40-Gb/s Optical Buffer Design and Simulation

Size: px
Start display at page:

Download "40-Gb/s Optical Buffer Design and Simulation"

Transcription

1 40-Gb/s Optical Buffer Design and Simulation Hyundai Park, Emily F. Burmeister, Staffan Björlin, and John E. Bowers Electrical and Computer Engineering Department University of California at Santa Barbara This work supported by DARPA through the LASOR program 1

2 Outline Introduction - Motivation and Device Structure Simulation Model and Method - Flow Chart - Model Description Results: Performance Dependence on - - Waveguide - Bandpass Filter - Optical Input Power Conclusions

3 Motivation Goal: To investigate 100 Tbit/s transparent optical packet switched networks Problem: Provide a means to store optical packets to reduce contention and packet loss Input Buffering ing& ing Output 3

4 Motivation Goal: To investigate 100 Tbit/s transparent optical packet switched networks Problem: Provide a means to store optical packets to reduce contention and packet loss. Solution: OPTICAL BUFFER should be realized with.. -Low signal degradation during storage -Fast switching time Requirements: -Buffering time increment; 10 ns corresponding to 40 bytes with guard signals (40 Gb/s) -Hold a packet up to 100 ns 4 -ing time less than 1ns

5 Proposed Device Silica Waveguide IN OUT InP Si Recirculating loop with spiral silica waveguide Length of 10 cm with 0.05 db/cm propagation loss InP and MZI based optical switch Provide gain and fast switching time 5 1 cm with 5 db/cm propagation loss

6 Flowchart Signal Input Initial Loss Silica Waveguide BER estimation 40 Gb/s, RZ Gaussian Pulse shape TE Polarization Input Field S in (t) 6

7 Flowchart Signal Input SiO Waveguide Initial Loss Silica Waveguide IN OUT BER estimation Initial Loss at the Input S sw (t) = S in (t) L 0 (L 0 = L C +L INP ) 7

8 Flowchart Signal Input SiO Waveguide Initial Loss Silica Waveguide IN OUT BER estimation Noise Filtering in Band Pass Filter S (t) = IFT(S sw (f) T (f)) 8

9 Model - & x InP MZI based Optical - Propagation Loss: 5 db per roundtrip - Assumptions: No crosstalk Ideal switching characteristics (Step function response) Band Pass Filter - Super Gaussian Shape Transfer Function T (ω) = exp f f f 0 m 9

10 Flowchart Signal Input SiO Waveguide Initial Loss Silica Waveguide IN OUT BER estimation Propagation in Waveguide S W (t) = IFT(S (f) D(f)) N(t) 10

11 Model - Silica Waveguide - Signal propagation Standard Fourier Domain Split-Step (FDSS) Method 1, - Assumption: Polarization is maintained in the waveguide. A( z + z, t) = IFT( A( z, ω)exp( Dˆ ( ω) z)) exp( Nˆ ( t) z) ˆ i D( ω) = α SiO + βω + Nˆ ( t) = iγ A( z, t) i 6 3 β ω 3 3 λ λ β = D β 3 = ( D + λs) πc (πc) γ = n ω 0 ca eff 1 R. H. Hardin and F. D. Tappert, SIAM Rev. Chronicle 15, 43 (1973) R. A. Fisher and W. K. Bischel, Appl. Phys. Lett. 3, 661 (1973); J. Appl. Phys. 46, 491 (1975) 11

12 Flowchart Signal Input SiO Waveguide Initial Loss Silica Waveguide IN OUT BER estimation Amplification in S (t)= IFT(FT(S W (t) G(t)) T G (f))+s ASE (t) 1

13 Gain Characteristics Model MQW - Rate Equation in Multiple Quantum Well s - Confinement factor (Γ): Length from 500 μm to mm τd τn τe dn dt dn dt B W dp dz I N B N Γ B qn 0 w = + evsch τ n τ d τ e N B Nw N w N = vga ln Γqτ d τ n τ e N w tr N N w vg hνv p = Γa ln P N, P = N P tr L P 13

14 Noise - Assumption: white Gaussian noise σ = f ) f N ASE N ASE ( 0 0 ) = ( G 1) nsphf0 ( G 1) Model MQW ( f NF hf Gain Ripple due to Reflection between facets 0 R) T G = iωnl / c 1 (1 G R e G 14

15 Flowchart Coupling Loss, Propagation loss Signal Input SiO Waveguide Initial Loss Silica Waveguide IN OUT BER estimation Optical S out (t)=s (t) L SW (L SW = L C + L INP ) 15

16 Gain Regulation G 0 G Final Roundtrip Loss P 1st P nd P 3rd P 4th P 5th P in - Amplifier gain is saturated to roundtrip loss typically within10 circulations. - Gain saturation occurs due to gain regulation behavior. 16

17 17 Maximum Delay (µs) Dependence on Dispersion 10 9 L round = 1.5 db 8 Delay per roundtrip = 10ns 7 D=5 ps/km-nm P in =13 dbm D=15 ps/km-nm P in =7 dbm Gain (db) - Without gain dynamics of the, the performance is limited by ASE noise accumulation at low gain Dispersion at high gain - Dispersion of 5 ps/km-nm is expected in the silica waveguide. 5 μsec delay with moderate input power and gain Maximum Number of Roundtrips

