Scintillators for SwissFEL
|
|
- Maximillian Hodge
- 6 years ago
- Views:
Transcription
1 P AUL SCHERRER INSTITUT Scintillators for SwissFEL Usage of Scintillators at the SwissFEL Injector Test Facility Rasmus Ischebeck, for the PSI Diagnostics Group
2 Scintillators for SwissFEL Profile monitors for Photocathode laser Electron beam Loss monitors Beam containment Wire scanners 2
3 SwissFEL Injector Test Facility Test the generation of beams suitable for SwissFEL operation Accelerating Cavity Quadrupole Magnets Beam Position Monitor Profile Monitor 3
4 !"#$%$&#'()"*&+#,("+--*./*0$%$-'1 <#*-,&4'E&*-.'9#,"'#/'#-AB'#-+'(G9%-C'&,/E),E/+'H*-' )%&+'#>'>%*AE/+I=! 2A&#'+&,%9A*&"+C'F#/D*-.'<#*-,'F*,"'!*?(%<<"'A%&+/ H</*$%/B'A%&+/'>#/'*-%E.E/%,*#-'F%&'7C?J10'A%&+/I=! 3%/+>EA'%&&+&&$+-,'#>'/%C*%,*#-'*&&E+&=!"#$%&'()"*+,*-.+/ 01234'56'7#8+$9+/':;5; <=':; Rasmus Ischebeck: Scintillators for SwissFEL Thomas Schietinger
5 !"#$%&%'(#!)*) J++<'*,'&*$<A+'K#/',"+'0+I+/%A' 3#?-)*AA#/B'#-+'9?,,#-4',L#'&*.-%A&!(+0&$%&1"23&,'-((%&4%&5-$%#&$5& 6(+0&)"07/ CD6'<3')"%/.+! C5E;'F+G'+-+/.H! C;=6'F+G'+-+/.H'&</+%I!"#$%&'()"*+,*-.+/ Rasmus Ischebeck: Scintillators for 01234'56'7#8+$9+/':;5; <=':5 Thomas Schietinger
6 Profile Monitor for the Photocathode Laser Tb:glass scintillator Part of the photocathode laser is reflected onto the scintillator for online monitoring Imaged onto CCD detector C. Vicario 6
7 Electron Beam Profile Monitors Usage Matching to design optics Measure transverse phase space (phase space density, emittance) Overlap electron beam with seed laser / laser heater With transverse deflecting structure: measure timeresolved parameters Bunch length Slice emittance In dispersive regions Measure energy profile Project the 6-dimensional phase space on 1 or 2 dimensions Reconstruct the phase space by numerical methods
8 Electron Beam Profile Monitors Scintillators, OTR Screens & Wire Scanners Alignment hole and calibration scale Wire scanner Installed scintillators Ce:YAG 5 µm 20 µm 200 µm Fluorescent crystal (Ce:LuAG) Ce:LuAG 200 µm OTR screen (Al-coated Si wafer) RF shield High Energy Screen Low Energy Screen F. Piffaretti 8
9 Electron Beam Profile Monitors Visual Light Optics OTR screen / scintillator is at an angle of 45º to the optical axis For overview camera (1:5.3 demagnification) Use Scheimpflug criterion to correct image plane orientation Projected pixel size: 23 µm For 1:1 imaging Perspective control lens is not available commercially Only central part (~1 2 mm) of the screen can be imaged within depth of field 9
10 Measurement at 7 MeV Electron beam behind a pepper pot (for emittance measurement) 200 µm thick Ce:YAG crystal imaged 1:1 onto CCD detector 10
11 Measurement at 130 MeV 200 pc electron beam focused by quadrupole triplet onto Ce:YAG scintillator Imaged 5.3:1 onto CCD detector 11
12 Measurement at 130 MeV Comparison to beam size measurement with optical transition radiation shows good agreement down to 60 µm rms Gauss fit to beam size; error bars represent statistical variation in 5 images each µm YAG OTR 160 Beam size / µm Focusing Quadrupole Current / A 12
13 Loss Monitors Beam containment Wire scanner readout 13
14 Loss Monitors Polystyrene scintillator fiber (1 mm 1 mm 1 m) Light detected by multi-pixel photon counter Pulse height is integrated, then digitized Work in progress: Fiber has been installed Digital readout is being commissioned 14
15 Summary Profile monitors for Photocathode laser Electron beam Loss monitors 5 µm YAG OTR Beam containment Wire scanners 15
16 Outlook 10 pc operation Use low noise CMOS camera 10 µm beam sizes Construct Scheimpflug-corrected objective Microbunching instability (COTR) Use shorter wavelength Use wire scanners Real-time data processing Use FPGAs for acquisition and on-line analysis 16
17 Outlook 10 pc operation Use low noise CMOS camera 10 µm beam sizes Construct Scheimpflug-corrected objective Microbunching instability (COTR) Use shorter wavelength Use wire scanners Real-time data processing Use FPGAs for acquisition and on-line analysis 16
18 Outlook 10 pc operation Use low noise CMOS camera 10 µm beam sizes Construct Scheimpflug-corrected objective Microbunching instability (COTR) Use shorter wavelength Use wire scanners Real-time data processing Use FPGAs for acquisition and on-line analysis Y(f) Single Sided Power Spectrum of y(t) Schematic Plot Frequency (Hz) x
