UMBC New Approaches to Modeling Optical Fiber Transmission Systems Presented by C. R. Menyuk With R.  M. Mu, D. Wang, T. Yu, and V. S. Grigoryan University.

Slides:



Advertisements
Similar presentations
EE 230: Optical Fiber Communication Lecture 17
Advertisements

Outline H History of lightwave undersea cable systems H Optical amplifier technologies H Examples of lightwave undersea cable networks – TPC-5CN – APCN.
Simultaneously Stokes and anti-Stokes Raman amplification in silica fiber Victor G. Bespalov Russian Research Center "S. I. Vavilov State Optical Institute"
Winter et al.: XPolM in PolDM Systems, Th.10.E.3, ECOC MMX olarization-Multiplexed System Outage due to Nonlinearity- Induced Depolarization Marcus Winter,
Marcus Winter: XPolM in Polarization-Multiplex Transmission Systems Cross-Polarization Modulation in Polarization-Multiplexed Systems M. Winter, D. Kroushkov,
Fiber Systems Dense Wavelength Division Multiplexing (DWDM) Alpina Kulkarni Optical Communications (EE566) Dr. Paolo Liu Electrical UB.
Razali Ngah and Z Ghassemlooy Optical Communications Research Group
Shedding and Interaction of solitons in imperfect medium Misha Chertkov (Theoretical Division, LANL) LANL, 02/05/03 ``Statistical Physics of Fiber Optics.
Optical Burst Switching (OBS): Issues in the Physical Layer University of Southern California Los Angeles, CA A. E. Willner.
Simulation of a Passively Modelocked All-Fiber Laser with Nonlinear Optical Loop Mirror Joseph Shoer ‘06 Strait Lab.
Modulation formats for digital fiber transmission
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.
11/7/2000EE228A Lecture1 Problem We need more bandwidth –Data traffic doubles every 4 (up to 12) months –More users connect to the Internet … –And stay.
Fiber-Optic Communications
EE 230: Optical Fiber Communication Lecture 14 From the movie Warriors of the Net Optical Time Division Multiplexing.
Lecture 8 Optical Fiber Amplifier – noise and BER Last lecture Introduction to Fiber Optical Amplifier – types and applications Erbium-doped fiber.
Soliton Research at the Lightwave Communication Systems Laboratory
Lecture 9 Optical Fiber Amplifier – PDL, Transient, Cross-talk Last Lecture Amplifier Noise OSNR and BER System Applications.
Fiber-Optic Communications
Optical Network Link Budgets EE 548 Spring Reference Model.
Lightwave Communications Systems Research at the University of Kansas.
System Performance Stephen Schultz Fiber Optics Fall 2005.
Optical Amplifiers An Important Element of WDM Systems Xavier Fernando ADROIT Group Ryerson University.
Chapter Twenty-Five: Optical Communication Systems.
EVLA Fiber Selection Critical Design Review December 5, 2001.
Vadim Winebrand Faculty of Exact Sciences School of Physics and Astronomy Tel-Aviv University Research was performed under a supervision of Prof. Mark.
Introduction to Optical Communication Dr. Manoj Kumar Professor & Head, Dept. of Electronics & Comm. Engg.
Poznan Supercomputing and Networking Center
Optical Fiber Basics-Part 2
Light Wave Systems Dr Manoj Kumar Professor & Head Department of ECE DAVIET,Jalandhar.
Test Plan for PMD Testing of a WDM Receiver Henry Yaffe, Principal January 2004.
Analysis of Phase Noise in a fiber-optic link
1 Chapter 5 Transmission System Engineering Design the physical layer Allocate power margin for each impairment Make trade-off.
SJD/TAB1 EVLA Fiber Selection Critical Design Review December 5, 2001.
Dense Wavelength Division Multiplexing (DWDM) Technology
