Analysis of Phase Noise in a fiber-optic link

Slides:



Advertisements
Similar presentations
Data Communications and Networking
Advertisements

S Digital Communication Systems Fiber-optic Communications - Supplementary.
Chromatic Dispersion Measurement methods  Pulse Delay Method (time-of-flight) ‏ IEC / ITU-T G650.1 EIA/TIA-455- FOTP-175-B  Phase Shift Method.
Present status of the laser system for KAGRA Univ. of Tokyo Mio Lab. Photon Science Center SUZUKI, Ken-ichiro.
END. PRESENTATION CONTENTS THESIS TILTLE (1) PRESENTATION CONTENTS (1) INTRODUCTION (2) DESIGN PROCEDURES (2) DESIGN SPECIFICATION (1) DESIGN FACTOR (5)
Optical Fibre Communication Systems
Modulation formats for digital fiber transmission
Lecture 8 Optical Fiber Amplifier – noise and BER Last lecture Introduction to Fiber Optical Amplifier – types and applications Erbium-doped fiber.
Snell’s Law    n2n2 n1n1 n1n1 Light rays bend when traversing boundaries between media with different refractive index: in out See
STUDY OF AMPLIFICATION ON ERBIUM DOPED FIBER AMPLIFIER Lita Rahmasari, Assoc. Prof. Dr. Yusof Munajat, Prof. Dr. Rosly Abdul Rahman Optoelectronics Laboratory,
Reports of optical fiber communication systems
1 ISIS-IPHOBAC SUMMER SCHOOL, May 17-18, 2007, Budapest, Hungary "Broadband Architectures and Functions" Photonic microwave signal processing Jianping.
Fiber Bragg Gratings.
Information Transmission
Chapter 7 Photonic Transmission Systems (Digital & Analog)
L5 Optical Fiber Link and LAN Design
WP06_AntennaIF. WP06_AntennaIF 3 principal modules switch amplifier (= ATA ‘PAM’) –includes attenuators (0-60 dB), power detector, and bias tee for the.
Lock-in amplifiers
Coherent System in Remote Antenna Application
Wireless Transmission Fundamentals (Physical Layer) Professor Honggang Wang
Spectrum Analyzer Basics Copyright 2000 Agenda Overview: What is spectrum analysis? What measurements do we make? Theory of Operation: Spectrum analyzer.
Servos Servos are everywhere. Elements of servo System -- to be controlled Sensor or detector -- measure quantity to be controlled Reference -- desired.
Light Wave Systems Dr Manoj Kumar Professor & Head Department of ECE DAVIET,Jalandhar.
NESCOT CATC1 Cable Testing CCNA 1 v3 – Module 4. NESCOT CATC2 Waves 1. The _________ of the waves is the amount of time between each wave, measured in.
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.
CE 4228 Data Communications and Networking