18 Dependence on Gain Dynamics Maximum Delay (ns) P in = 7 dbm Delay per roundtrip = 10 ns P 3dB = 0dBm P 3dB = 17dBm P 3dB = 14dBm Roundtrip Loss = 1.5 db Maximum Number of Roundtrips Gain (db) - Typical carrier life time in the ; ~50ps ns maximum delay with P sat = 17 dbm - Pattern effect dominates the overall performance. 18

19 Dependence on Facet Reflectivity Maximum Delay (ns) R= Gain (db) W avelength (nm) P in = 10 dbm Roundtrip Loss = 1.5dB Delay per roundtrip = 10 ns Gain (db) db Gain G 0 =db and R= db accumulated distortion at 10 circulations R=0 - Reflectivity should be kept less than 10-5 to achieve large delay Maximum Number of Roundtrips 19

20 Dependence on Bandwidth Maximum Delay (ns) m = 3 10 m = m = Filter Bandwidth (nm) Maximum Number of Roundtrips - Filter Bandwidth < nm; limited by passband flatness - Filter Bandwidth > nm; limited by ASE noise accumulation 0 - Optimum bandwidth is a compromise between distortion and noise.

21 Dependence on Input power Maximum Delay (ns) P 3dB = 0dBm Delay per roundtrip = 10 ns L C = 1dB G 0 = 18dB L C = 3dB L C = 5dB G 0 = db G 0 = 6dB Average Input Power (dbm) Maximum Number of Roundtrips Maximum Pin = 10 dbm 160 L round = 17.5 db 110 L round = 1.5 db 60 L round = 5.5 db -Maximum delay tends to be saturated at high input power. -It can be attributed to fast gain saturation. 1

22 Overall Device Performance P db = 13dBm 17dBm Carrier Life Time = ps

23 Conclusions Performance of optical buffer was predicted using FDSS and a rate equation model. The maximum delay is limited to 100 ns in 40Gb/s system by the pattern effect due to gain dynamics. Nonzero reflectivity of the and non-ideal transfer function of the can degrade the performance due to accumulated distortion. 3

An integrated recirculating optical buffer

An integrated recirculating optical buffer An integrated recirculating optical buffer Hyundai Park, John P. Mack, Daniel J. Blumenthal, and John E. Bowers* University of California, Santa Barbara, Department of Electrical and Computer Engineering,

More information

Notes on Optical Amplifiers

Notes on Optical Amplifiers Notes on Optical Amplifiers Optical amplifiers typically use energy transitions such as those in atomic media or electron/hole recombination in semiconductors. In optical amplifiers that use semiconductor

More information

All-Optical Signal Processing and Optical Regeneration

All-Optical Signal Processing and Optical Regeneration 1/36 All-Optical Signal Processing and Optical Regeneration Govind P. Agrawal Institute of Optics University of Rochester Rochester, NY 14627 c 2007 G. P. Agrawal Outline Introduction Major Nonlinear Effects

More information

DESIGN TEMPLATE ISSUES ANALYSIS FOR ROBUST DESIGN OUTPUT. performance, yield, reliability

DESIGN TEMPLATE ISSUES ANALYSIS FOR ROBUST DESIGN OUTPUT. performance, yield, reliability DESIGN TEMPLATE ISSUES performance, yield, reliability ANALYSIS FOR ROBUST DESIGN properties, figure-of-merit thermodynamics, kinetics, process margins process control OUTPUT models, options Optical Amplification

More information

Self-phase-modulation induced spectral broadening in silicon waveguides

Self-phase-modulation induced spectral broadening in silicon waveguides Self-phase-modulation induced spectral broadening in silicon waveguides Ozdal Boyraz, Tejaswi Indukuri, and Bahram Jalali University of California, Los Angeles Department of Electrical Engineering, Los

More information

Simulation of semiconductor modelocked ring lasers with monolithically integrated pulse shaping elements

Simulation of semiconductor modelocked ring lasers with monolithically integrated pulse shaping elements Simulation of semiconductor modelocked ring lasers with monolithically integrated pulse shaping elements Martijn Heck, Yohan Barbarin, Erwin Bente Daan Lenstra Meint Smit Richard Nötzel, Xaveer Leijtens,

More information

In Search of the Elusive All-Optical Packet Buffer

In Search of the Elusive All-Optical Packet Buffer In Search of the Elusive All-Optical Packet Buffer Rod Tucker Centre for Ultra-Broadband Information Networks (CUBIN) Department for Electrical and Electronic Engineering University of Melbourne, Australia

More information

Lecture 3 Fiber Optical Communication Lecture 3, Slide 1

Lecture 3 Fiber Optical Communication Lecture 3, Slide 1 Lecture 3 Dispersion in single-mode fibers Material dispersion Waveguide dispersion Limitations from dispersion Propagation equations Gaussian pulse broadening Bit-rate limitations Fiber losses Fiber Optical

More information

Timing Jitter In Long-haul WDM Return-To-Zero Systems

Timing Jitter In Long-haul WDM Return-To-Zero Systems Timing Jitter In Long-haul WDM Return-To-Zero Systems vorgelegt von Diplom-Ingenieur André Richter aus Berlin von der Fakultät IV Elektrotechnik und Informatik der Technischen Universität Berlin zur Erlangung

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

Chapter 3 Signal Degradation in Optical Fibers

Chapter 3 Signal Degradation in Optical Fibers What about the loss in optical fiber? Why and to what degree do optical signals gets distorted as they propagate along a fiber? Fiber links are limited by in path length by attenuation and pulse distortion.

