Broadband Laser Ranging: Optimizing the Design for Different Experiments
|
|
- Maximilian Lewis
- 6 years ago
- Views:
Transcription
1 Broadband Laser Ranging: Optimizing the Design for Different Experiments Patrick Younk May 2016 Operated by Los Alamos National Security, LLC for the U.S. Department of Energy's NNSA UNCLASSIFIED 1
2 Outline Why BLR Design Equations Calibration considerations LANL Prototype System: A wide pulse, Multiplexed Architecture Summary Operated by Los Alamos National Security, LLC for the U.S. Department of Energy's NNSA UNCLASSIFIED 2
3 Some Reasons to Field BLR 1. Indication of 1-D: When you want an indication that your experiment is 1-D or nearly 1-D throughout the motion. 2. Transverse Motion: When there may be transverse (or complex) motion, but you can only field probes along a single direction due to other constraints. 3. Interested in Displacement: When you are interested in position more than velocity, and/or when there may be drop-outs in the signal so that integrating the PDV signal is unreliable. 4. Interested in Thickness: When you want to measure the thickness of a cloud of ejecta particles (or any other semitransparent medium). May be other reasons.. Operated by Los Alamos National Security, LLC for the U.S. Department of Energy's NNSA UNCLASSIFIED 3
4 Some Reasons to Field OR, cont. We do not believe that ranging will have inherently better temporal or spatial resolution or sensitivity than a Doppler-based measurement. (Comparable but not better). Nor is ranging easier to field. Ranging is Complementary to PDV. Operated by Los Alamos National Security, LLC for the U.S. Department of Energy's NNSA UNCLASSIFIED 4
5 Design Equations. Usable Range: x = λ 2 FD Displacement Resolution*: Δx = λ 2 /(4w p ) Time Resolution*: Δt = w p D/ 12 Doppler Sensitivity: b x = (D 0 λ)v Max Pulse Energy: E pulse = (400 W/m) (D 0 w p /L) λ: center wavelength (nm) w p : Pulse BW (nm) F: Recording BW (GHz) D: Total Dispersion (ns/nm) D 0 : Dispersion on target (ns/nm) L: Length of Fiber to Target (m) * Resolution is the ability to differentiate two surfaces. Note that displacement precision is ~10x the displacement resolution for strong signals. Operated by Los Alamos National Security, LLC for the U.S. Department of Energy's NNSA UNCLASSIFIED 5
6 Design Equations for BLR. λ: center wavelength (nm) w p : Pulse BW (nm) F: Recording BW (GHz) D: Total Dispersion (ns/nm) D 0 : Dispersion on target (ns/nm) L: Length of Fiber to Target (m) Typical Design: D = 2 ns/nm (120 km of fiber), w p = 20 nm, λ = 1560 nm L = 30m, D 0 = ns/nm Performance: x = 12 cm, Δx = 30 µm, Δt = 12 ns. B x = 26 µm / (km/s) E pulse = 4.5 nj (~90 mw CW) The optimum values will be different for each experiment. * Resolution is the ability to differentiate two surfaces. Note that position precision (i.e., repeatability) is ~10x the resolution for strong signals. Operated by Los Alamos National Security, LLC for the U.S. Department of Energy's NNSA UNCLASSIFIED 6
7 Calibration The mapping of a time waveform to a distance. Two Categories of Methods: In Situ: Calibration at shot time. Ex Situ: Calibration before/after shot. Operated by Los Alamos National Security, LLC for the U.S. Department of Energy's NNSA 5 cm 10 cm UNCLASSIFIED 7
8 In Situ Calibration For example: Extra Reflection(s) in the reference leg of the interferometer at known distances. Benefits: Fairly straightforward to field. Confidence of calibration at shot-time. Concerns: Works well if the legs of the interferometer are well-matched in dispersion. If not, a more complicated calibration function may be required that cannot be constrained with this method. End of Reference Leg 50:50 VOA VOA Au Au τ Operated by Los Alamos National Security, LLC for the U.S. Department of Energy's NNSA UNCLASSIFIED 8
9 Ex Situ Calibration For example: Accurately moving the Reference Reflection to different known positions and recording the waveforms before the shot. Benefits: Gain confidence in the repeatability of the system before the shot. The entire interferometer is calibrated. Can do many Calibration Points without much trouble -> A Complex Calibration Function could be used. Concerns: The placement of the pulse in the analysis window has to be consistent between all cal records and the shot record. This can be done with a spectral feature or recording the heart beat of the laser. How much time will the Ex Situ Calibration take, and how far ahead of the shot should I do the calibration? Operated by Los Alamos National Security, LLC for the U.S. Department of Energy's NNSA UNCLASSIFIED 9
10 LANL Prototype System with Front- End and Back-End Multiplexing PDV sys. Custom 3U Chassis Seed Laser 1 km spool 2 W EDFA Key Points 8-ch time duplexed (only 4 channels shown here). Not highly integrated, but configurable (e.g., pulse width). Capable of several nj/ pulse. Good SNR on -50 db surfaces. Currently, one pair of channels are built. Ch4 Filter, 1560±10 Ch3 Ch2 10 km spool Ch1 1 2 circ PM Ch Splitter Tap Out DG switch EDFA VOA VOA FSD 120km DCM WDM WDM PM O-scope Object Ref. Reflector Operated by Los Alamos National Security, LLC for the U.S. Department of Energy's NNSA UNCLASSIFIED 10
11 LANL Prototype System R&D in Lab System in a Hardigg Rack Custom Chassis Thank you Lenny Tabaka and Ruben Manzanares Operated by Los Alamos National Security, LLC for the U.S. Department of Energy's NNSA UNCLASSIFIED 11