19 Outlook 10 pc operation Use low noise CMOS camera 10 µm beam sizes Construct Scheimpflug-corrected objective Microbunching instability (COTR) Use shorter wavelength Use wire scanners Real-time data processing Use FPGAs for acquisition and on-line analysis 16
20 Scintillators for SwissFEL Rasmus Ischebeck, for the PSI Diagnostics Group Thank you to the Diagnostics Group & the SwissFEL Team Special thanks for slides, drawings & help with this talk Markus Baldinger, Peter Heimgartner, Goran Marinkovic, Gian Luca Orlandi, Federico Piffaretti, Thomas Schietinger, Volker Schlott, Vincent Thominet, Carlo Vicario Paul Scherrer Institut Rasmus Ischebeck SwissFEL Diagnostics Layout
Transverse Coherence of a Vacuum Ultraviolet Free Electron Laser
Transverse Coherence of a Vacuum Ultraviolet Free Electron Laser Rasmus Ischebeck March 16, 2004 Transverse Coherence of a VUV Free Electron Laser Introduction Relevance of Coherence Definition and Measurements
More informationIMPROVEMENT OF SCREEN MONITOR WITH SUPPRESSION OF COHERENT-OTR FOR SACLA
IMPROVEMENT OF SCREEN MONITOR WITH SUPPRESSION OF COHERENT-OTR FOR SACLA S. Matsubara 1, H. Maesaka 1,2, S. Inoue 3, Y. Otake 1,2 1: JASRI, 2: RIKEN SPring-8 Center, 3: SPring-8 Service Co. Ltd. Outline
More informationOptimized Design of 3D Laser Triangulation Systems
The Scan Principle of 3D Laser Triangulation Triangulation Geometry Example of Setup Z Y X Target as seen from the Camera Sensor Image of Laser Line The Scan Principle of 3D Laser Triangulation Detektion
More informationDetectors for Future Light Sources. Gerhard Grübel Deutsches Elektronen Synchrotron (DESY) Notke-Str. 85, Hamburg
Detectors for Future Light Sources Gerhard Grübel Deutsches Elektronen Synchrotron (DESY) Notke-Str. 85, 22607 Hamburg Overview Radiation from X-Ray Free Electron lasers (XFEL, LCLS) Ultrafast detectors
More informationLaser readiness for all optical EUV FEL
Laser readiness for all optical EUV FEL Akira Endo EUVA (Extreme Ultraviolet Lithography System Development Association) EUVL Source Workshop 19 October, 2006 Barcelona, Spain Acknowledgments This work
More informationPeak Detector. Minimum Detectable Z Step. Dr. Josep Forest Technical Director. Copyright AQSENSE, S.L.
Peak Detector Minimum Detectable Z Step Dr. Josep Forest Technical Director Peak Detector Minimum Detectable Defect Table of Contents 1.Introduction...4 2.Layout...4 3.Results...8 4.Conclusions...9 Copyright
More informationInstallation of Optical Replica Synthesizer
FLASH Seminar 27 November 2007 Installation of Optical Replica Synthesizer G.Angelova OUTLINE How it works Where What - Undulators - Chicane -OTR - Optical Station I and II - Laser Transfer Line - Seed
More informationSCDI for EUV photomask metrology RESCAN - Reflective EUV Mask Scanning Lensless Imaging Tool
EUV Litho Workshop 2017 WIR SCHAFFEN WISSEN HEUTE FÜR MORGEN P. Helfenstein a, I. Mochi a, R. Rajendran a, S. Fernandez a, S. Yoshitake b, Y. Ekinci a a Paul Scherrer Institut, Switzerland b NuFlare Technology
More informationWAVELENGTH MANAGEMENT
BEAM DIAGNOS TICS SPECIAL PRODUCTS OEM DETECTORS THZ DETECTORS PHOTO DETECTORS HIGH POWER SOLUTIONS POWER DETECTORS ENERGY DETECTORS MONITORS Camera Accessories WAVELENGTH MANAGEMENT UV CONVERTERS UV Converters
More informationProgress of the Thomson Scattering Experiment on HSX
Progress of the Thomson Scattering Experiment on HSX K. Zhai, F.S.B. Anderson, D.T. Anderson HSX Plasma Laboratory, UW-Madison Bill Mason PSL, UW-Madison, The Thomson scattering system being constructed
More informationSynchronization and pump-probe experiments
Synchronization and pump-probe experiments by Stefan Düsterer Outline o Pump-probe probe infrastructure VUV + VUV VUV + optical o o Temporal overlap and jitter As example: the pump-probe probe chamber
More informationChapter 2: Wave Optics
Chapter : Wave Optics P-1. We can write a plane wave with the z axis taken in the direction of the wave vector k as u(,) r t Acos tkzarg( A) As c /, T 1/ and k / we can rewrite the plane wave as t z u(,)
More informationFLUOSTAR Rhodamine B- encapsulating microspheres are seeding particles optimized for Particle Image Velocimetry. Technical handbook ver.