More information

ELSEVIER FIRST PROOFS

ELSEVIER FIRST PROOFS OPTICAL AMPLIFIERS / Semiconductor Optical Amplifiers 1 OPTICAL AMPLIFIERS A5 S5 P5 P1 Semiconductor Optical Amplifiers M J Connelly, University of Limerick, Limerick, Ireland q 24, Elsevier Ltd. All Rights

More information

Semiconductor Optical Amplifiers with Low Noise Figure

Semiconductor Optical Amplifiers with Low Noise Figure Hideaki Hasegawa *, Masaki Funabashi *, Kazuomi Maruyama *, Kazuaki Kiyota *, and Noriyuki Yokouchi * In the multilevel phase modulation which is expected to provide the nextgeneration modulation format

More information

Chapter 8. Digital Links

Chapter 8. Digital Links Chapter 8 Digital Links Point-to-point Links Link Power Budget Rise-time Budget Power Penalties Dispersions Noise Content Photonic Digital Link Analysis & Design Point-to-Point Link Requirement: - Data

More information

Lecture 8 Fiber Optical Communication Lecture 8, Slide 1

Lecture 8 Fiber Optical Communication Lecture 8, Slide 1 Lecture 8 Bit error rate The Q value Receiver sensitivity Sensitivity degradation Extinction ratio RIN Timing jitter Chirp Forward error correction Fiber Optical Communication Lecture 8, Slide Bit error

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

Application Instruction 001. The Enhanced Functionalities of Semiconductor Optical Amplifiers and their Role in Advanced Optical Networking

Application Instruction 001. The Enhanced Functionalities of Semiconductor Optical Amplifiers and their Role in Advanced Optical Networking The Enhanced Functionalities of Semiconductor Optical Amplifiers and their Role in Advanced Optical Networking I. Introduction II. III. IV. SOA Fundamentals Wavelength Conversion based on SOAs The Role

More information

SIMULATION OF FIBER LOOP BUFFER MEMORY OF ALL-OPTICAL PACKET SWITCH. Mandar Naik, Yatindra Nath Singh

SIMULATION OF FIBER LOOP BUFFER MEMORY OF ALL-OPTICAL PACKET SWITCH. Mandar Naik, Yatindra Nath Singh SIMULATION OF FIBER LOOP BUFFER MEMORY ABSTRACT OF ALL-OPTICAL PACKET SWITCH Mandar Naik, Yatindra Nath Singh Center for Laser Technology Indian Institute of Technology Kanpur - 28 16 India {mandy,ynsingh}@iitk.ac.in

More information

Chapter 12: Optical Amplifiers: Erbium Doped Fiber Amplifiers (EDFAs)

Chapter 12: Optical Amplifiers: Erbium Doped Fiber Amplifiers (EDFAs) Chapter 12: Optical Amplifiers: Erbium Doped Fiber Amplifiers (EDFAs) Prof. Dr. Yaocheng SHI ( 时尧成 ) yaocheng@zju.edu.cn http://mypage.zju.edu.cn/yaocheng 1 Traditional Optical Communication System Loss

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

Broadcast and distribution networks

Broadcast and distribution networks 4/7/06 SYSTEM ARCHITECTURES Point-to-point links Point-to-point links constitute the simplest kind of lightwave systems The link length can vary from less than a kilometer (short haul) to thousands of

More information

Study of All-Optical Wavelength Conversion and Regeneration Subsystems for use in Wavelength Division Multiplexing (WDM) Telecommunication Networks.

Study of All-Optical Wavelength Conversion and Regeneration Subsystems for use in Wavelength Division Multiplexing (WDM) Telecommunication Networks. Study of All-Optical Wavelength Conversion and Regeneration Subsystems for use in Wavelength Division Multiplexing (WDM) Telecommunication Networks. Hercules Simos * National and Kapodistrian University

More information

τ mod = T modal = longest ray path shortest ray path n 1 L 1 = L n 2 1

τ mod = T modal = longest ray path shortest ray path n 1 L 1 = L n 2 1 S. Blair February 15, 2012 23 2.2. Pulse dispersion Pulse dispersion is the spreading of a pulse as it propagates down an optical fiber. Pulse spreading is an obvious detrimental effect that limits the

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

Vestigial Side Band Demultiplexing for High Spectral Efficiency WDM Systems

Vestigial Side Band Demultiplexing for High Spectral Efficiency WDM Systems The University of Kansas Technical Report Vestigial Side Band Demultiplexing for High Spectral Efficiency WDM Systems Chidambaram Pavanasam and Kenneth Demarest ITTC-FY4-TR-737- March 4 Project Sponsor:

More information

Performance analysis of Erbium Doped Fiber Amplifier at different pumping configurations