12 Latest Dynamic Tests at LANL, Week of May 23 Steel (100 mils) or Stainless Steel (5mils) Flyer Plate BLR in Fiber Layout on Flyer Plate SE-1 Detonator (Similar to RP-1) 2 mm BLR in Fiber Point (2) BLR Points Plastic Housing Al Standoffs Al Plate Probe Pigtails (2) AC Photonic Collimating Probes Operated by Los Alamos National Security, LLC for the U.S. Department of Energy's NNSA UNCLASSIFIED 12
13 Results: BLR Det Run #1 Simple Spectrogram of Data Record (time duplexed) Channel 1 Channel 2 Operated by Los Alamos National Security, LLC for the U.S. Department of Energy's NNSA UNCLASSIFIED 13
14 Results: BLR Det Run #2 Simple Spectrogram of Data Record (time duplexed) Channel 1 Channel 2 Operated by Los Alamos National Security, LLC for the U.S. Department of Energy's NNSA UNCLASSIFIED 14
15 BLR in Fiber: Det Run #1 Simple Spectrogram of Data Record This is an intriguing new diagnostic. More work has to be performed to understand its limitations, etc. Initial Motion Thank you, George and Steve for sharing this brand new data set! Possible location of new sheared end of fiber Weird features at later times Operated by Los Alamos National Security, LLC for the U.S. Department of Energy's NNSA UNCLASSIFIED 15
16 Summary The BLR Design Equations: You can build a BLR system that works for your experiment. But you probably can t build one system for all experiments. There are different ways to do calibration. The PI must decide which one is best or possible both. LANL has a prototype system with both front-end multiplexing and back-end multiplex architectures. Our first dynamic BLR and BLR In-Fiber shots were performed two weeks ago. We have several more shots planned this summer. The inter-lab working group has and will continue to help the BLR effort. Operated by Los Alamos National Security, LLC for the U.S. Department of Energy's NNSA UNCLASSIFIED 16
One & Two Dimensional Diagnostics for Detonators & Boosters
One & Two Dimensional Diagnostics for Detonators & Boosters S.A. Clarke, K.A. Thomas, C.D. Landon, & T.A. Mason Weapons Engineering Los Alamos National Lab NDIA Fuze Conference May 2007 LA-UR-07-3127 Diagnostics
More informationPhotonic Doppler Pressure Gauge (PDPG) Scott Levinson, Rod Russell & Stephan Bless Contact:
Photonic Doppler Pressure Gauge (PDPG) Scott Levinson, Rod Russell & Stephan Bless Contact: levinson@ieee.org 1 Why another gauge? Original Motivation: We wish to measure in situ pressure at multiple locations
More informationResolving the Velocity Vector in Two Dimensions
Resolving the Velocity Vector in Two Dimensions Presentation for the 5 th annual PDV Conference and Workshop, Ohio State University, Columbus, Ohio Matthew Briggs, Michael Shinas, Larry Hull Los Alamos
More informationSlow, Fast, and Backwards Light: Fundamentals and Applications Robert W. Boyd
Slow, Fast, and Backwards Light: Fundamentals and Applications Robert W. Boyd Institute of Optics and Department of Physics and Astronomy University of Rochester www.optics.rochester.edu/~boyd with George
More informationSecurity and implementation of differential phase shift quantum key distribution systems
Security and implementation of differential phase shift quantum key distribution systems Eleni Diamanti University Ph.D. Oral Examination June 1 st, 2006 Classical cryptography cryptography = κρυπτός +
More informationWolter Imaging On Z. Chris Bourdon, Manager Z Imaging and Spectroscopy Julia Vogel, LLNL; Ming Wu, SNL ICF Diagnostics Workshop, October 5 th 2015
Photos placed in horizontal position with even amount of white space between photos and header Wolter Imaging On Z Chris Bourdon, Manager Z Imaging and Spectroscopy Julia Vogel, LLNL; Ming Wu, SNL ICF
More informationApplication of Proton Radiography to High Energy Density Research
Application of Proton Radiography to High Energy Density Research S.A. Kolesnikov*, S.V. Dudin, V.B. Mintsev, A.V. Shutov, A.V. Utkin, V.E. Fortov IPCP RAS, Chernogolovka, Russia A.A. Golubev, V.S. Demidov,
More informationUsing a Relativistic Electron Beam to Generate Warm Dense Matter for Equation of State Studies
Using a Relativistic Electron Beam to Generate Warm Dense Matter for Equation of State Studies DOE/NV/25946--1257 M. J. Berninger National Security Technologies, LLC, Los Alamos, NM 87544 T. J. T. Kwan,
More informationAbstract Submitted for the DPP99 Meeting of The American Physical Society
Abstract Submitted for the DPP99 Meeting of The American Physical Society Sorting Category: 5.1.1.2(Experimental) Calibration of a Three Path Thomson System at DIII- D 1 B.D. BRAY, C.L. HSIEH, T.N. CARLSTROM,
More informationILC Laser-wires. G A Blair, RHUL Snowmass 17 th August 2005
ILC Laser-wires G A Blair, RHUL 17 th August 2005 Introduction Energy regimes Signal Extraction Scanning techniques Laser requirements Light delivery Summary Laser-wire Few microns GA Blair Laser-wire
More informationChamber Development Plan and Chamber Simulation Experiments
Chamber Development Plan and Chamber Simulation Experiments Farrokh Najmabadi HAPL Meeting November 12-13, 2001 Livermore, CA Electronic copy: http://aries.ucsd.edu/najmabadi/talks UCSD IFE Web Site: http://aries.ucsd.edu/ife
More informationCan we fake a signal with gratings, and what happened to 1/r 2?