Physical Impairments in Optical Systems and Networks (FIBER NON-LINEARITIES) Prof. Manoj Kumar Dept. of Electronics and Communication Engineering DAVIET.
1 PHYSICAL IMPAIRMENTS Maruthy Mentireddi Raghu Kalyan Anna.
Intermode Dispersion (MMF)
Chapter 4: Optical fibers and their parameters Graphic representation of three different types of how the refractive index change in the core of an optical.
1 Razali Ngah, and Zabih Ghassemlooy Optical Communication Research Group School of Engineering & Technology Northumbria University, United Kingdom http:
Chapter 10 Optical Communication Systems
Open-source NSE Codes Applied to 40 Gbit/s Soliton Lines KAZUHIRO SHIMOURA Kansai Electric Power Co., Japan ECOC2001 ( Oct. 4, 2001 RAI Congress Centre,
Receiver design for Modal Multiplexing in Multimode Fiber Communication Systems Alan Pak Tao Lau Stanford University Supervisor: Dr. Lei Xu, Dr. Ting Wang.
Investigations on PMD-induced penalties in 40 Gbps optical transmission link Irfan Ullah Department of Information and Communication Engineering Myongji.
Statistical physics approach to evaluation of outage probability in optical communications Misha Chertkov (Theoretical Division, LANL) In collaboration.
Lecture Note on Optical Components. Optical Couplers Combines & splits signals Light couples from one waveguide to a closely placed waveguide because.
Pulse confinement in optical fibers with random dispersion Misha Chertkov (LANL) Ildar Gabitov (LANL) Jamey Moser (Brown U.)
Optical telecommunication networks.  Introduction  Multiplexing  Optical Multiplexing  Components of Optical Mux  Application  Advantages  Shortcomings/Future.
The University of Kansas / ITTC Lightwave System Modeling at the Lightwave Communication Systems Laboratory Information and Telecommunications Technology.
Ahmed Musa, John Medrano, Virgillio Gonzalez, Cecil Thomas University of Texas at El Paso Circuit Establishment in a Hybrid Optical-CDMA and WDM All- Optical.
Pulse confinement in optical fibers with random dispersion Misha Chertkov (LANL) Ildar Gabitov (LANL) Jamey Moser (Brown U.)
Nonlinear Optics Lab. Hanyang Univ. Chapter 6. Processes Resulting from the Intensity-Dependent Refractive Index - Optical phase conjugation - Self-focusing.
An integrated survey in Optical Networks: Concepts, Components and Problems Delivered by Erna Sri Sugesti, Ir., MSc. 1 May 2013 Ali Norouzi †, A.Halim.
Design of Lightwave Communication Systems and Networks
Parametric Solitons in isotropic media D. A. Georgieva, L. M. Kovachev Fifth Conference AMITaNS June , 2013, Albena, Bulgaria.
Photonic Components Rob Johnson Standards Engineering Manager 10th July 2002 Rob Johnson Standards Engineering Manager 10th July 2002.
Phase velocity. Phase and group velocity Group velocity.
Date of download: 6/25/2016 Copyright © 2016 SPIE. All rights reserved. The variation of BER when the relative phase and delay between channels are randomly.
Sistemas de Comunicación Óptica
distributed versus discrete amplification
Optical Amplifier.
Prof. Manoj Kumar Dept. of Electronics and Communication Engineering
Design and Simulation of Photonic Devices and Circuits
Sandis Spolitis, Inna Kurbatska, Vjaceslavs Bobrovs
DWDM and Internets’ Bandwidth Future
Making Networks Light March 29, 2018 Charleston, South Carolina.
The University of Adelaide, School of Computer Science
Back End & LO PDR April 2002 FIBRE-OPTIC LINKS -An Introduction Ralph Spencer Jodrell Bank Observatory University of Manchester UK --The use of.
D. Dahan, A. Bilenca, R. Alizon and G. Eisenstein
Presentation transcript:

UMBC New Approaches to Modeling Optical Fiber Transmission Systems Presented by C. R. Menyuk With R.  M. Mu, D. Wang, T. Yu, and V. S. Grigoryan University of Maryland Baltimore County Computer Science and Electrical Engineering Department Baltimore, MD 21250

UMBC New Approaches to Modeling Optical Fiber Transmission Systems Presented by V. S. Grigoryan With R.  M. Mu, D. Wang, T. Yu, and C. R. Menyuk University of Maryland Baltimore County Computer Science and Electrical Engineering Department Baltimore, MD 21250

UMBC Professors Gary Garter Curtis Menyuk Associates Vladimir Grigoryan Edem Ibragimov Pranay Sinha Students Ronald Holzlöhner Ivan Lima, Jr. Ruomei Mu Yu Sun Ding Wang Tao Yu Current research group

UMBC A Decade Ago System with Electronic Repeaters 500 Mb/s looked achievable; 100 Mb/s was achieved Only attenuation mattered in fibers – fibers were a transparent pipe Repeaters had limited bandwidth (WDM and upgrading impossible) – Cost and complexity rose dramatically with data rate – spacings of 20 km were required RRR 20 km

UMBC Today System with Erbium-doped amplifiers 1 Tbit/s looks achievable; 200 Gbits/s achieved Wavelength division multiplexing (WDM) is possible and becoming widely used (200 Gb/s = 80 channels  2.5 Gb/s) Fiber dispersion, nonlinearity, and polarization effects all accumulate! Fiber impairments set the limits on what is achievable – nonlinearity is strong and hard to model properly. 50 km or more

UMBC What formats should be used? Non-return to zero (NRZ) (close to zero dispersion) Solitons (anomalous dispersion) vs

UMBC Approaches are converging! Solitons and NRZ resemble each other – solitons dispersion-managed solitons – NRZ phase- and amplitude-modulated pulses

UMBC What formats should be used? Time-division multiplexed (TDM) I t channels Wavelength-division multiplexed (WDM) channels I

UMBC Fiber impairments Chromatic Dispersion Polarization Effects Nonlinearity ASE noise Four Horsemen of the Apocalypse Albrecht Dürer Four Horsemen of Optical Fiber Transmission

UMBC Modeling approaches ¶ Multiple scale length methods — for establishing equations · Split-step modeling — often too slow (especially with WDM) ¸ Reduced methods — dealing with many channels, long-term effects, networks

UMBC Modeling approaches ¶ Monte Carlo — often too slow · Ito’s method — often does not work ¸ Linearization Randomly varying effects

UMBC Multiple Scale Lengths methods Light wavelength 1  m 10  m 100  m 1 mm 10 mm 100 mm 1 m 100 m 10 m 1 km 100 km 10 km 1 Mm 10 Mm 100 Mm Core diameter Pulse durations Polarization beat length Attenuation length Nonlinear length Fiber correlation length Dispersion length FLAG trans-Atlantic Manakov-PMD approximation Slowly varying envelope approximation Maxwell’s equations land link Optical systems have a wide spread in length scales! Scale lengths in fiber transmission

UMBC Coupled Nonlinear Schrödinger Equation Maxwell’s Equations Coupled Nonlinear Schrödinger Equation Manakov-PMD Equation Averaging over the Poincaré sphere Using the slowly varying envelope approximation

UMBC Linearization approach Monte Carlo: Linearization (with small noise): signalnoisecomplicated mix signalnoiseGaussian statistics (nonlinear) (linear)

UMBC Comparison of theory & experiment Timing jitter (ps) Distance (km) experiment Monte Carlo simulation our approach

UMBC Average Power Approximation With N channels, scaling reduces from N 2 to better than N! Useful for point-to-point systems (Yu, Reimer, and Menyuk; Wang and Menyuk) Critical for network simulations (Bellcore: R. Wagner, I. Roudas, & colleagues)  target channel complete channel averaged channel

UMBC With polarization Stokes vector distance (km) simulation theory Evolution of the Stokes vector – – – S 1 S 3 S 2 (a) S 1 S 3 S 2 (b) S 1 S 3 S 2 (c) realistic dispersionlarge dispersion

UMBC Reduced Polarization Model ¶ PDL effects calculated — one year ago · Verification of model effectiveness with chromatic dispersion and nonlinearity — now ¸ Inclusion of PMD, PDL, and PDG — in one year

UMBC Experimental Applications D L Normal Anomalous Average 1.2 nm Filter AO Switch 60/40 Coupler Input To Receiver PC EDFA Normal Anomalous Dispersion-managed soliton experiments

UMBC Theory and experiment Dynamic Evolution in One Round Trip Amplitude Margin experimental theoretical experimental theoretical

UMBC Normal dispersion solitons: A B  D=110  D=100  D=90  D=80  D=70  D=60 Pulse energy Average dispersion — Solitons exist in the normal dispersion regime — These solutions are stable Intensity 0 Time – At point B: Distance

UMBC World record experiment 20 Gbit/s: BER 20 Mm 20 Gbit/s input 10 Gbit/s Demux output (20 Mm) experimental theoretical 1 Bit 0 Bit

UMBC Conclusions ¶Optical fiber transmission systems are rapidly changing · Good modeling has become critical ¸ Enormous strides have been made