Dr. Rüdiger Paschotta RP Photonics Consulting GmbH

Slides:



Advertisements
Similar presentations
Dr. Rüdiger Paschotta RP Photonics Consulting GmbH
Advertisements

Beyond The Standard Quantum Limit B. W. Barr Institute for Gravitational Research University of Glasgow.
Radio over fiber.
Mostly by Gwyn Williams and the JLab Team, Presented by D. Douglas Working Group 4 Diagnostics & Synchronization Requirements Where we are and what needs.
// RF Transceiver Design Condensed course for 3TU students Peter Baltus Eindhoven University of Technology Department of Electrical Engineering
Chapter 3. Noise Husheng Li The University of Tennessee.
Nuclear Magnetic Resonance
Lecture: 10 New Trends in Optical Networks
Koji Arai – LIGO Laboratory / Caltech LIGO-G v2.
1 Optical Fibre Amplifiers. 2 Introduction to Optical Amplifiers Raman Fibre Amplifier Brillouin Fibre Amplifier Doped Fibre Amplifier.
Coherent Lightwave Systems
Department of Electronic Engineering City University of Hong Kong EE3900 Computer Networks Data Transmission Slide 1 Continuous & Discrete Signals.
Fiber-Optic Communications
Integrated Circuits Design for Applications in Communications Dr. Charles Surya Department of Electronic and Information Engineering DE636  6220
Laser to RF synchronisation A.Winter, Aachen University and DESY Miniworkshop on XFEL Short Bunch Measurement and Timing.
A quantum optical beam n Classically an optical beam can have well defined amplitude AND phase simultaneously. n Quantum mechanics however imposes an uncertainty.
Fiber Optic Receiver A fiber optic receiver is an electro-optic device that accepts optical signals from an optical fiber and converts them into electrical.
1 Cessna EME Lab Reverb Chamber Emissions Matthew Wills EME Lab Supervisor December 7th, 2004.
Array Waveguide Gratings (AWGs). Optical fiber is a popular carrier of long distance communications due to its potential speed, flexibility and reliability.
Spectrum Analyzer Basics Copyright 2000 Agenda Overview: What is spectrum analysis? What measurements do we make? Theory of Operation: Spectrum analyzer.
Spectrum Analyzer Basics Copyright 2000 Agenda Overview: What is spectrum analysis? What measurements do we make? Theory of Operation: Spectrum analyzer.
Formatting and Baseband Modulation
4/11/2006BAE Application of photodiodes A brief overview.
Servos Servos are everywhere. Elements of servo System -- to be controlled Sensor or detector -- measure quantity to be controlled Reference -- desired.
3/26/2003BAE of 10 Application of photodiodes A brief overview.
Analysis of Phase Noise in a fiber-optic link
This teaching material is a part of e-Photon/ONe Master study in Optical Communications and Networks Course and module: Author(s): No part of this presentation.
CE 4228 Data Communications and Networking
RF readout scheme to overcome the SQL Feb. 16 th, 2004 Aspen Meeting Kentaro Somiya LIGO-G Z.
Controlling the dynamics time scale of a diode laser using filtered optical feedback. A.P.A. FISCHER, Laboratoire de Physique des Lasers, Universite Paris.
Chapter 10 Optical Communication Systems
Copyright 1998, S.D. Personick. All Rights Reserved. Telecommunications Networking I Lectures 12&13 Fiber Optics.
Lab Group L2Bx EECE 380 – Electrical Engineering Design Studio (Spring 2014) 1 Spectrum Analyzer Michael Halpenny-Mason, Presenter 2, Presenter 3, Presenter.
Modulation techniques for length sensing and control of advanced optical topologies B.W. Barr, S.H. Huttner, J.R. Taylor, B. Sorazu, M.V. Plissi and K.A.
Injection Locked Oscillators Optoelectronic Applications E. Shumakher, J. Lasri, B. Sheinman, G. Eisenstein, D. Ritter Electrical Engineering Dept. TECHNION.
SPECTRUM ANALYZER 9 kHz GHz
Optical Amplifiers By: Ryan Galloway.
EE 230: Optical Fiber Communication Lecture 12
Photodetectors What is photodetector (PD)? Photodetector properties
Stefan Hild 111th WG1 meeting, Hannover, January 2007 DC-Readout for GEO Stefan Hild for the GEO-team.
Signal Analyzers. Introduction In the first 14 chapters we discussed measurement techniques in the time domain, that is, measurement of parameters that.
High precision phase monitoring Alexandra Andersson, CERN Jonathan Sladen, CERN This work is supported by the Commission of the European Communities under.
Optical and Quantum Communications Group June 9, 2005 Three Themes for Theory Research: Gaussian States, Coherent Laser Radars, and Multi-Photon Detectors.
Cape Electrical and Electronic Technology Topic: Electromagnetic Waves By: Tahvorn George & Charles,J.
December 1997 Circuit Analysis Examples 걼 Hairpin Edge Coupled Filter 걼 Bipolar Amplifier 걼 Statistical Analysis and Design Centering 걼 Frequency Doubler.
April 12 | Comparison of Sophisticated Synthesizer Concepts and Modern Step Attenuator Implementations | 2 Comparison of Sophisticated Synthesizer Concepts.
The Proposed Holographic Noise Experiment Rainer Weiss, MIT On behalf of the proposing group Fermi Lab Proposal Review November 3, 2009.
By. Jadhav Avinash J Roll no - 2K13E11. Reference: Hewlett Packard Agilent Technology Wikipedia GwINSTEK.
What is thermal noise? Thermal noise in the resistance of the signal source is the fundamental limit on achievable signal sensitivity is unavoidable, and.
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).
SUPERHETERODYNE SPECTRUM ANALYZER. TOPICS Superheterodyne spectrum analyzer – Basic architecture – Frequency resolution – Sweep time – Video section.
Application of photodiodes
OptiSystem applications: Photodiode sensitivity modelling
H1 Squeezing Experiment: the path to an Advanced Squeezer
Four wave mixing in submicron waveguides
Quantum noise reduction using squeezed states in LIGO
Optical PLL for homodyne detection
The Proposed Holographic Noise Experiment
Integrated Semiconductor Modelocked Lasers
Progress toward squeeze injection in Enhanced LIGO
A. Bramati M. Romanelli E. Giacobino
Optoelectronic Microwave Oscillators
Homodyne or heterodyne Readout for Advanced LIGO?
Quantum Information with Continuous Variables
A New OEO Design Using Optical Phase Modulation and Modulation Suppression G. John Dick and Nan Yu Jet Propulsion Laboratory, California Institute of Technology.
8.5 Modulation of Signals basic idea and goals
RF readout scheme to overcome the SQL
Noise I Abigail Firme.
ANALOG AND DIGITAL LINKS
Presentation transcript:

Dr. Rüdiger Paschotta RP Photonics Consulting GmbH Competence Area: Fluctuations & Noise

Overview: Noise in Optics and Electronics Why we need to understand noise Topics in this area. For various topics, the following is given: short description of topic previous activities of R. Paschotta in this field (See the website for references on scientific results) examples for possible consulting activities Note: for more details (with references to publications) on the scientific achievements of R. Paschotta, see http://www.rp-photonics.com/Science_Paschotta.ppt

Why we Need to Understand Noise Noise is often a limiting factor for the performance of a device or system. Examples: transmission rate of telecommunication system limited by the need to keep the bit error rate low enough; sensitivity of measurements is limited by noise. Efficient product development often requires quantification of noise from components calculation of noise effects on system performance Noise issues can have an important impact on system cost. Example: by choosing the right measurement scheme, which is less sensitive to noise, one might do the job with a less costly laser system. Note: incompetent noise specifications can irritate customers! If that kind of competence is not available in house, have your staff trained!

Topics in this Area Mathematical description of noise Origins of noise Electronic noise measurements Optical noise measurements Feedback systems for noise suppression Noise modeling

Mathematical Description of Noise

Mathematical Description of Noise Noise of devices or systems needs to be reliably quantified. Reason: designs based on properly quantified noise properties save development time and cost by eliminating trial & error. This requires correct measurements, but also correct and helpful specifications. Specification and comparison of noise properties is not trivial due to manifold types of quantities (power spectral densities, correlation functions, probability distributions, etc.) mathematical difficulties (related to divergent quantities, required approximations, statistics, etc.) inconsistent notations in the literature (different sign conventions, one- or two-sided power spectral densities, f or w variables, 2p issues, etc.) Only a real expert can do reliable and efficient work in this field.

Mathematical Description of Noise Examples for previous activities of R. Paschotta: Extensive calculations on quantum noise and thermal fluctuations in optics and electronics Group-internal teaching on noise specifications

Mathematical Description of Noise Examples for possible consulting activities: Checking noise specifications of a product for completeness and soundness, so as to convince your customers. Investing just half a day of consulting can help to secure sales. Comparing noise specs of your product to theoretical expectations. Otherwise you won’t know whether there is room for further improvement. Checking whether the noise specs of a product will be sufficient for your application, or compare noise specs of different products, or calculate limits to the expected performance. Don’t loose a lot of money by trying things which can’t work, or by buying the wrong product. Training your personnel in such areas. Is there a more cost-efficient way to obtain solid know-how?