1 Can we fake a signal with gratings, and what happened to 1/r 2? Experiments: Steve Hare, Mike Shinas, Matt Briggs Interpretation discussions: David Holtkamp, Dan Dolan, Jim Faulkner, Mike Shinas, Willard
More informationNanosecond Broadband Spectroscopy For Laser-Driven Compression Experiments
Nanosecond Broadband Spectroscopy For Laser-Driven Compression Experiments Dylan K. Spaulding, R. Jeanloz Department of Earth and Planetary Science, University of California, Berkeley307 McCone Hall, Berkeley,
More informationLecture 11: Doppler wind lidar
Lecture 11: Doppler wind lidar Why do we study winds? v Winds are the most important variable studying dynamics and transport in the atmosphere. v Wind measurements are critical to improvement of numerical
More informationNonlinear effects in optical fibers - v1. Miguel A. Muriel UPM-ETSIT-MUIT-CFOP
Nonlinear effects in optical fibers - v1 Miguel A. Muriel UPM-ETSIT-MUIT-CFOP Miguel A. Muriel-015/10-1 Nonlinear effects in optical fibers 1) Introduction ) Causes 3) Parameters 4) Fundamental processes
More informationObservation of Ultra-Wide Bandwidth SASE FEL
Observation of Ultra-Wide Bandwidth SASE FEL Gerard Andonian Particle Beam Physics Laboratory University of California Los Angeles The Physics and Applications of High Brightness Electron Beams Erice,
More informationPDV in a Railgun. The Institute for Advanced Technology The University of Texas at Austin. Scott Levinson, Sikhanda Satapathy, Dwight Landen,
PDV in a Railgun The Institute for Advanced Technology The University of Texas at Austin Scott Levinson, Sikhanda Satapathy, Dwight Landen, 8/14/27 17:51 2nd Annual PDV Workshop Aug 16-17, 27 Lawrence
More informationdisplacement measuring interferometery measurement uncertainty Mike Holmes and Chris Evans (contact info:
displacement measuring interferometery measurement uncertainty Mike Holmes and Chris Evans (contact info: mholmes@zygo.com) 1 agenda heterodyne displacement measuring interferometer (DMI) overview case
More informationSlow, Fast, and Backwards Light Propagation in Erbium-Doped Optical Fibers. Zhimin Shi
Slow, Fast, and Backwards Light Propagation in Erbium-Doped Optical Fibers Zhimin Shi Institute of Optics and Department of Physics and Astronomy University of Rochester www.optics.rochester.edu/~boyd
More informationULTRAFAST COMPONENTS
ULTRAFAST COMPONENTS Mirrors CVI Laser Optics offers both the PulseLine family of optical components and other existing product lines that are ideal for use with femtosecond lasers and associated applications.
More informationFiber-Optics Group Highlights of Micronova Department of Electrical and Communications Engineering Helsinki University of Technology
Highlights of 2004 Micronova Department of Electrical and Communications Engineering Micronova Seminar 3 December 2004 Group Leader: Hanne Ludvigsen Postdoctoral researcher: Goëry Genty Postgraduate students:
More informationDevelopment of Polarization Interferometer Based on Fourier Transform Spectroscopy for Thomson Scattering Diagnostics
16th International Toki Conference Advanced Imaging and Plasma Diagnostics Ceratopia Toki, Gifu, JAPAN December 5-8, 2006 Development of Polarization Interferometer Based on Fourier Transform Spectroscopy
More informationObservational methods for astrophysics. Pierre Hily-Blant
Observational methods for astrophysics Pierre Hily-Blant IPAG pierre.hily-blant@univ-grenoble-alpes.fr, OSUG-D/306 2016-17 P. Hily-Blant (Master2 APP) Observational methods 2016-17 1 / 323 VI Spectroscopy
More information! Fiber!Laser!Intracavity!Absorption! Spectroscopy!(FLICAS)!of!CO/CO2! mixture.!!! This experiment will expose you to tools and approaches, common in
FiberLaserIntracavityAbsorption Spectroscopy(FLICAS)ofCO/CO2 mixture. This experiment will expose you to tools and approaches, common in modern laser spectroscopy. During the following weeks we will cover
More informationSupplementary Information. Temporal tweezing of light through the trapping and manipulation of temporal cavity solitons.