Effects of EDFA Gain on RF Phase Noise in a WDM Fiber Optic Link John Summerfield, Mehdi Shadaram, and Jennifer Bratton Photonics Research Laboratory Department.
Summary Thus far we have: ECE 4710: Lecture #39
Multi Frequency Laser Driver for Near Infrared Optical Spectroscopy in Biomedical Application Chenpeng Mu Department of Electrical and Computer Engineering,
Chapter 10 Optical Communication Systems
CLIPPING DISTORTION IN LASER DIODE: MODEL, SIMULATIONS AND STATISTICS By: Omar Falou.
CHAPTER 7 SYSTEM DESIGN. Transmission Types Two types of transmissions: - Link (point to point) - Network -point to multipoint -Mesh -Ring.
ECE 4710: Lecture #36 1 Chapter 8  Chapter 8 : Wired and Wireless Communication Systems  Telephone  Fiber Optic  DSL  Satellite  Digital & Analog.
MOCT(Magneto Optic Current Transduser)
1/21 Chapter 4 – Transmission Media. 2/21 Overview  guided – copper twisted pair, coaxial cable optical fiber  unguided – wireless; through air, vacuum,
Fig. 3 Wind measurements experimental setup Lidar (light detection and ranging) operates using the same concept of microwave RADAR, but it employs a lot.
Phase and Gain stability of optical fibre link used in MeerKAT Author : Roufurd Julie Supervised by : Prof Michael Inggs SKA HCD bursary conference Dec.
Definition: Nonlinear effect that occurs in nonlinear optical materials such as photonic switch, optical fiber cable, etc. This interaction between waves.
RF Phase Noise in WDM Fiber Optic Links Mehdi Shadaram, Cecil Thomas *, John Summerfield, and Pushkar Chennu Department of Electrical and Computer Engineering,
Fiber Optic Transmission SL/HL – Option C.3. Reflection/Refraction Reflection – A wave encounters a boundary between two mediums and cannot pass through.
SPECTRUM ANALYZER 9 kHz GHz
© 2014 IBM Corporation IBM Research - Zurich VCSEL based Radio-over-Fiber Links for Radio Astronomy Jonas Weiss, IBM Zurich Research Lab, Switzerland.
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.
Fiber Optic Transmission SL/HL – Option F Mr. Jean.
EE 230: Optical Fiber Communication Lecture 12
FIBER OPTIC TRANSMISSION
Generation of Spurious Signals in Nonlinear Frequency Conversion Tyler Brewer, Russell Barbour, Zeb Barber.
IB Physics Option F – Fibre Optics Mr. Jean. The plan: Video clip of the day Fibre Optics – C+-+Imaginghttps://ibphysics2016.wikispaces.com/Option+
Krzysztof Czuba1 REFERENCE FREQUENCY DISTRIBUTION SYSTEM FOR THE TESLA TECHNOLOGY BASED PROJECTS Krzysztof Czuba Matthias Felber.
Receiver Circuit Testing Test setup Eye diagrams BER measurement Eye - BER relationship.
教育部顧問室光通訊系統教育改進計畫台科大 師大 淡江 東南 萬能 教育部顧問室光通訊系統教育改進計畫 台科大 師大 淡江 東南 萬能 3. 光調變器之性能量測 (Modulation Measurements) Modulation measurement is essential in characterizing.
Date of download: 6/23/2016 Copyright © 2016 SPIE. All rights reserved. A schematic design of the all-dielectric polymer waveguide E-field sensor (a).
Date of download: 6/25/2016 Copyright © 2016 SPIE. All rights reserved. Photograph (top) and structure (bottom) of the transmitter module. Figure Legend:
Fundamentals of Communications. Communication System Transmitter: originates the signal Receiver: receives transmitted signal after it travels over the.
Date of download: 9/17/2016 Copyright © 2016 SPIE. All rights reserved. Top: Schematic representation of input and output signals. LF-intensity-modulated.
OptiSystem applications: Photodiode sensitivity modelling
Eng.: Ahmed Abdo AbouelFadl
by: Mrs. Aboli N. Moharil Assistant Professor, EXTC dept.
Optical Amplifier.
Methods of transfer of ultra-stable frequencies to radio telescope
Subject Name: Optical Fiber Communication Subject Code: 10EC72
Introduction to electronic communication systems
Lock-in amplifiers
Device test stations Multi-probe electrical DC injection and optical input/output Near-field measurement Analogue characteristics 1) 50GHz Network analyzer,
Fiber Optic Transmission
Fibre Optic Transmission
Transverse coherence and polarization measurement of 131 nm coherent femtosecond pulses from a seeded FEL J. Schwenke, E. Mansten, F. Lindau, N. Cutic,
ANALOG AND DIGITAL LINKS
Presentation transcript:

Analysis of Phase Noise in a fiber-optic link Cecil D. Thomas Aug 20 ’04

Outline Introduction Why optical fibers? > Huge bandwidth > Immunity to interference > Low attenuation > Etc. * Where do we use optical fibers? Problems in a fiber link > Attenuation > Dispersion > Phase noise ( How to quantify this problem in different applications?) > etc. * Conclusions

Analog fiber-optic links are used in Distribution of reference signals like local oscillators. Video transmission as in Cable TV. Antenna remoting for radar systems. Etc.

Major problems in a fiber-optic link Attenuation = deterioration in signal strength Dispersion = pulse broadening (causes ISI) Phase Noise Etc.

Significance of Phase Noise A high merit frequency distribution system should perform with a phase fluctuation of less than 1 degree over several days of operation. Detection range, dynamic range, range resolution etc. are some of the radar parameters affected by phase instabilities. Poor phase noise degrades the quality of television pictures and data transmission.

Definition of Phase Noise

What causes phase noise in a fiber-optic link? Temperature fluctuation of the link Fluctuation of longitudinally applied stress Relative intensity noise of the laser Back reflections in the cable Bias fluctuations of the photodiode Bias fluctuations of either directly modulated laser or the external modulator Amplified spontaneous emission noise Etc.

Our Tasks Quantify Phase Noise in the fiber-optic link Study the effect of Wavelength selection Study the effect of optical amplification Assumptions External modulation and direct detection Optical amplification

Block diagram of experimental setup Laser Modulator EDFA Photo detector Phase detector Filter RF Amp Phase shift = 90 degrees

Methodology Signal from the RF source traverses two separate paths before reaching the phase-detector > 8.8 Km of fiber after modulating the laser output > One meter of electric cable The length of the electric cable is adjusted so that the phase difference between the two paths is 90 degrees. Time samples from the digital oscilloscope are downloaded to a PC. Matlab is then used to calculate Power Spectral Density from the time-voltage samples.

Average noise floor = -85.66dBm/Hz

Effect of wavelength selection (no optical amplification)

Effect of varying the output power of laser source

Output power vs. Input Power of EDFA

Effect of EDFA

Phase noise for different input powers

Conclusions Phase noise in an optical fiber-link was quantified Wavelength selection does not have much effect on phase noise (< 2dB). As laser power output increases, phase noise increases almost linearly (effect of shot noise, thermal noise). Average phase noise increases by about 2.7dB with the addition of the EDFA. For EDFA, phase noise decreases as input power increases (matches with theory).