Performance analysis of Erbium Doped Fiber Amplifier at different pumping configurations Performance analysis of Erbium Doped Fiber Amplifier at different pumping configurations Mayur Date M.E. Scholar Department of Electronics and Communication Ujjain Engineering College, Ujjain (M.P.) datemayur3@gmail.com

More information

EXAMINATION FOR THE DEGREE OF B.E. and M.E. Semester

EXAMINATION FOR THE DEGREE OF B.E. and M.E. Semester EXAMINATION FOR THE DEGREE OF B.E. and M.E. Semester 2 2009 101908 OPTICAL COMMUNICATION ENGINEERING (Elec Eng 4041) 105302 SPECIAL STUDIES IN MARINE ENGINEERING (Elec Eng 7072) Official Reading Time:

More information

Power penalty caused by Stimulated Raman Scattering in WDM Systems

Power penalty caused by Stimulated Raman Scattering in WDM Systems Paper Power penalty caused by Stimulated Raman Scattering in WDM Systems Sławomir Pietrzyk, Waldemar Szczęsny, and Marian Marciniak Abstract In this paper we present results of an investigation into the

More information

Optical solitons in a silicon waveguide

Optical solitons in a silicon waveguide Optical solitons in a silicon waveguide Jidong Zhang 1, Qiang Lin 2, Giovanni Piredda 2, Robert W. Boyd 2, Govind P. Agrawal 2, and Philippe M. Fauchet 1,2 1 Department of Electrical and Computer Engineering,

More information

A 3.9 ns 8.9 mw 4 4 Silicon Photonic Switch Hybrid-Integrated with CMOS Driver

A 3.9 ns 8.9 mw 4 4 Silicon Photonic Switch Hybrid-Integrated with CMOS Driver A 3.9 ns 8.9 mw 4 4 Silicon Photonic Switch Hybrid-Integrated with CMOS Driver A. Rylyakov, C. Schow, B. Lee, W. Green, J. Van Campenhout, M. Yang, F. Doany, S. Assefa, C. Jahnes, J. Kash, Y. Vlasov IBM

More information

Optical Fiber Technology. Photonic Network By Dr. M H Zaidi

Optical Fiber Technology. Photonic Network By Dr. M H Zaidi Optical Fiber Technology Numerical Aperture (NA) What is numerical aperture (NA)? Numerical aperture is the measure of the light gathering ability of optical fiber The higher the NA, the larger the core

More information

Technical Feasibility of 4x25 Gb/s PMD for 40km at 1310nm using SOAs

Technical Feasibility of 4x25 Gb/s PMD for 40km at 1310nm using SOAs Technical Feasibility of 4x25 Gb/s PMD for 40km at 1310nm using SOAs Ramón Gutiérrez-Castrejón RGutierrezC@ii.unam.mx Tel. +52 55 5623 3600 x8824 Universidad Nacional Autonoma de Mexico Introduction A

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

Phase Sensitive Amplifier Based on Ultrashort Pump Pulses

Phase Sensitive Amplifier Based on Ultrashort Pump Pulses Phase Sensitive Amplifier Based on Ultrashort Pump Pulses Alexander Gershikov and Gad Eisenstein Department of Electrical Engineering, Technion, Haifa, 32000, Israel. Corresponding author: alexger@campus.technion.ac.il

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

ANALYSIS OF DISPERSION COMPENSATION IN A SINGLE MODE OPTICAL FIBER COMMUNICATION SYSTEM

ANALYSIS OF DISPERSION COMPENSATION IN A SINGLE MODE OPTICAL FIBER COMMUNICATION SYSTEM ANAYSIS OF DISPERSION COMPENSATION IN A SINGE MODE OPTICA FIBER COMMUNICATION SYSTEM Sani Abdullahi Mohammed 1, Engr. Yahya Adamu and Engr. Matthew Kwatri uka 3 1,,3 Department of Electrical and Electronics

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

UNIT Write notes on broadening of pulse in the fiber dispersion?

UNIT Write notes on broadening of pulse in the fiber dispersion? UNIT 3 1. Write notes on broadening of pulse in the fiber dispersion? Ans: The dispersion of the transmitted optical signal causes distortion for both digital and analog transmission along optical fibers.

More information

SIGNAL DEGRADATION IN OPTICAL FIBERS

SIGNAL DEGRADATION IN OPTICAL FIBERS Volume Issue January 04, ISSN 348 8050 SIGNAL DEGRADATION IN OPTICAL FIBERS Gyan Prakash Pal, Manishankar Gupta,,, Assistant Professor, Electronics & Communication Engineering Department, Shanti Institute

More information

Analysis of Self Phase Modulation Fiber nonlinearity in Optical Transmission System with Dispersion

Analysis of Self Phase Modulation Fiber nonlinearity in Optical Transmission System with Dispersion 36 Analysis of Self Phase Modulation Fiber nonlinearity in Optical Transmission System with Dispersion Supreet Singh 1, Kulwinder Singh 2 1 Department of Electronics and Communication Engineering, Punjabi

More information

WDM Transmitter Based on Spectral Slicing of Similariton Spectrum

WDM Transmitter Based on Spectral Slicing of Similariton Spectrum WDM Transmitter Based on Spectral Slicing of Similariton Spectrum Leila Graini and Kaddour Saouchi Laboratory of Study and Research in Instrumentation and Communication of Annaba (LERICA), Department of