Supplementary Information Temporal tweezing of light through the trapping and manipulation of temporal cavity solitons Jae K. Jang, Miro Erkintalo, Stéphane Coen, and Stuart G. Murdoch The Dodd-Walls Centre
More informationLecture 26. Wind Lidar (4) Direct Detection Doppler Lidar
Lecture 26. Wind Lidar (4) Direct Detection Doppler Lidar Considerations (Accuracy and Precision) for DDL Na-DEMOF DDL -- Multi-frequency edge-filter DDL New development of DDL -- DDL based on Fizeau etalon
More informationShock Wave Experiments Using PDV: Window Characterization at 1550 nm
Shock Wave Experiments Using PDV: Window Characterization at 1550 nm B. J. Jensen (DE-9), D. Holtkamp (P-22), D. H. Dolan (Sandia) Los Alamos National Laboratory Acknowlegements: Tim Pierce (DE-9), Mark
More informationBeam Shape and Halo Monitor Study
EUROPEAN ORGANISATION FOR NUCLEAR RESEARCH CERN A&B DEPARTMENT AB-Note-2006-047 ABP Beam Shape and Halo Monitor Study J-B. Lallement, E.Z. Sargsyan, M. Hori Abstract The Beam Shape and Halo Monitor, designed
More informationSimilarities of PMD and DMD for 10Gbps Equalization
Similarities of PMD and DMD for 10Gbps Equalization Moe Win Jack Winters win/jhw@research.att.com AT&T Labs-Research (Some viewgraphs and results curtesy of Julien Porrier) Outline Polarization Mode Dispersion
More informationNonlinear Effects in Optical Fiber. Dr. Mohammad Faisal Assistant Professor Dept. of EEE, BUET
Nonlinear Effects in Optical Fiber Dr. Mohammad Faisal Assistant Professor Dept. of EEE, BUET Fiber Nonlinearities The response of any dielectric material to the light becomes nonlinear for intense electromagnetic
More informationPhotonic Displacement Interferometer
Photonic Displacement Interferometer Thermomechanical Shock (TMS) and Early Thermostructural Response (TSR) Measurement Applications Scott C. Jones Sandia National Laboratories Radiation Materials Science,
More informationRemote Raman & Fluorescence Capabilities for Chemical Detection at University of Hawaii
Remote Raman & Fluorescence Capabilities for Chemical Detection at University of Hawaii Anupam Misra Shiv Sharma HIGP, SOEST, Univ. of Hawaii * Daytime Operation * Long Detection Range (no sample collection)
More informationOPTICAL COMMUNICATIONS
L21-1 OPTICAL COMMUNICATIONS Free-Space Propagation: Similar to radiowaves (but more absorption by clouds, haze) Same expressions: antenna gain, effective area, power received Examples: TV controllers,
More informationDOE NNSA B&W Y-12, LLC Argonne National Lab University of Missouri INR Pitesti. IAEA Consultancy Meeting Vienna, August 24-27, 2010
Stress Analysis Finite Element Modeling DOE NNSA B&W Y-12, LLC Argonne National Lab University of Missouri INR Pitesti IAEA Consultancy Meeting Vienna, August 24-27, 2010 Target Manufacturing & Processing
More informationOptimization of Thermal Radiation Source for High Temperature Infrared Thermometer Calibration
Optimization of Thermal Radiation Source for High Temperature Infrared Thermometer Calibration Gavin McQuillan NLA T&M Conference Guateng, September 26-28, 2016 2011 Fluke Calibration 1 Outline Introduction
More informationThe Nulling Coronagraph Using a Nulling Interferometer for Planet Detection in Visible Light with a Single Aperture Telescope
Terrestrial Planet Finder The Nulling Coronagraph Using a Nulling Interferometer for Planet Detection in Visible Light with a Single Aperture Telescope Michael Shao, B. Martin Levine, Duncan Liu, J. Kent
More informationTemperature measurement and real-time validation
Temperature measurement and real-time validation A. Herrmann, B. Sieglin, M. Faitsch, P. de Marné, ASDEX Upgrade team st IAEA Technical Meeting on Fusion Data Processing, Validation and Analysis ITER-
More informationNTUA. Physics Department, National Technical University of Athens. June IPRD10,, Siena, Italy S. Maltezos SIENA ITALY
NTUA SIENA ITALY ATMOSPHERIC MONITORING FOR VERY HIGH ENERGY GAMMA RAY CHERENKOV TELESCOPES BASED ON HSRL: DEVELOPMENT OF HIGH ACCURACY NON-INVASIVE ETALON CHARACTERIZATION TECHNIQUES S. Maltezos,, E.