Origins of Noise gain medium HR OC pump noise spontaneous emission, dipole fluctuations losses introduce vacuum fluctuations additional classical noise vacuum fluctuations

Origins of Noise Thermal fluctuations: often an important source of noise in electronic circuits, e.g. in photodiode preamplifiers Other electronic noise, e.g. flicker noise: various sources; may critically depend on parts used Quantum noise: often important in optical devices, e.g. shot noise in photodetection or intensity and phase noise in lasers Mechanical noise: e.g. in the form of vibrations which can couple to optical or electronic parameters

Origins of Noise Examples for previous activities of R. Paschotta: Comparison of noise influences in highly nonlinear pulse propagation in photonic crystal fibers Comprehensive analysis of various noise influences on the timing jitter and the optical phase noise of mode-locked lasers, using a combination of new analytical calculations and numerical techniques

Origins of Noise Examples for possible consulting activities: Calculate the expected impact of different noise sources on the performance of your product. Or would you prefer guess work to guide your development? Identify the dominating effect to avoid working on the wrong aspect Identify the key factors for optimization and quantify the remaining potential so that your decisions will be well founded

Electronic Noise Measurements envelope detector mixer tunable oscillator f RBW log VBW sample peak A/D converter S/H display detector display attenuator

Electronic Noise Measurements Noise in electrical signals is often measured with RF spectrum analyzers. Such measurements are prone to an intimidating ensemble of possible errors: confusion between 3-dB bandwidth and effective noise bandwidth statistical effects from averaging logarithmic (dBm) values wrong detector mode: peak detector overestimates noise, particularly when combined with wrong video averaging saturation of mixer or logarithmic amplifier by signals outside the displayed range influence of phase noise from local oscillator Correct noise measurements with an RF spectrum analyzer require a decent understanding of how such a device works.

Electronic Noise Measurements Examples for previous activities of R. Paschotta: Acquired a deep understanding of electronic spectrum analyzers Optimization of photodetector circuits for noise measurements below the shot noise limit ( experiments with nonclassical states of light) Development of new measurement schemes for low levels of phase noise Detailed lecturing

Electronic Noise Measurements Examples for possible consulting activities: Comparison of different technical approaches for noise measurements ideally before you heavily invest into some scheme Development of a measurement setup, or checking an existing setup and proposing improvements in a process during which your engineers can learn a lot Checking the data processing to ensure validity of the obtained data

Optical Noise Measurements oscillator 10.1 GHz laser 2 10 GHz laser 1 100 MHz FFT analyzer

Optical Noise Measurements Intensity noise: measurements e.g. with photodiodes or photomultiplier tubes Phase noise: beating with reference laser; heterodyne measurement with unbalanced Mach-Zehnder interferometer Timing jitter of mode-locked lasers: various measurement schemes exist – high demands for low jitter levels!

Optical Noise Measurements Examples for previous activities of R. Paschotta: Detection of nonclassical (“squeezed“) states of light below the shot noise limit Development of a novel measurement technique, which is very sensitive, very versatile (can be applied to free-running or timing-stabilized mode-locked lasers), and does not require an ultrastable electronic reference oscillator

Optical Noise Measurements Examples for possible consulting activities: Compare different measurement techniques Help to set up measurements of relative intensity noise, phase noise, or timing jitter Identify limiting factors of existing measurement setups and propose possible improvements

Feedback Systems for Noise Suppression mode-locked laser RF analyzer

Feedback Systems for Noise Suppression Noise can often be suppressed with automatic feedback systems. Examples: Stabilization of a laser output power Stabilization of the gain or average output power in telecom amplifiers Phase locking the pulses of a mode-locked laser to an electronic reference Effective stabilization and suppression of oscillations requires well-designed feedback loop Limits for stabilization arise from dead times, electronic noise, quantum effects, etc.

Feedback Systems for Noise Suppression Examples for previous activities of R. Paschotta: Designed and operated various electronic feedback systems Developed advanced schemes for timing stabilization of mode-locked lasers

Feedback Systems for Noise Suppression Examples for possible consulting activities: Design or check an electronic feedback system for the stabilization of an optical power Help to optimize the performance, considering control elements, optimized frequency response of feedback electronics, possible feed-forward schemes, etc.

Noise Modeling dipole fluctuations & vacuum fluctuations from OC pump noise dipole fluctuations & vacuum fluctuations from OC

Noise Modeling Models can greatly help to identify limiting factors optimize the design before trying in the lab verify by comparison with measurements whether the expectable performance is reached Analytical and/or numerical techniques are required, depending on the circumstances Noise modeling requires detailed know-how on mathematical issues, numerical techniques, physical effects, and technical possibilities, and extensive general experience of working with models. Note: Setting up a model is one thing – producing results is another one!

Noise Modeling Examples for previous activities of R. Paschotta: Analytical calculation of quantum noise properties of lasers, frequency doublers, parametric oscillators, etc. Numerical simulation of noise in highly nonlinear pulse propagation in photonic crystal fibers, and studies of its effects on pulse compression Modeling of timing noise and other noise properties of mode-locked lasers, based on quantum noise and classical noise inputs Note: R. Paschotta has developed extremely powerful and versatile simulation software, allowing to get quick and reliable results in graphical or text form.

Noise Modeling Examples for possible consulting activities: Give advice on what kind of model will be feasible, useful and efficient Set up a model and use it to answer concrete questions, e.g. on critical parameters possibilities for optimization effects of noise in components and systems (e.g. timing jitter, carrier-envelope offset noise, impact in metrology, e.g. in interferometers)