www.ebm.vc FLUOSTAR Rhodamine B- encapsulating microspheres are seeding particles optimized for Particle Image Velocimetry Technical handbook ver.1, Feb, 2010 CONTENTS 1) Introduction of fluorescent PIV
More informationImproving the 3D Scan Precision of Laser Triangulation
Improving the 3D Scan Precision of Laser Triangulation The Principle of Laser Triangulation Triangulation Geometry Example Z Y X Image of Target Object Sensor Image of Laser Line 3D Laser Triangulation
More informationContinuation Format Page
C.1 PET with submillimeter spatial resolution Figure 2 shows two views of the high resolution PET experimental setup used to acquire preliminary data [92]. The mechanics of the proposed system are similar
More informationApplications of the IEEE-1394 CCD Camera for Beam Diagnostics in NSRRC
Applications of the IEEE-1394 CCD Camera for Beam Diagnostics in NSRRC C. J. Wang, C. H. Kuo, Teno Yang, K. H. Hu, S. Y. Hsu, Jenny Chen, and K. T. Hsu National Synchrotron Radiation Research Center, 101
More informationPhase-Contrast Imaging and Tomography at 60 kev using a Conventional X-ray Tube
Phase-Contrast Imaging and Tomography at 60 kev using a Conventional X-ray Tube T. Donath* a, F. Pfeiffer a,b, O. Bunk a, W. Groot a, M. Bednarzik a, C. Grünzweig a, E. Hempel c, S. Popescu c, M. Hoheisel
More informationPARTICLE IMAGE VELOCIMETRY (PIV) AND VOLUMETRIC VELOCIMETRY (V3V) SYSTEMS
PARTICLE IMAGE VELOCIMETRY (PIV) AND VOLUMETRIC VELOCIMETRY (V3V) SYSTEMS VERSATILE, UPGRADEABLE FLUID MECHANICS MEASUREMENT SOLUTIONS UNDERSTANDING, ACCELERATED FULL SPECTRUM OF GLOBAL VELOCITY SYSTEMS
More informationWork in Tbilisi. David Mchedlishvili (SMART EDM_lab of TSU) GGSWBS , Tbilisi. Shota Rustaveli National Science Foundation
Mitglied der Helmholtz-Gemeinschaft David Mchedlishvili (SMART EDM_lab of TSU) Work in Tbilisi GGSWBS 18 23.08.2018, Tbilisi JEDI: Charged-Particle EDM Search Main principle: Inject polarized particles
More informationNovel Magnetic Field Mapping Technology for Small and Closed Aperture Undulators
Novel Magnetic Field Mapping Technology for Small and Closed Aperture Undulators Erik Wallen and Hyun-Wook Kim 06.06.2017 Outline Introduction - Measurement systems at LBNL - Activities at LBNL - Need
More informationSimulation Study for EUDET Pixel Beam Telescope using ILC Software
Simulation Study for EUDET Pixel Beam Telescope using ILC Software Linear Collider Workshop, Hamburg, May/June 2007 Tatsiana Klimkovich DESY Tatsiana Klimkovich, Linear Collider Workshop, May/June 2007
More informationFNPL control system: an overview
FNPL control system: an overview Philippe PIOT, FNAL Overview of FNPL controls System needed to be controlled Some personal thoughts Present infrastructure at FNPL Optical room Cryogenic system Optical
More informationL. Pina, A. Fojtik, R. Havlikova, A. Jancarek, S.Palinek, M. Vrbova
L. Pina, A. Fojtik, R. Havlikova, A. Jancarek, S.Palinek, M. Vrbova Faculty of Nuclear Sciences, Czech Technical University, Brehova 7, 115 19 Prague, Czech Republic CD EXPERIMENTAL ARRANGEMENT SPECTRAL
More informationATLAS Muon Endcap Alignment
Muon Endcap Alignment Jim Bensinger Brandeis University/BMC Siena_04 May 24, 2004 Basic Concept of Endcap Muon Alignment To determine the location of the muon endcap chambers, a grid is setup with alignment
More informationFirst Operational Experience from the LHCb Silicon Tracker
First Operational Experience from the LHCb Silicon Tracker 7 th International Hiroshima Symposium on Development and Application of Semiconductor Tracking Devices The LHCb Silicon Tracker Installation
More informationDevelopment of automated ultraviolet laser beam profiling system using fluorometric technique
Development of automated ultraviolet laser beam profiling system using fluorometric technique BB Shrivastava*, NS Benerji, P Bhatnagar, HS Vora a and U Nundy Chemical and Excimer Laser Section a Laser
More informationReconstruction of the 3D charge distribution of an electron bunch using a novel variable-polarization transverse deflecting structure (TDS)
Journal of Physics: Conference Series PAPER OPEN ACCESS Reconstruction of the 3D charge distribution of an electron bunch using a novel variable-polarization transverse deflecting structure (TDS) Recent