More information

UNIT-II : SIGNAL DEGRADATION IN OPTICAL FIBERS

UNIT-II : SIGNAL DEGRADATION IN OPTICAL FIBERS UNIT-II : SIGNAL DEGRADATION IN OPTICAL FIBERS The Signal Transmitting through the fiber is degraded by two mechanisms. i) Attenuation ii) Dispersion Both are important to determine the transmission characteristics

More information

The Report of Gain Performance Characteristics of the Erbium Doped Fiber Amplifier (EDFA)

The Report of Gain Performance Characteristics of the Erbium Doped Fiber Amplifier (EDFA) The Report of Gain Performance Characteristics of the Erbium Doped Fiber Amplifier (EDFA) Masruri Masruri (186520) 22/05/2008 1 Laboratory Setup The laboratory setup using in this laboratory experiment

More information

Physical Layer Modelling of Semiconductor Optical Amplifier Based Terabit/second Switch Fabrics

Physical Layer Modelling of Semiconductor Optical Amplifier Based Terabit/second Switch Fabrics Physical Layer Modelling of Semiconductor Optical Amplifier Based Terabit/second Switch Fabrics K.A. Williams, E.T. Aw*, H. Wang*, R.V. Penty*, I.H. White* COBRA Research Institute Eindhoven University

More information

HIGH-EFFICIENCY MQW ELECTROABSORPTION MODULATORS

HIGH-EFFICIENCY MQW ELECTROABSORPTION MODULATORS HIGH-EFFICIENCY MQW ELECTROABSORPTION MODULATORS J. Piprek, Y.-J. Chiu, S.-Z. Zhang (1), J. E. Bowers, C. Prott (2), and H. Hillmer (2) University of California, ECE Department, Santa Barbara, CA 93106

More information

Ultralow-power all-optical RAM based on nanocavities

Ultralow-power all-optical RAM based on nanocavities Supplementary information SUPPLEMENTARY INFORMATION Ultralow-power all-optical RAM based on nanocavities Kengo Nozaki, Akihiko Shinya, Shinji Matsuo, Yasumasa Suzaki, Toru Segawa, Tomonari Sato, Yoshihiro

More information

Multimode Optical Fiber

Multimode Optical Fiber Multimode Optical Fiber 1 OBJECTIVE Determine the optical modes that exist for multimode step index fibers and investigate their performance on optical systems. 2 PRE-LAB The backbone of optical systems

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

S Optical Networks Course Lecture 4: Transmission System Engineering

S Optical Networks Course Lecture 4: Transmission System Engineering S-72.3340 Optical Networks Course Lecture 4: Transmission System Engineering Edward Mutafungwa Communications Laboratory, Helsinki University of Technology, P. O. Box 2300, FIN-02015 TKK, Finland Tel:

More information

Chirped Bragg Grating Dispersion Compensation in Dense Wavelength Division Multiplexing Optical Long-Haul Networks

Chirped Bragg Grating Dispersion Compensation in Dense Wavelength Division Multiplexing Optical Long-Haul Networks 363 Chirped Bragg Grating Dispersion Compensation in Dense Wavelength Division Multiplexing Optical Long-Haul Networks CHAOUI Fahd 3, HAJAJI Anas 1, AGHZOUT Otman 2,4, CHAKKOUR Mounia 3, EL YAKHLOUFI Mounir

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

O. Mahran 1,2 and A.A.Samir 1

O. Mahran 1,2 and A.A.Samir 1 International Journal of Scientific & Engineering Research, Volume 6, Issue 1, January-2015 1306 The Effect of the Amplifier Length on the Gain and Noise Figure of the Er/Yb Co-Doped Waveguide Amplifiers

More information

Characterization of Chirped volume bragg grating (CVBG)

Characterization of Chirped volume bragg grating (CVBG) Characterization of Chirped volume bragg grating (CVBG) Sobhy Kholaif September 7, 017 1 Laser pulses Ultrashort laser pulses have extremely short pulse duration. When the pulse duration is less than picoseconds

More information

Lecture 5 Fiber Optical Communication Lecture 5, Slide 1

Lecture 5 Fiber Optical Communication Lecture 5, Slide 1 Lecture 5 Bit error rate The Q value Receiver sensitivity Sensitivity degradation Extinction ratio RIN Timing jitter Chirp Forward error correction Fiber Optical Communication Lecture 5, Slide 1 Bit error

More information

Optical Local Area Networking

Optical Local Area Networking Optical Local Area Networking Richard Penty and Ian White Cambridge University Engineering Department Trumpington Street, Cambridge, CB2 1PZ, UK Tel: +44 1223 767029, Fax: +44 1223 767032, e-mail:rvp11@eng.cam.ac.uk

More information

Four wave mixing and parametric amplification in Si-nano waveguides using reverse biased pnjunctions

Four wave mixing and parametric amplification in Si-nano waveguides using reverse biased pnjunctions Four wave mixing and parametric amplification in Si-nano waveguides using reverse biased pnjunctions for carrier removal E-Mail: petermann@tu-berlin.de Acknowledgements A.Gajda 1, G.Winzer 1, L.Zimmermann

