A Beam Halo Monitor Based on Adaptive Optics. Courtesy of Dr Carsten P. Welsch AB/BI/PM
|
|
- Virginia Parks
- 8 years ago
- Views:
Transcription
1 A Beam Halo Monitor Based on Adaptive Optics Courtesy of Dr Carsten P. Welsch AB/BI/PM
2 Outline 1. Beam Halo Measurements Whydowecare? How to do the measurement? Introduction to CID technology 2. Core-masking Technique The idea Initial tests fixed mask DLP Technology (MMA) Results from Tests
3 Definition: What is 'Halo'? General definition difficult to make: Accelerator physicists Instrumentation specialists Low density / difficult to measure
4 Halo: Why do we care? Less transmission, more radiation Ati Activation of vacuum chamber Maintenance more difficult Higher cost Different reasons Dispersion Mismatch Scattering (beam - gas, intra-beam, Touschek) Noise Space charge... Goal: Understand mechanisms!
5 OTR characteristics Created when charged particles pass through the interface between two materials with different permittivity. OTR Backward emission (θ) (φ) Specular reflection
6 A Brief (incomplete) Comparison OTR SR + + Screen choice Non-destructive Linear, directive Signal Highly directive Fast time response Good signal if E~150 MeV Add. Info (ε, x, y,..) Destructive Installation/Maintenance Max. beam charge Only in bends or chicane Alignment of line Diffraction limited
7 Halo Monitor Under investigation: 2D PMT setup SpectraCAM CID camera Micro Mirror Array Meas. Sci. Technol. 17 (2006)
8 Non-destructive read-out Row Column Steps: Determine sense voltage ΔV Transfer charges to RE Continue integration or Inject charges to substrate Substrate
9 Halo Measurements Meas. Sci. Technol. 17 (2006)
10 SOHO * Solar and Heliospheric Observatory
11 Lab Setup optical system 2 mask (image plane 1) filter wheel Mask: spot printed on polyesther foil CCD camera (image plane 2) optical system 1 On / Off (beam core) OTR light Proc. EPAC04
12 Calibration: Opacity Phantom image without mask Phantom image with mask am mplitude [a.u ] amplitude with mask amplitude without mask Proc. EPAC04 horizontal position [mm] Factor 100 higher dynamic range.
13 Micro Mirror Array Micro Electro-Mechanical device 1024 x 768 pixels (XGA) USB Interface high-speed port 120 MHz for data transfer up to full array mirror patterns / sec (7.6 Gbs) 16 μm insize +/- 10 of rotation Switch of 15 μs physically, 2 μs optically
14 Performance Test and More Camera Filter Wheel Light source MMA
15 Measurement (1) Aquire profile (2) Define core (4) Re-Measure (3) Generate mask
16 Results from Measurements 1,0E+00 Position [μm] Normalized I ntensity 1,0E-01 1,0E-02 1,0E-03 1,0E-04 Masked region SpectraCAM 600s DMD CCD Camera, OD4 10E-05 1,0E 05 1,0E-06
17 Next Steps Test MMA setup in running machine Improve Software / automate process Adapt to new Test Beam Line Combine with CID camera?