More informationTABLE OF CONTENTS PRODUCT DESCRIPTION CINCAM CCD TECHNICAL DATA SENSOR RESPONSE DIMENSIONS CINCAM CCD LARGE FORMAT TECHNICAL DATA SENSOR RESPONSE
TABLE OF CONTENTS PRODUCT DESCRIPTION CINCAM CCD TECHNICAL DATA SENSOR RESPONSE DIMENSIONS CINCAM CCD LARGE FORMAT TECHNICAL DATA SENSOR RESPONSE DIMENSIONS CINCAM CMOS TECHNICAL DATA SENSOR RESPONSE DIMENSIONS
More informationLeica TCS STED. The Fast Track to Superresolution Technical Documentation
Leica TCS STED The Fast Track to Superresolution Technical Documentation 8 9 6 7 Inverted research microscope Leica DMI6000 CS Scan head Laser and power supply Computer table Air damped optical table 6
More informationTutorial: Instantaneous Measurement of M 2 Beam Propagation Ratio in Real-Time
Tutorial: Instantaneous Measurement of M 2 Beam Propagation Ratio in Real-Time By Allen M. Cary, Jeffrey L. Guttman, Razvan Chirita, Derrick W. Peterman, Photon Inc A new instrument design allows the M
More informationScintillators and photodetectors. 1. Generation of Optical Photons 2. Transport of Optical Photons 3. Detection of Optical Photons
Scintillators and photodetectors 1. Generation of Optical Photons 2. Transport of Optical Photons 3. Detection of Optical Photons 1) Generation of Optical Photons A) Organic (molecular) scintillators Advantages:
More informationTORCH: A large-area detector for precision time-of-flight measurements at LHCb
TORCH: A large-area detector for precision time-of-flight measurements at LHCb Neville Harnew University of Oxford ON BEHALF OF THE LHCb RICH/TORCH COLLABORATION Outline The LHCb upgrade TORCH concept
More informationWAVELENGTH MANAGEMENT
Camera Accessories WAVELENGTH MANAGEMENT UV CONVERTERS UV Converters take advantage of a phenomenon called fluorescence to extend the performance range of the Beamage beam profiling camera to ultraviolet
More informationSimulation study for the EUDET pixel beam telescope
EUDET Simulation study for the EUDET pixel beam telescope using ILC software T. Klimkovich January, 7 Abstract A pixel beam telescope which is currently under development within the EUDET collaboration
More informationThomas Cajgfinger, Eric Chabanat, Agnes Dominjon, Quang T. Doan, Cyrille Guerin, Julien Houles, Remi Barbier.
Thomas Cajgfinger, Eric Chabanat, Agnes Dominjon, Quang T. Doan, Cyrille Guerin, Julien Houles, Remi Barbier. IPNL, Université de Lyon, Université Lyon 1, CNRS/IN2P3, 4 rue E. Fermi 69622 Villeurbanne
More informationPhysics 625 Femtosecond laser Project
Physics 625 Femtosecond laser Project The purpose of this project is for each person to gain experience in designing part of a femtosecond laser system for pump-probe experiments. The system diagram is
More informationHigh Precision Optical Instrumentation for Large Structure Position Monitoring: The BCAM System Applied to the CMS Magnet
High Precision Optical Instrumentation for Large Structure Position Monitoring: The BCAM System Applied to the CMS Magnet International Workshop on Accelerator Alignment Stanford Linear Accelerator Center
More informationStatus of the TORCH time-of-flight detector
Status of the TORCH time-of-flight detector Neville Harnew University of Oxford (On behalf of the TORCH collaboration : the Universities of Bath, Bristol and Oxford, CERN, and Photek) August 7-9, 2017
More informationMEMS SENSOR FOR MEMS METROLOGY
MEMS SENSOR FOR MEMS METROLOGY IAB Presentation Byungki Kim, H Ali Razavi, F. Levent Degertekin, Thomas R. Kurfess 9/24/24 OUTLINE INTRODUCTION Motivation Contact/Noncontact measurement Optical interferometer
More informationDigital Image Processing
Digital Image Processing SPECIAL TOPICS CT IMAGES Hamid R. Rabiee Fall 2015 What is an image? 2 Are images only about visual concepts? We ve already seen that there are other kinds of image. In this lecture
More informationDiagnostic Tools for the Transverse Coherence of an X-FEL
Diagnostic Tools for the Transverse Coherence of an X-FEL Rasmus Ischebeck Diagnostic Tools for the Transverse Coherence of an X-FEL Importance of Coherence in an FEL Definition of coherence properties
More informationspecular diffuse reflection.