More informationX-band Experience at FEL
X-band Experience at FERMI@Elettra FEL Gerardo D Auria Elettra - Sincrotrone Trieste GdA_TIARA Workshop, Ångström Laboratory, June 17-19, 2013 1 Outline The FERMI@Elettra FEL project Machine layout and
More informationVASCO Flex TM Remote Particle size Analyzer
Technical note NT01-VASCO Flex_EN_V01 VASCO Flex TM Remote Particle size Analyzer Nano-particle Size measurements brought into your process! 1 VASCO Flex TM Analyzer: «in situ» Nano Particle size measurement
More informationMEFT / Quantum Optics and Lasers. Suggested problems Set 4 Gonçalo Figueira, spring 2015
MEFT / Quantum Optics and Lasers Suggested problems Set 4 Gonçalo Figueira, spring 05 Note: some problems are taken or adapted from Fundamentals of Photonics, in which case the corresponding number is
More informationPART 2 : BALANCED HOMODYNE DETECTION
PART 2 : BALANCED HOMODYNE DETECTION Michael G. Raymer Oregon Center for Optics, University of Oregon raymer@uoregon.edu 1 of 31 OUTLINE PART 1 1. Noise Properties of Photodetectors 2. Quantization of
More informationObservation of spectral enhancement in a soliton fiber laser with fiber Bragg grating
Observation of spectral enhancement in a soliton fiber laser with fiber Bragg grating L. M. Zhao 1*, C. Lu 1, H. Y. Tam 2, D. Y. Tang 3, L. Xia 3, and P. Shum 3 1 Department of Electronic and Information
More informationStimulated Emission. Electrons can absorb photons from medium. Accelerated electrons emit light to return their ground state
Lecture 15 Stimulated Emission Devices- Lasers Stimulated emission and light amplification Einstein coefficients Optical fiber amplifiers Gas laser and He-Ne Laser The output spectrum of a gas laser Laser
More informationLarge Plasma Device (LAPD)
Large Plasma Device (LAPD) Over 450 Access ports Computer Controlled Data Acquisition Microwave Interferometers Laser Induced Fluorescence DC Magnetic Field: 0.05-4 kg, variable on axis Highly Ionized
More informationFundamental investigation on CO 2 laser-produced Sn plasma for an EUVL source
Fundamental investigation on CO 2 laser-produced Sn plasma for an EUVL source Yezheng Tao*, Mark Tillack, Kevin Sequoia, Russel Burdt, Sam Yuspeh, and Farrokh Najmabadi University of California, San Diego
More informationExperimental Measurements of the ORION Photoinjector Drive Laser Oscillator Subsystem
Experimental Measurements of the ORION Photoinjector Drive Laser Oscillator Subsystem D.T Palmer and R. Akre Laser Issues for Electron RF Photoinjectors October 23-25, 2002 Stanford Linear Accelerator
More informationSupporting Online Material for
www.sciencemag.org/cgi/content/full/313/5794/1765/dc1 Supporting Online Material for Self-Healing Pulse-Like Shear Ruptures in the Laboratory George Lykotrafitis, Ares J. Rosakis,* Guruswami Ravichandran
More informationThomson Scattering from Nonlinear Electron Plasma Waves
Thomson Scattering from Nonlinear Electron Plasma Waves A. DAVIES, 1 J. KATZ, 1 S. BUCHT, 1 D. HABERBERGER, 1 J. BROMAGE, 1 J. D. ZUEGEL, 1 J. D. SADLER, 2 P. A. NORREYS, 3 R. BINGHAM, 4 R. TRINES, 5 L.O.
More informationRichard Miles and Arthur Dogariu. Mechanical and Aerospace Engineering Princeton University, Princeton, NJ 08540, USA
Richard Miles and Arthur Dogariu Mechanical and Aerospace Engineering Princeton University, Princeton, NJ 08540, USA Workshop on Oxygen Plasma Kinetics Sept 20, 2016 Financial support: ONR and MetroLaser
More informationTiming and cross-talk properties of BURLE multi-channel MCP-PMTs
Timing and cross-talk properties of BURLE multi-channel MCP-PMTs, Peter Križan, Rok Pestotnik University of Maribor, University of Ljubljana and Jožef Stefan Institute Outline of the talk: Motivation:
More informationMaRIE. MaRIE X-Ray Free-Electron Laser Pre-Conceptual Design
Operated by Los Alamos National Security, LLC, for the U.S. Department of Energy MaRIE (Matter-Radiation Interactions in Extremes) MaRIE X-Ray Free-Electron Laser Pre-Conceptual Design B. Carlsten, C.