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

PERFORMANCE ASSESSMENT OF TWO-CHANNEL DISPERSION SUPPORTED TRANSMISSION SYSTEMS USING SINGLE AND DOUBLE-CAVITY FABRY-PEROT FILTERS AS DEMULTIPLEXERS

PERFORMANCE ASSESSMENT OF TWO-CHANNEL DISPERSION SUPPORTED TRANSMISSION SYSTEMS USING SINGLE AND DOUBLE-CAVITY FABRY-PEROT FILTERS AS DEMULTIPLEXERS PERFORMANCE ASSESSMENT OF TWO-CHANNEL DISPERSION SUPPORTED TRANSMISSION SYSTEMS USING SINGLE AND DOUBLE-CAVITY FABRY-PEROT FILTERS AS DEMULTIPLEXERS Mário M. Freire Department of Mathematics and Information

More information

Dispersion properties of mid infrared optical materials

Dispersion properties of mid infrared optical materials Dispersion properties of mid infrared optical materials Andrei Tokmakoff December 16 Contents 1) Dispersion calculations for ultrafast mid IR pulses ) Index of refraction of optical materials in the mid

More information

Dispersion and Ultrashort Pulses II

Dispersion and Ultrashort Pulses II Dispersion and Ultrashort Pulses II Generating negative groupdelay dispersion angular dispersion Pulse compression Prisms Gratings Chirped mirrors Chirped vs. transform-limited A transform-limited pulse:

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

Performance Analysis of SOA-MZI based All-Optical AND & XOR Gate

Performance Analysis of SOA-MZI based All-Optical AND & XOR Gate International Journal of Current Engineering and Technology E-ISSN 2277 4106, P-ISSN 2347 5161 2016 INPRESSCO, All Rights Reserved Available at http://inpressco.com/category/ijcet Research Article Utkarsh

More information

Slow, Fast, and Backwards Light: Fundamental Aspects

Slow, Fast, and Backwards Light: Fundamental Aspects Slow, Fast, and Backwards Light: Fundamental Aspects Robert W. Boyd University of Rochester Paul Narum Norwegian Defence Research Establishment with George Gehring, Giovanni Piredda, Aaron Schweinsberg,

More information

Improving the efficiency of an optical parametric oscillator by tailoring the pump pulse shape

Improving the efficiency of an optical parametric oscillator by tailoring the pump pulse shape Improving the efficiency of an optical parametric oscillator by tailoring the pump pulse shape Zachary Sacks, 1,* Ofer Gayer, 2 Eran Tal, 1 and Ady Arie 2 1 Elbit Systems El Op, P.O. Box 1165, Rehovot

More information

Supercontinuum based all-optical Digital communication system at 2THz

Supercontinuum based all-optical Digital communication system at 2THz Supercontinuum based all-optical Digital communication system at 2THz Sai Venkatesh Balasubramanian Sree Sai Vidhya Mandhir, Mallasandra, Bengaluru-569, Karnataka, India. saivenkateshbalasubramanian@gmail.com

More information

Optical Transport Tutorial

Optical Transport Tutorial Optical Transport Tutorial 4 February 2015 2015 OpticalCloudInfra Proprietary 1 Content Optical Transport Basics Assessment of Optical Communication Quality Bit Error Rate and Q Factor Wavelength Division

More information

OTemp: Optical Thermal Effect Modeling Platform User Manual

OTemp: Optical Thermal Effect Modeling Platform User Manual OTemp: Optical Thermal Effect Modeling Platform User Manual Version 1., July 214 Mobile Computing System Lab Department of Electronic and Computer Engineering The Hong Kong University of Science and Technology

More information

DIRECT MODULATION WITH SIDE-MODE INJECTION IN OPTICAL CATV TRANSPORT SYSTEMS

DIRECT MODULATION WITH SIDE-MODE INJECTION IN OPTICAL CATV TRANSPORT SYSTEMS Progress In Electromagnetics Research Letters, Vol. 11, 73 82, 2009 DIRECT MODULATION WITH SIDE-MODE INJECTION IN OPTICAL CATV TRANSPORT SYSTEMS W.-J. Ho, H.-H. Lu, C.-H. Chang, W.-Y. Lin, and H.-S. Su

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

All-Optical and Opto-Electronic Signal Regenerators

All-Optical and Opto-Electronic Signal Regenerators All-Optical and Opto-Electronic Signal Regenerators Masayuki Graduate School of Engineering Osaka University 15th International SAOT Workshop on All-Optical Signal Regeneration September 28-29, 2011 1

More information

Workshop on Coherent Phenomena in Disordered Optical Systems May Slow-light Propagation in Photonic Nano-Structures

Workshop on Coherent Phenomena in Disordered Optical Systems May Slow-light Propagation in Photonic Nano-Structures 2583-15 Workshop on Coherent Phenomena in Disordered Optical Systems 26-30 May 2014 Slow-light Propagation in Photonic Nano-Structures Jin HOU College of Electronics & Information Engineering, South-Central

More information

Chaotic communication in radio-over-fiber transmission based on optoelectronic feedback semiconductor lasers