Lesson 8 Light and Optics The Nature of Light Properties of Light: Reflection Refraction Interference Diffraction Polarization Dispersion and Prisms Total Internal Reflection Huygens s Principle The Nature
More informationBME I5000: Biomedical Imaging
1 Lucas Parra, CCNY BME I5000: Biomedical Imaging Lecture 4 Computed Tomography Lucas C. Parra, parra@ccny.cuny.edu some slides inspired by lecture notes of Andreas H. Hilscher at Columbia University.
More informationSingle Photon Counting Module
Description Laser Components COUNT series of s has been developed to offer a unique combination of high quantum efficiency, wide dynamic range and ease of use for photon counting applications. Combining
More informationDevelopment of Ultrafast CXRS system in Heliotron J. Graduate School of Energy Science Kyoto University LU XIANGXUN 03/15/2016
1 Development of Ultrafast CXRS system in Heliotron J Graduate School of Energy Science Kyoto University LU XIANGXUN 03/15/2016 2 Outline 1. Introduction 2. Charge exchange Recombination Spectroscopy (CXRS)
More informationHigh spatial resolution measurement of volume holographic gratings
High spatial resolution measurement of volume holographic gratings Gregory J. Steckman, Frank Havermeyer Ondax, Inc., 8 E. Duarte Rd., Monrovia, CA, USA 9116 ABSTRACT The conventional approach for measuring
More informationCherenkov Radiation. Doctoral Thesis. Rok Dolenec. Supervisor: Prof. Dr. Samo Korpar
Doctoral Thesis Time-of-Flight Time-of-Flight Positron Positron Emission Emission Tomography Tomography Using Using Cherenkov Cherenkov Radiation Radiation Rok Dolenec Supervisor: Prof. Dr. Samo Korpar
More informationOptical Sectioning. Bo Huang. Pharmaceutical Chemistry
Optical Sectioning Bo Huang Pharmaceutical Chemistry Approaches to 3D imaging Physical cutting Technical difficulty Highest resolution Highest sensitivity Optical sectioning Simple sample prep. No physical
More informationTime-resolved PIV measurements with CAVILUX HF diode laser
Time-resolved PIV measurements with CAVILUX HF diode laser Author: Hannu Eloranta, Pixact Ltd 1 Introduction Particle Image Velocimetry (PIV) is a non-intrusive optical technique to measure instantaneous
More informationCinCam CCD - Technical Data -
- Technical Data - SENSOR DATA CCD-1201 CCD-1301 CCD-2301 CCD-2302 Format: 1/2 1/3 2/3 2/3 Active area: 6.5mm x 4.8mm 4.8mm x 3.6mm 9.0mm x 6.7mm 8.5mm x 7.1mm Number of pixel: 1388 x 1038 (1.4MPixel)
More informationGeneral Computing Concepts. Coding and Representation. General Computing Concepts. Computing Concepts: Review
Computing Concepts: Review Coding and Representation Computers represent all information in terms of numbers ASCII code: Decimal number 65 represents A RGB: (255,0,0) represents the intense red Computers
More informationWinCamD-LCM 1" CMOS Beam Profiling Camera, SuperSpeed USB 3.0, * nm * model-dependent
Datasheet WinCamD-LCM 1" CMOS Beam Profiling Camera, SuperSpeed USB 3.0, 190 1610* nm * model-dependent With an 11.3 x 11.3 mm active area, 4.2 Mpixels, 5.5 x 5.5 μm pixels, optical and electronic triggering
More informationSingle Photon Counting Module COUNT blue -Series
Single Photon Counting Module COUNT blue -Series Description Laser Components COUNT blue series of Single Photon Counting Modules has been developed to offer a unique combination of high quantum efficiency,
More informationDEFLECTION AND TWIST MEASUREMENT SYSTEM (DTMS) Model 47
Features DEFLECTION AND TWIST MEASUREMENT SYSTEM (DTMS) Model 47 Results are not affected by the motion or acceleration of the structure being tested Three or five degrees of freedom are measured between
More informationProduction and Quality Assurance of Detector Modules for the LHCb Silicon Tracker
Production and Quality Assurance of Detector Modules for the LHCb Silicon Tracker Olaf Steinkamp for Dmytro Volyanskyy Physik-Institut der Universität Zürich 10th ICATPP Conference on Astroparticle, Particle,
More informationVision Based Metal Spectral Analysis using