More informationSystem optimization of a long-range Brillouin-loss-based distributed fiber sensor
System optimization of a long-range Brillouin-loss-based distributed fiber sensor Yongkang Dong, 1,2 Liang Chen, 1 and Xiaoyi Bao 1, * 1 Fiber Optics Group, Department of Physics, University of Ottawa,
More informationQuantum Imaging Technologies: Quantum Laser Radar
MURI 2005 Quantum Imaging: New Methods and Applications Year 3 Review / 17 November 2008 / UMBC, Baltimore, MD Quantum Imaging Technologies: Quantum Laser Radar Prem Kumar and Geraldo Barbosa EECS Department,
More informationFATIGUE DAMAGE PROGRESSION IN PLASTICS DURING CYCLIC BALL INDENTATION
FATIGUE DAMAGE PROGRESSION IN PLASTICS DURING CYCLIC BALL INDENTATION AKIO YONEZU, TAKAYASU HIRAKAWA, TAKESHI OGAWA and MIKIO TAKEMOTO Department of Mechanical Engineering, College of Science and Engineering,
More informationLecture 32. Lidar Error and Sensitivity Analysis
Lecture 3. Lidar Error and Sensitivity Analysis Introduction Accuracy in lidar measurements Precision in lidar measurements Error analysis for Na Doppler lidar Sensitivity analysis Summary 1 Errors vs.
More informationSIZE-SELECTED AEROSOL FILTER ANALYSIS USING ELECTROSTATIC CLASSIFICATION AND LIBS
SIZE-SELECTED AEROSOL FILTER ANALYSIS USING ELECTROSTATIC CLASSIFICATION AND LIBS APPLICATION NOTE LIBS-023 Quantitative elemental composition analysis is possible using size-selected aerosol samples collected
More informationIn situ wavelength calibration of the edge CXS spectrometers on JET
EUROFUSION WPJET1-PR(16) 15408 E Delabie et al. In situ wavelength calibration of the edge CXS spectrometers on JET Preprint of Paper to be submitted for publication in 21st Topical Conference on High
More informationExperiment O-2. The Michelson Interferometer
Experiment O-2 The Michelson Interferometer The Michelson interferometer is one of the best known and historically important interferometers. It is a very accurate length-measuring device and has been
More informationLarge area scintillation detector for dosimetric stand with improved light collection
NUKLEONIKA 2011;56(4):317 321 ORIGINAL PAPER Large area scintillation detector for dosimetric stand with improved light collection Bronisław Machaj, Jan Mirowicz, Ewa Kowalska Abstract. In order to improve
More informationVELA/CLARA as Advanced Accelerator Studies Test-bed at Daresbury Lab.
VELA/CLARA as Advanced Accelerator Studies Test-bed at Daresbury Lab. Yuri Saveliev on behalf of VELA and CLARA teams STFC, ASTeC, Cockcroft Institute Daresbury Lab., UK Outline VELA (Versatile Electron
More informationNonlinear ultrafast fiber optic devices based on Carbon Nanotubes
Nonlinear ultrafast fiber optic devices based on Carbon Nanotubes Guillermo E. Villanueva, Claudio J. Oton Michael B. Jakubinek, Benoit Simard,, Jaques Albert, Pere Pérez-Millán Outline Introduction CNT-coated
More informationADAPTIVE EQUALIZATION AT MULTI-GHZ DATARATES
ADAPTIVE EQUALIZATION AT MULTI-GHZ DATARATES Department of Electrical Engineering Indian Institute of Technology, Madras 1st February 2007 Outline Introduction. Approaches to electronic mitigation - ADC
More informationDesign studies for a neutrino telescope based on optical fiber hydrophones
Design studies for a neutrino telescope based on optical fiber hydrophones TNO Technical Sciences, P.O. Box 155, 2600 AD Delft, The Netherlands E-mail: ernst-jan.buis@tno.nl E. Doppenberg TNO Technical
More informationLecture 9. PMTs and Laser Noise. Lecture 9. Photon Counting. Photomultiplier Tubes (PMTs) Laser Phase Noise. Relative Intensity
s and Laser Phase Phase Density ECE 185 Lasers and Modulators Lab - Spring 2018 1 Detectors Continuous Output Internal Photoelectron Flux Thermal Filtered External Current w(t) Sensor i(t) External System
More informationSensing Rotation with Light: From Fiber Optic Gyroscope to Exceptional Points
Sensing Rotation with Light: From Fiber Optic Gyroscope to Exceptional Points Michel Digonnet Applied Physics Department Stanford University Stanford University 1 The Sagnac Effect in Vacuum! The fiber
More informationQuantum optics and squeezed states of light
Quantum optics and squeezed states of light Eugeniy E. Mikhailov The College of William & Mary June 15, 2012 Eugeniy E. Mikhailov (W&M) Quantum optics June 15, 2012 1 / 44 From ray optics to semiclassical
More information6WDWXVRI/,*2. Laser Interferometer Gravitational-wave Observatory. Nergis Mavalvala MIT IAU214, August 2002 LIGO-G D
6WDWXVRI/,*2 Laser Interferometer Gravitational-wave Observatory Hanford, WA Livingston, LA Nergis Mavalvala MIT IAU214, August 2002 *UDYLWDWLRQDOZDYH,QWHUIHURPHWHUVWKHSULQ LSOH General Relativity (Einstein