Chaotic communication in radio-over-fiber transmission based on optoelectronic feedback semiconductor lasers Chaotic communication in radio-over-fiber transmission based on optoelectronic feedback semiconductor lasers Fan-Yi Lin* and Meng-Chiao Tsai Institute of Photonics Technologies, Department of Electrical

More information

Ultra Short Two-Section Vertical Directional Coupler Switches with High Extinction Ratios

Ultra Short Two-Section Vertical Directional Coupler Switches with High Extinction Ratios Jpn. J. Appl. Phys. Vol. 40 (2001) pp. 4045 4050 Part 1, No. 6A, June 2001 c 2001 The Japan Society of Applied Physics Ultra Short Two-Section Vertical Directional Coupler Switches with High Extinction

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

Lecture 3. Optical Noise. Lecture 3. Noise in Optical Amplification. Noise Spectrum. Noise Figure

Lecture 3. Optical Noise. Lecture 3. Noise in Optical Amplification. Noise Spectrum. Noise Figure in Sources Power Factor Limit Optical ECE 185 Lasers and Modulators Lab - Spring 2018 1 in Sources Power Factor Limit We treat noise on a per mode basis Total noise is then noise/mode number of modes An

More information

Optimisation of DSF and SOA based Phase Conjugators. by Incorporating Noise-Suppressing Fibre Gratings

Optimisation of DSF and SOA based Phase Conjugators. by Incorporating Noise-Suppressing Fibre Gratings Optimisation of DSF and SOA based Phase Conjugators by Incorporating Noise-Suppressing Fibre Gratings Paper no: 1471 S. Y. Set, H. Geiger, R. I. Laming, M. J. Cole and L. Reekie Optoelectronics Research

More information

MODELING OF BROADBAND LIGHT SOURCE FOR OPTICAL NETWORK APPLICATIONS USING FIBER NON-LINEAR EFFECT

MODELING OF BROADBAND LIGHT SOURCE FOR OPTICAL NETWORK APPLICATIONS USING FIBER NON-LINEAR EFFECT MODELING OF BROADBAND LIGHT SOURCE FOR OPTICAL NETWORK APPLICATIONS USING FIBER NON-LINEAR EFFECT 1 G GEETHA, 2 I LAKSHMI PRIYA, 3 M MEENAKSHI 1 Associate Professor, Department of ECE, CEG, Anna University,

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

Optimization of supercontinuum generation in photonic crystal fibers for pulse compression

Optimization of supercontinuum generation in photonic crystal fibers for pulse compression Optimization of supercontinuum generation in photonic crystal fibers for pulse compression Noah Chang Herbert Winful,Ted Norris Center for Ultrafast Optical Science University of Michigan What is Photonic

More information

Pulse breaking recovery in fiber lasers

Pulse breaking recovery in fiber lasers Pulse breaking recovery in fiber lasers L. M. Zhao 1,, D. Y. Tang 1 *, H. Y. Tam 3, and C. Lu 1 School of Electrical and Electronic Engineering, Nanyang Technological University, Singapore 639798 Department

More information

1. Evolution Of Fiber Optic Systems

1. Evolution Of Fiber Optic Systems OPTICAL FIBER COMMUNICATION UNIT-I : OPTICAL FIBERS STRUCTURE: 1. Evolution Of Fiber Optic Systems The operating range of optical fiber system term and the characteristics of the four key components of

More information

OPTICAL COMMUNICATIONS S

OPTICAL COMMUNICATIONS S OPTICAL COMMUNICATIONS S-108.3110 1 Course program 1. Introduction and Optical Fibers 2. Nonlinear Effects in Optical Fibers 3. Fiber-Optic Components 4. Transmitters and Receivers 5. Fiber-Optic Measurements

More information

Physics of Waveguide Photodetectors with Integrated Amplification

Physics of Waveguide Photodetectors with Integrated Amplification Physics of Waveguide Photodetectors with Integrated Amplification J. Piprek, D. Lasaosa, D. Pasquariello, and J. E. Bowers Electrical and Computer Engineering Department University of California, Santa

More information

All-Optical Processing for Ultrafast Data Networks Using Semiconductor Optical Amplifiers

All-Optical Processing for Ultrafast Data Networks Using Semiconductor Optical Amplifiers All-Optical Processing for Ultrafast Data Networks Using Semiconductor Optical Amplifiers Jade P. Wang Ph.D. Thesis Defense Thesis Committee: Professor Erich P. Ippen, Dr. Scott A. Hamilton, Professor

More information

Module 10 - Optical Amplifiers

Module 10 - Optical Amplifiers Module 10 - Optical Amplifiers Dr. Alan Kost Associate Research Professor Of Optical Sciences, University Of Arizona Dr. Alan Kost is an Associate Research Professor of Optical Sciences in the University

More information

Reference Distribution

Reference Distribution EPAC 08, Genoa, Italy RF Reference Signal Distribution System for FAIR M. Bousonville, GSI, Darmstadt, Germany P. Meissner, Technical University Darmstadt, Germany Dipl.-Ing. Michael Bousonville Page 1

More information

Title. Author(s)Fujisawa, Takeshi; Koshiba, Masanori. CitationOptics Letters, 31(1): Issue Date Doc URL. Rights. Type.