1/27 Vision Based Metal Spectral Analysis using Eranga Ukwatta Department of Electrical and Computer Engineering The University of Western Ontario May 25, 2009 2/27 Outline 1 Overview of Element Spectroscopy
More informationImprovement of Infrared Imaging Video Bolometer Systems in LHD )
Improvement of Infrared Imaging Video Bolometer Systems in LHD ) Kiyofumi MUKAI, Byron J. PETERSON, Shwetang N. PANDYA 1), Ryuichi SANO 1) and Muneji ITOMI 2) National Institute for Fusion Science, Toki
More informationMPI TS2500-RF 200 mm Fully Automated Probe System For RF Production Test Measurements
MPI TS2500-RF 200 mm Fully Automated Probe System For RF Production Test Measurements FEATURES / BENEFITS Designed for Wide Variety of RF On-Wafer Production Applications RF applications up to 67 GHz &
More informationUV-NIR LASER BEAM PROFILER
CinCam CMOS - Technical Data - CMOS-1201 CMOS-1202 CMOS-1203 CMOS-1204 Standard Series Standard Series Standard Series Standard Series SENSOR DATA Format: 1/2 1/1.8 1/1.8 1/2.5 Active area (without cover
More informationApplications of Piezo Actuators for Space Instrument Optical Alignment
Year 4 University of Birmingham Presentation Applications of Piezo Actuators for Space Instrument Optical Alignment Michelle Louise Antonik 520689 Supervisor: Prof. B. Swinyard Outline of Presentation
More informationMEASUREMENT OF SMALL TRANSVERSE BEAM SIZE USING INTERFEROMETRY
MEASUREMENT OF SMALL TRANSVERSE BEAM SIZE USING INTERFEROMETRY T. Mitsuhashi High Energy Accelerator Research Organisation, Oho, Tsukuba, Ibaraki, 35-81 Japan Abstract The principle of measurement of the
More informationDeliverable D10.2. WP10 JRA04 INDESYS Innovative solutions for nuclear physics detectors
MS116 Characterization of light production, propagation and collection for both organic and inorganic scintillators D10.2 R&D on new and existing scintillation materials: Report on the light production,
More informationSupporting information for: A highly directional room-temperature single. photon device
Supporting information for: A highly directional room-temperature single photon device Nitzan Livneh,, Moshe G. Harats,, Daniel Istrati, Hagai S. Eisenberg, and Ronen Rapaport,, Applied Physics Department,
More informationShielding factors for traditional safety glasses
Shielding factors for traditional safety glasses Malcolm McEwen, Hong Shen and Ernesto Mainegra-Hing Ionizing Radiation Standards, National Research Council Canada Alan DuSautoy, Radiation and Health Sciences
More informationFormulas of possible interest
Name: PHYS 3410/6750: Modern Optics Final Exam Thursday 15 December 2011 Prof. Bolton No books, calculators, notes, etc. Formulas of possible interest I = ɛ 0 c E 2 T = 1 2 ɛ 0cE 2 0 E γ = hν γ n = c/v
More informationAP* Optics Free Response Questions
AP* Optics Free Response Questions 1978 Q5 MIRRORS An object 6 centimeters high is placed 30 centimeters from a concave mirror of focal length 10 centimeters as shown above. (a) On the diagram above, locate
More informationMeasurements using three-dimensional product imaging
ARCHIVES of FOUNDRY ENGINEERING Published quarterly as the organ of the Foundry Commission of the Polish Academy of Sciences ISSN (1897-3310) Volume 10 Special Issue 3/2010 41 46 7/3 Measurements using
More informationASI Photoport TIRF Injector Instruction Manual
ASI Photoport TIRF Injector Instruction Manual Applied Scientific Instrumentation, Inc. 29391 W. Enid Rd. Eugene, OR 97402-9533 USA Phone: (800) 706-2284 (541) 461-8181 Fax: (541) 461-4018 Web: www.asiimaging.com
More informationNon-Contact Depth Measuring Microscope System DH2/IMH
Non-Contact Depth Measuring Microscope System DH2/IMH Specially designed focus indicator (Target Mark) facilitates focusing operation greatly. Highly accurate and repeatable measurement is possible. No
More information4.2 Megapixel Scientific CMOS Camera
CMOS, EMCCD AND CCD CAMERAS FOR LIFE SCIENCES 4.2 Megapixel Scientific CMOS Camera Photometrics Prime is the first intelligent scientific CMOS (scmos) camera to incorporate a powerful FPGA-based Embedded
More informationEUDET Telescope Geometry and Resolution Studies