More informationII) Experimental Design
SLAC Experimental Advisory Committee --- September 12 th, 1997 II) Experimental Design Theory and simulations Great promise of significant scientific and technological achievements! How to realize this
More informationSpectral Resolution in Interferometry
Spectral Resolution in Interferometry Christopher Tycner Michelson Postdoctoral Fellow @ U. S. Naval Observatory Flagstaff Station Outline Spectral Resolution in Interferometry Implementation Benefits
More informationMapping Rise Time Information with Down-Shift Analysis
DOE/NV/25946--1361 Mapping Rise Time Information with Down-Shift Analysis Thomas W. Tunnell, Eric A. Machorro, and Abel B. Diaz National Security Technologies, LLC This work was done by National Security
More informationIntroduction to FT-IR Spectroscopy
Introduction to FT-IR Spectroscopy An FT-IR Spectrometer is an instrument which acquires broadband NIR to FIR spectra. Unlike a dispersive instrument, i.e. grating monochromator or spectrograph, an FT-IR
More informationPropagation losses in optical fibers
Chapter Dielectric Waveguides and Optical Fibers 1-Fev-017 Propagation losses in optical fibers Charles Kao, Nobel Laureate (009) Courtesy of the Chinese University of Hong Kong S.O. Kasap, Optoelectronics
More informationCalibration of Ocean Colour Sensors
Dr. A. Neumann German Aerospace Centre DLR Remote Sensing Technology Institute Marine Remote Sensing What is Calibration, why do we need it? Sensor Components Definition of Terms Calibration Standards
More informationMeasurments with Michelson interferometers
Please do not remove this manual from from the lab. It is available at www.cm.ph.bham.ac.uk/y2lab Optics Measurments with Michelson interferometers Objectives In this experiment you will: Understand the
More informationNonlinear Optics (WiSe 2016/17) Lecture 9: December 16, 2016 Continue 9 Optical Parametric Amplifiers and Oscillators
Nonlinear Optics (WiSe 2016/17) Lecture 9: December 16, 2016 Continue 9 Optical Parametric Amplifiers and Oscillators 9.10 Passive CEP-stabilization in parametric amplifiers 9.10.1 Active versus passive
More informationOptical amplifiers and their applications. Ref: Optical Fiber Communications by: G. Keiser; 3 rd edition
Optical amplifiers and their applications Ref: Optical Fiber Communications by: G. Keiser; 3 rd edition Optical Amplifiers Two main classes of optical amplifiers include: Semiconductor Optical Amplifiers
More informationhock-timing Measurements in ctly Driven Spherical ICF Targets
Spectrometer wo-beam SPIDER for dual-pulse single-shot characterization Doug French1, Christophe Dorrer2, and Igor Jovanovic1 hock-iming Measurements in ctly Driven Spherical ICF argets 1Department of
More informationSelf-Phase Modulation in Optical Fiber Communications: Good or Bad?
1/100 Self-Phase Modulation in Optical Fiber Communications: Good or Bad? Govind P. Agrawal Institute of Optics University of Rochester Rochester, NY 14627 c 2007 G. P. Agrawal Outline Historical Introduction
More informationChapter 5. Transmission System Engineering. Design the physical layer Allocate power margin for each impairment Make trade-off
Chapter 5 Transmission System Engineering Design the physical layer Allocate power margin for each impairment Make trade-off 1 5.1 System Model Only digital systems are considered Using NRZ codes BER is
More informationFSA TM Multi-bit Digital Processors
Laser Diagnostics FSA TM Multi-bit Digital Processors Revolutionary, State-of-the- Art Digital Signal Processing for Velocity and Size TSI is the only instrument supplier that developed two powerful, digital
More informationCommissioning of the SNS Beam Instrumentation
Commissioning of the SNS Beam Instrumentation Commissioning of the SNS Beam Instrumentation Tom Shea for the SNS Diagnostics Team Oak Ridge National Laboratory (ORNL), Oak Ridge, TN, USA The Spallation
More informationA New Spectrometer for the Green Bank Telescope
A New Spectrometer for the Green Bank Telescope Marty Bloss, Patrick Brandt, Hong Chen, Jayanth Chennamangalam, Jeff Cobb, Ramon Creager, Paul Demorest, Glenn Jones, Randy McCullough, Jason Ray, D. Anish
More informationStimulated Emission Devices: LASERS
Stimulated Emission Devices: LASERS 1. Stimulated Emission and Photon Amplification E 2 E 2 E 2 hυ hυ hυ In hυ Out hυ E 1 E 1 E 1 (a) Absorption (b) Spontaneous emission (c) Stimulated emission The Principle
More informationFRONTAL AND TILTED PDV PROBES FOR MEASURING VELOCITY HISTORY OF LASER- SHOCK INDUCED CALIBRATED PARTICLES