Title. Author(s)Fujisawa, Takeshi; Koshiba, Masanori. CitationOptics Letters, 31(1): Issue Date Doc URL. Rights. Type. Title Polarization-independent optical directional coupler Author(s)Fujisawa, Takeshi; Koshiba, Masanori CitationOptics Letters, 31(1): 56-58 Issue Date 2006 Doc URL http://hdl.handle.net/2115/948 Rights

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

Optical Amplifiers. Continued. Photonic Network By Dr. M H Zaidi

Optical Amplifiers. Continued. Photonic Network By Dr. M H Zaidi Optical Amplifiers Continued EDFA Multi Stage Designs 1st Active Stage Co-pumped 2nd Active Stage Counter-pumped Input Signal Er 3+ Doped Fiber Er 3+ Doped Fiber Output Signal Optical Isolator Optical

More information

Degradation of BER by Group Delay in Digital Phase Modulation

Degradation of BER by Group Delay in Digital Phase Modulation The Fourth Advanced International Conference on Telecommunications Degradation of BER by Group Delay in Digital Phase Modulation A.Azizzadeh 1, L.Mohammadi 1 1 Iran Telecommunication Research Center (ITRC)

More information

Femtosecond pulse generation

Femtosecond pulse generation Femtosecond pulse generation Marc Hanna Laboratoire Charles Fabry Institut d Optique, CNRS, Université Paris-Saclay Outline Introduction 1 Fundamentals of modelocking 2 Femtosecond oscillator technology

More information

Performance Assessment of High Density Wavelength Division Multiplexing Systems with Dispersion Supported Transmission at 10 Gbit/s

Performance Assessment of High Density Wavelength Division Multiplexing Systems with Dispersion Supported Transmission at 10 Gbit/s Performance Assessment of High Density Wavelength Division Multiplexing Systems with Dispersion Supported Transmission at 10 Gbit/s Mário M. Freire Department of Mathematics and Computer Science, University

More information

Investigations on Yb-doped CW Fiber Lasers

Investigations on Yb-doped CW Fiber Lasers Investigations on Yb-doped CW Fiber Lasers B.N. Upadhyaya *1, S. Kher 1, M.R. Shenoy 2, K. Thyagarajan 2, T.P.S. Nathan 1 1 Solid State Laser Division, Centre for Advanced Technology, Indore, India-452013

More information

Theoretical and Simulation Approaches for Studying Compensation Strategies of Nonlinear Effects Digital Lightwave Links Using DWDM Technology

Theoretical and Simulation Approaches for Studying Compensation Strategies of Nonlinear Effects Digital Lightwave Links Using DWDM Technology Journal of Computer Science (11): 887-89, 007 ISSN 1549-66 007 Science Publications Theoretical and Simulation Approaches for Studying Compensation Strategies of Nonlinear Effects Digital Lightwave Links

More information

Ultra-fast all-optical wavelength conversion in silicon waveguides using femtosecond pulses

Ultra-fast all-optical wavelength conversion in silicon waveguides using femtosecond pulses Ultra-fast all-optical wavelength conversion in silicon waveguides using femtosecond pulses R.Dekker a, J. Niehusmann b, M. Först b, and A. Driessen a a Integrated Optical Micro Systems, Mesa+, University

More information

Overview. Tasks: 1.1. Realization of a direct coherent microwave-to-optical link

Overview. Tasks: 1.1. Realization of a direct coherent microwave-to-optical link Overview Optical cavity Microwave cavity Mechanical resonator Tasks: 1.1. Realization of a direct coherent microwave-to-optical link 1.2 Development of large gain-bandwidth product microwave amplifiers

More information

Universidade do Algarve Faculdade de Ciências e Tecnologia Departamento de Física Ano lectivo

Universidade do Algarve Faculdade de Ciências e Tecnologia Departamento de Física Ano lectivo Universidade do Algarve Faculdade de Ciências e Tecnologia Departamento de Física Ano lectivo 2016-2017 Unidade Curricular Sistemas de Comunicação Ótica Optical Communication Systems Mestrado Integrado

More information

Performance Improvement of 40-Gb/s Capacity Four-Channel WDM. Dispersion-Supported Transmission by Using Broadened Passband

Performance Improvement of 40-Gb/s Capacity Four-Channel WDM. Dispersion-Supported Transmission by Using Broadened Passband Performance Improvement of 40-Gb/s Capacity Four-Channel WDM Dispersion-Supported Transmission by Using Broadened Passband Arrayed-Waveguide Grating Demultiplexers Mário M. Freire Department of Mathematics

More information

WITH the vast rise in parallel multicore architectures, the

WITH the vast rise in parallel multicore architectures, the JOURNAL OF LIGHTWAVE TECHNOLOGY, VOL. 34, NO. 12, JUNE 15, 2016 2975 Comprehensive Design Space Exploration of Silicon Photonic Interconnects Meisam Bahadori, Student Member, IEEE, Sébastien Rumley, Member,

More information

All optical wavelength converter based on fiber cross-phase modulation and fiber Bragg grating

All optical wavelength converter based on fiber cross-phase modulation and fiber Bragg grating All optical wavelength converter based on fiber cross-phase modulation and fiber Bragg grating Pavel Honzatko a, a Institute of Photonics and Electronics, Academy of Sciences of the Czech Republic, v.v.i.,

More information