EUDET EUDET Telescope Geometry and Resolution Studies A.F.Żarnecki, P.Nieżurawski February 2, 2007 Abstract Construction of EUDET pixel telescope will significantly improve the test beam infrastructure
More informationMeasurement of the beam yz crabbing tilt due to wakefields using streak camera at CESR
Journal of Physics: Conference Series PAPER OPEN ACCESS Measurement of the beam yz crabbing tilt due to wakefields using streak camera at CESR To cite this article: S T Wang and D L Rubin 018 J. Phys.:
More informationMeasurements of Three-Dimensional Velocity Fields Under Breaking Waves
The Journal of Undergraduate Research Volume 11 Journal of Undergraduate Research, Volume 11: 2013 Article 3 2013 Measurements of Three-Dimensional Velocity Fields Under Breaking Waves Matthew Auch South
More informationTechnical Specifications for High speed PIV and High speed PIV-PLIF system
Technical Specifications for High speed PIV and High speed PIV-PLIF system MODULE A. HIGH SPEED PIV (3-C) A1. Double Cavity High Speed Laser (up to 10 khz): The vendor should provide Dual Head (DH) laser
More informationInformation page for written examinations at Linköping University TER2
Information page for written examinations at Linköping University Examination date 2016-08-19 Room (1) TER2 Time 8-12 Course code Exam code Course name Exam name Department Number of questions in the examination
More informationSiPMs for Čerenkov imaging
SiPMs for Čerenkov imaging Peter Križan University of Ljubljana and J. Stefan Institute Trends in Photon Detectors in Particle Physics and Calorimetry, Trieste, June 2-4, 2008 Contents Photon detectors
More informationSpherical Crystal X-ray Imaging for MTW, OMEGA, and OMEGA EP
Spherical Crystal X-ray Imaging for MTW, OMEGA, and OMEGA EP C.STOECKL, G. FISKEL, R. K. JUNGQUIST, P. M. NILSON, AND W. THEOBALD University of Rochester, Laboratory for Laser Energetics Spherical Crystal
More informationUV-NIR LASER BEAM PROFILER
- Technical Data - CCD-1201 CCD-2301 CCD-2302 Standard Series Standard Series Standard Series SENSOR DATA Format: 1/2 2/3 2/3 Active area (without cover glass): 6.5mm x 4.8mm 9.0mm x 6.7mm 8.5mm x 7.1mm
More informationPump-probe. probe optical laser systems at FLASH. S. Düsterer
Pump-probe probe optical laser systems at FLASH S. Düsterer Outline Current status of the laser systems ( what is working) Planned upgrades till spring 2010 ( what will be working) The future. Lasers from
More informationarxiv:physics/ v1 [physics.ins-det] 18 Dec 1998
Studies of 1 µm-thick silicon strip detector with analog VLSI readout arxiv:physics/981234v1 [physics.ins-det] 18 Dec 1998 T. Hotta a,1, M. Fujiwara a, T. Kinashi b, Y. Kuno c, M. Kuss a,2, T. Matsumura
More informationCATALOGUE INFRARED VIEWERS AND CAMERAS 2017
CATALOGUE INFRARED VIEWERS AND CAMERAS 2017 Wider spectral range IR viewers and cameras Content Spectral sensitivity... 26 Power density... 26 Content... 5 Technical information... 27 What s in the box?...
More informationHARP-NEF Front End Assembly
Science Fibers HARP-NEF Front End Assembly Calib Fibers HARPN Front End Assembly ( w/ Partial Cover Plates ) HARPN Front End Assembly 1 HARP-NEF Front End Assembly Roger Eng December 6, 2007 2 HARP-NEF
More informationFEL diagnostics and control system
FEL diagnostics and control system Thomas M. Baumann WP-85, Scientific Instrument SQS Instrument Scientist Satellite meeting Soft X-ray instruments SQS and SCS Hamburg, 24.01.2017 2 Outline FEL diagnostics
More informationElectron detector(s) decision to proceed with 2 detectors
Electron detector(s) decision to proceed with 2 detectors Direct hit detector (DH1K) reciprocal space Fast application (DH80K) real space imaging Thin nonlinear DEPFETs Thin (nonlinear) Fast DEPFETs Thin
More informationPI-MAX 4: 1024i-RF. Compatible with Windows 8/7/XP, and Linux; Universal programming interfaces for easy custom programming.
The PI-MAX4: 1024i-RF from Princeton Instruments is the ultimate scientific, intensified CCD camera (ICCD) system, featuring a 1k x 1k interline CCD fiberoptically coupled to Gen III filmless intensifiers.