FRONTAL AND TILTED PDV PROBES FOR MEASURING VELOCITY HISTORY OF LASER- SHOCK INDUCED CALIBRATED PARTICLES Gabriel PRUDHOMME (Ph.D. student), Patrick MERCIER Jacky BENIER, Pierre-Antoine FRUGIER Laurent
More informationRayleigh-Brillouin Scattering Experiment with Atmospheric Lidar from a Mountain Observatory
Rayleigh-Brillouin Scattering Experiment with Atmospheric Lidar from a Mountain Observatory Oliver Reitebuch, Christian Lemmerz, Engelbert Nagel, Benjamin Witschas Institut für Physik der Atmosphäre intensity
More informationStudies of Hadron Calorimeter
Studies of Hadron Calorimeter Zhigang Wang Institute of High Energy Physics 2012.10.17 in IHEP Outline 1,The Dark Matter Calorimeter 2,The Hadron Calorimeter(HCAL) 3, Summary 1,Dark Matter Calorimeter
More informationLayout of the HHG seeding experiment at FLASH
Layout of the HHG seeding experiment at FLASH V. Miltchev on behalf of the sflash team: A. Azima, J. Bödewadt, H. Delsim-Hashemi, M. Drescher, S. Düsterer, J. Feldhaus, R. Ischebeck, S. Khan, T. Laarmann
More informationOptimization of Wall Velocity Measurements Using Photonic Doppler Velocimetry (PDV) *)
Optimization of Wall Velocity Measurements Using Photonic Doppler Velocimetry... 89 Central European Journal of Energetic Materials, 2015, 12(1), 89-97 ISSN 2353-1843 Optimization of Wall Velocity Measurements
More informationContinuous-variable quantum key distribution with a locally generated local oscillator
Continuous-variable quantum key distribution with a locally generated local oscillator Bing Qi, Pavel Lougovski, Raphael Pooser, Warren Grice, Miljko Bobrek, Charles Ci Wen Lim, and Philip G. Evans Quantum
More informationHOW ADVANCED PYROMETERS INCREASE THERMAL PROCESS REPEATABILITY AND PRODUCT QUALITY
HOW ADVANCED PYROMETERS INCREASE THERMAL PROCESS REPEATABILITY AND PRODUCT QUALITY Accurate temperature measurement is key for controlling the stability and repeatability of many temperature-critical processes.
More informationGratings in Electrooptic Polymer Devices
Gratings in Electrooptic Polymer Devices Venkata N.P.Sivashankar 1, Edward M. McKenna 2 and Alan R.Mickelson 3 Department of Electrical and Computer Engineering, University of Colorado at Boulder, Boulder,
More informationMid-infrared supercontinuum covering the µm molecular fingerprint region using ultra-high NA chalcogenide step-index fibre
SUPPLEMENTARY INFORMATION DOI: 1.138/NPHOTON.214.213 Mid-infrared supercontinuum covering the 1.4 13.3 µm molecular fingerprint region using ultra-high NA chalcogenide step-index fibre Christian Rosenberg
More informationC S N f - 7 7Ob / 5'+RADIATION TEMPERATURE MEASUREMENTS
- 9 7-2903 C S N f - 7 7Ob / 5'+RADATON TEMPERATURE MEASUREMENTS N LASER-HEATED HOHLRAUMS *.-r-3 9, w " b,:~l*w;+$ij" ; ;r-j c J. A. Cobblel, A. V. Bessarabz, A. V. Kuninz, V. A. Tokarev2, S. R. Goldmanl,
More informationB 2 P 2, which implies that g B should be
Enhanced Summary of G.P. Agrawal Nonlinear Fiber Optics (3rd ed) Chapter 9 on SBS Stimulated Brillouin scattering is a nonlinear three-wave interaction between a forward-going laser pump beam P, a forward-going
More informationOPTI510R: Photonics. Khanh Kieu College of Optical Sciences, University of Arizona Meinel building R.626
OPTI510R: Photonics Khanh Kieu College of Optical Sciences, University of Arizona kkieu@optics.arizona.edu Meinel building R.626 Important announcements Homework #1 is due. Homework #2 is assigned, due
More informationAir Flow through Woven Stainless Steel Mesh
Air Flow through Woven Stainless Steel Mesh Abstract It was known that a mesh screen placed across an airflow will have an evening effect, distributing both the velocity and pressure across the screen,
More informationNoise Correlations in Dual Frequency VECSEL
Noise Correlations in Dual Frequency VECSEL S. De, A. El Amili, F. Bretenaker Laboratoire Aimé Cotton, CNRS, Orsay, France V. Pal, R. Ghosh Jawaharlal Nehru University, Delhi, India M. Alouini Institut
More informationLecture 20. Wind Lidar (2) Vector Wind Determination
Lecture 20. Wind Lidar (2) Vector Wind Determination Vector wind determination Ideal vector wind measurement VAD and DBS technique for vector wind Coherent versus incoherent Detection Doppler wind lidar
More informationApplication of high-precision temperature-controlled FBG f ilter and light source self-calibration technique in the BOTDR sensor system
Application of high-precision temperature-controlled FBG f ilter and light source self-calibration technique in the BOTDR sensor system Jiacheng Hu ( ) 1,2, Fuchang Chen ( ) 1,2, Chengtao Zhang ( ) 1,2,
More information