Ref: SMAD Sections – 13 Communications Architecture.
E D F A Seminar By: Geno G James EE-566 Optical Communication.
STUDY OF AMPLIFICATION ON ERBIUM DOPED FIBER AMPLIFIER Lita Rahmasari, Assoc. Prof. Dr. Yusof Munajat, Prof. Dr. Rosly Abdul Rahman Optoelectronics Laboratory,
System Performance Stephen Schultz Fiber Optics Fall 2005.
Optical Amplifiers An Important Element of WDM Systems Xavier Fernando ADROIT Group Ryerson University.
Vincent Auroux 1,2, Arnaud Fernandez 1, Olivier Llopis 1, Pierre-Henri Merrer 2, Alexandre Vouzellaud 2 1 CNRS, LAAS, Univ. de Toulouse, France 2 OSAT,
Protection notice / Copyright notice Bidirectional EDFA for future XL-PONs M. Rasztovits-Wiech / Siemens, 25. September 2006 Copyright © Siemens AG 2006.
Introduction to Fibre Optic Communication Mid Sweden University.
EPH 7112 LECTURE 2: CHARACTERISTICS AND TYPES OF RESEARCH
1 Numerical and Analytical models for various effects in models for various effects inEDFAs Inna Nusinsky-Shmuilov Supervisor:Prof. Amos Hardy TEL AVIV.
SJD/TAB1 EVLA Fiber Selection Critical Design Review December 5, 2001.
1 PHYSICAL IMPAIRMENTS Maruthy Mentireddi Raghu Kalyan Anna.
A Complete Course in Power Point Second Edition Version
CHAPTER 6 OPTICAL AMPLIFIERS
PREAMBLE OF OPTICAL NETWORKS. INDEX PREAMBLE STRUCTUREPREAMBLE STRUCTURE HOLLISTIC FIX HOLLISTIC FIX KEY CONCEPT KEY CONCEPT KEY RESEARCH AREA KEY RESEARCH.
Question 1 Find the following using dB and dBm transformations: a) Power in dB for 22 W b) Power in dBm for 4.8 W c) Power in W for 25 dB.
A NEW METHOD TO STABILIZE HIGH FREQUENCY HIGH GAIN CMOS LNA RF Communications Systems-on-chip Primavera 2007 Pierpaolo Passarelli.
CHAPTER 6 OPTICAL AMPLIFIERS. The Need of Optical Amplification Erbium-Doped Fiber Amplifiers (EDFAs) – application in long haul. Today’s amplifier of.
Power Considerations in Optical Transmission Systems in Presence of Nonlinear Phase Noise Alan Pak Tao Lau Department of Electrical Engineering, Stanford.
Comparison of Three Dispersions Normal Anomalous.
Optical Amplifiers By: Ryan Galloway.
Fig. 11-1: Applications of optical amplifiers. Fig. 11-2: Generic optical amplifier.
FIBER OPTIC TRANSMISSION
Optical sources Types of optical sources
Erbium Doped Fiber Amplifiers Erbium Doped Fiber Amplifiers are considered the most important invention of the 1990’s in the telecommunication industry.
Multicore EDFA for DWDM Transmission in Full C-band Yukihiro. etc. 张浩
Subject Name: Optical Fiber Communication Subject Code: 10EC72
Absorption Small-Signal Loss Coefficient. Absorption Light might either be attenuated or amplified as it propagates through the medium. What determines.
© 2005, it - instituto de telecomunicações. Todos os direitos reservados. This tutorial is licensed under the Creative Commons
Date of download: 9/19/2016 Copyright © 2016 SPIE. All rights reserved. Higher-order Raman gain generation with pump power of 0.9 W (——), 2 W (....) and.
Four wave mixing in submicron waveguides
Optical Sources.
Presentation Overview
by: Mrs. Aboli N. Moharil Assistant Professor, EXTC dept.
distributed versus discrete amplification
Optical Amplifier.
CHAPTER 7 Optical Amplifier.
1. For a resonant cavity shown below, the transmission matrix can be written as below Z=0 Z=L Prove that the E field is continuous at the interfaces, z=0.
Problem We need more bandwidth
COMMUNICATION ENG. PROF. A.M.ALLAM
Optical communications
Fiber Optic Communication Lec 11 By
Fiber Laser Part 1.
Slab waveguide solution
D. Dahan, A. Bilenca, R. Alizon and G. Eisenstein
Presentation transcript:

Characterization of fiber amplifiers Lecture-5

EDFA architecture Figure: EDFA architecture Characterization of DFA

Three level Energy System Figure: Three level energy system Characterization of DFA

Rate Equations for three level Energy System. Characterization of DFA

Modeling of EDFA…………. Characterization of DFA

Modeling of EDFA Characterization of DFA

Noise figure of EDFA Characterization of DFA

Figure: Gain and NF in dB as a function of pump power in mW using a 10 m long EDF at 1550 nm signal wavelength and injected signal power of -35 dBm. From the numerical simulation. Characterization of DFA

Figure: Population in the upper state (N2) and ground state (N1) as a function of position along a 21 m long EDF at 1550 nm using 14 mW of pump power and injected signal power of -35 dBm. From the numerical simulation. Characterization of DFA

Figure: Gain as a function of EDF length at 1550 nm signal wavelength using 14 mW of pump power and injected signal power of -35 dBm. Characterization of DFA

Figure: Gain and NF in dB as a function of pump power in mW using a 10 m (non- optimized) and 21 m (optimized) long EDF at 1550 nm signal wavelength and injected signal power of -35 dBm. Characterization of DFA

Figure: Gain and NF in dB as a function of signal power in dBm using a 21 m long EDF at 1550 nm signal wavelength and injected pump power of 14 mW. Characterization of DFA

Figure: Absorption and emission cross sections of Erbium near 1500 nm for the fiber mentioned in table -1. Characterization of DFA

Figure: Gain in dB as a function of signal wavelength for various pump powers and injected signal power of -35 dBm using a 21 m long EDF Characterization of DFA

Figure: Gain in dB as a function of pump power in mW and signal power in dBm using a 21 m long EDF at 1550 nm signal wavelength. Characterization of DFA

Figure: NF in dB as a function of pump power in mW and signal power in dBm using a 21 m long EDF at 1550 nm signal wavelength. Characterization of DFA