More informationDevelopment of EUV-Scatterometry for CD Characterization of Masks. Frank Scholze, Gerhard Ulm Physikalisch-Technische Bundesanstalt, Berlin, Germany
Development of EUV-Scatterometry for CD Characterization of Masks PB Frank Scholze, Gerhard Ulm Physikalisch-Technische Bundesanstalt, Berlin, Germany Jan Perlich, Frank-Michael Kamm, Jenspeter Rau nfineon
More informationNEW OPTICAL MEASUREMENT TECHNIQUE FOR SI WAFER SURFACE DEFECTS USING ANNULAR ILLUMINATION WITH CROSSED NICOLS
NEW OPTICAL MEASUREMENT TECHNIQUE FOR SI WAFER SURFACE DEFECTS USING ANNULAR ILLUMINATION WITH CROSSED NICOLS Satoru Takahashi 1, Takashi Miyoshi 1, Yasuhiro Takaya 1, and Takahiro Abe 2 1 Department of
More informationThe Anfatec Level AFM a short description. Atomic Force Microscopy - approved devices for affordable prices
The Anfatec Level AFM a short description Atomic Force Microscopy - approved devices for affordable prices Our system is complete for almost all typical applications. It provides all basic modes as: contact
More informationCalibration of the LIGO Interferometer Using the Recoil of Photons
Calibration of the LIGO Interferometer Using the Recoil of Photons Justice Bruursema Mentor: Daniel Sigg Motivation The Photon Calibrator has been developed to provide a physically independent means of
More informationNASA Miniature Inspection LADAR
NASA Miniature Inspection LADAR Bradley Sallee SPEC 1 SPEC s Multi-Dimensional Imaging Programs NASA HD6D NRO HD6D AFRL LGSS Army 3D Change AFRL MST Army Imaging SAL DARPA AIRSS DARPA SUAVTL NASA Inspection
More informationVariation of Refractive Index inside an Aerogel Block
Università degli Studi di Milano Bicocca Variation of Refractive Index inside an Aerogel Block Davide Perego RICH MEETING - CERN - April 21 st 2004 Introduction The Refractive Index of aerogel and its
More informationPolarization Ray Trace, Radiometric Analysis, and Calibration
Polarization Ray Trace, Radiometric Analysis, and Calibration Jesper Schou Instrument Scientist Stanford University jschou@solar.stanford.edu 650-725-9826 HMI00905 Page 1 Polarization Ray Trace Purpose
More informationLCLS Undulator Quadrupole Fiducialization Plan
LCLS-TN-07-7 LCLS Undulator Quadrupole Fiducialization Plan Zachary Wolf, Michael Levashov, Eric Lundahl, Ed Reese, Catherine LeCocq, Robert Ruland Stanford Linear Accelerator Center August 14, 2007 Abstract
More informationSCINTILLATORS-SiPM COUPLING
SCINTILLATORS-SiPM COUPLING G.FELICI LNF-INFN SCINTILLATOR ßàSIPM 1 st PROBLEM: EJ-200 peak emission spectrum do not match S18825 peak sensitivity AMPLITUDE 1.0 0.8 0.6 0.4 0.2 EJ-200 EMISSION SPECTRUM
More information4D Technology Corporation
4D Technology Corporation Dynamic Laser Interferometry for Company Profile Disk Shape Characterization DiskCon Asia-Pacific 2006 Chip Ragan chip.ragan@4dtechnology.com www.4dtechnology.com Interferometry
More informationThree-Dimensional Laser Scanner. Field Evaluation Specifications
Stanford University June 27, 2004 Stanford Linear Accelerator Center P.O. Box 20450 Stanford, California 94309, USA Three-Dimensional Laser Scanner Field Evaluation Specifications Metrology Department
More informationMicraGEM-Si A flexible process platform for complex MEMS devices
MicraGEM-Si A flexible process platform for complex MEMS devices By Dean Spicer, Jared Crawford, Collin Twanow, and Nick Wakefield Introduction MicraGEM-Si is a process platform for MEMS prototyping and
More informationpanasonic.net/id/pidsx/global CCD The sensor can be used for various applications with its binary data output with four different sensing modes.
1123 PHOTO PHOTO PARTICUR Type Edge Sensor SERIES Related Information General terms and conditions... F-3 About laser beam... P.1593~ guide... P.1021~ General precautions... P.1595 Conforming to FDA regulations
More informationSupplementary Figure 1 Optimum transmissive mask design for shaping an incident light to a desired
Supplementary Figure 1 Optimum transmissive mask design for shaping an incident light to a desired tangential form. (a) The light from the sources and scatterers in the half space (1) passes through the
More informationFast data acquisition measurement system for plasma diagnostics using GEM detectors
Fast data acquisition measurement system for plasma diagnostics using GEM detectors A. Wojenski 1a, K. Pozniak a, G. Kasprowicz a, W. Zabolotny a, A. Byszuk a, P. Zienkiewicz a, M. Chernyshova b, T. Czarski
More information