18 Conclusion Understanding of beam halo of central importance for future accelerators CID camera provided high-dynamic range measurements to 10 6 level MMA as central element of future halo monitor
19 A i t Thanks to Patrick Amiot, Cathelijne Bal, Enrico Bravin, Stephane Burger, Christian Dutriat, Morad Hamani, Phillippe Lavanchy, Thibaut Lefèvre, Romain Ruffieux, ErminioRugo, Guy Yvon, Patrick Amiot, Cathelijne Bal, Enrico Bravin, Stephane Burger, Christian Dutriat, Morad Hamani, Phillippe Lavanchy, Thibaut Lefèvre, Romain Ruffieux, ErminioRugo, Guy Yvon, Patrick Amiot, Cathelijne Bal, Enrico Bravin, Stephane Burger, Christian Dutriat, Morad Hamani, Phillippe Lavanchy, Thibaut Lefèvre, Romain Ruffieux, ErminioRugo, Guy Yvon, Patrick Amiot, Cathelijne Bal, Enrico Bravin, Stephane Burger,, Christian Dutriat, Morad Hamani, Phillippe Lavanchy, Thibaut Lefèvre, Romain Ruffieux, ErminioRugo, Guy Yvon, Patrick Amiot, Cathelijne Bal, Enrico Bravin, Stephane Burger,, Christian L h Dutriat, Morad Hamani, Phillippe Lavanchy, Thibaut Lefèvre, Romain Ruffieux, ErminioRugo, Guy Yvon, Patrick Amiot, Cathelijne Bal, Enrico Bravin, Stephane Burger,, Christian Dutriat, Morad Hamani, Phillippe Lavanchy, Thibaut Lefèvre, Romain Ruffieux, ErminioRugo, Guy Yvon, Patrick Amiot, Cathelijne Bal, Enrico Bravin, Stephane Burger,Christian Dutriat, Morad Hamani, Phillippe Lavanchy, Thibaut Lefèvre, Romain Ruffieux, ErminioRugo, Guy Yvon, Patrick Amiot, Cathelijne Bal, Enrico Bravin, Stephane Burger,, Christian Dutriat, Morad Hamani, Phillippe Lavanchy, Thibaut Lefèvre, Romain Ruffieux, ErminioRugo, Guy Yvon, Patrick Amiot, Cathelijne Bal, Enrico Bravin, Stephane Burger,, Christian Dutriat, Morad Hamani, Phillippe Lavanchy, Thibaut Lefèvre, Romain Ruffieux, ErminioRugo, Guy Yvon, Patrick Amiot, Cathelijne Bal, Enrico Bravin, Stephane Burger,, Christian Dutriat, Morad Hamani, Phillippe Lavanchy, Thibaut Lefèvre, Romain Ruffieux, ErminioRugo, Guy Yvon, Patrick Amiot, Cathelijne Bal, Enrico Bravin, Stephane Burger,, Christian Dutriat, Morad Hamani, Phillippe Lavanchy, Thibaut Lefèvre, Romain Ruffieux, Erminio Rugo, Guy Yvon, Patrick Amiot, Cathelijne Bal, Enrico Bravin, Stephane Burger,, Christian Dutriat, Morad Hamani, Phillippe Lavanchy, Thibaut Lefèvre, Romain Ruffieux, ErminioRugo, Guy Yvon, Patrick Amiot, Cathelijne Bal, Enrico Bravin, Stephane Burger, Christian Dutriat, Morad Hamani, Phillippe Lavanchy, Thibaut Lefèvre, Romain Ruffieux, ErminioRugo, Guy Yvon, Patrick Amiot, Cathelijne Bal, Enrico Bravin, Stephane Burger,, Christian Dutriat, Morad Hamani, Phillippe Lavanchy, Thibaut Lefèvre, Romain Ruffieux, ErminioRugo, Guy Yvon, Patrick Amiot, Cathelijne Bal, Enrico Bravin, Stephane Burger,, Christian Dutriat, Morad Hamani, Phillippe Lavanchy, Thibaut Lefèvre, Romain Ruffieux, ErminioRugo, Guy Yvon, Patrick Amiot, Cathelijne Bal, Enrico Bravin, Stephane Burger,, Christian Dutriat, Morad Hamani, Phillippe Lavanchy, Thibaut Lefèvre, Romain Ruffieux, ErminioRugo, Guy Yvon, Patrick Amiot, Cathelijne Bal, Enrico Bravin, Stephane Burger,, Christian Dutriat, Morad Hamani, Phillippe Lavanchy, Thibaut Lefèvre, Romain Ruffieux, ErminioRugo, Guy Yvon, Patrick Amiot, Cathelijne Bal, Enrico Bravin, Stephane Burger, Christian Dutriat, Morad Hamani, Phillippe Lavanchy, Thibaut Lefèvre, Romain Ruffieux, ErminioRugo, Guy Yvon, Patrick Amiot, Cathelijne Bal, Enrico Bravin, Stephane Burger,, Christian Dutriat, Morad Hamani, Phillippe Lavanchy, Thibaut Lefèvre, Romain Ruffieux, ErminioRugo, Guy Yvon, Patrick Amiot, Cathelijne Bal, Enrico Bravin, Stephane Burger,, Christian Dutriat, Morad Hamani, Phillippe Lavanchy, Thibaut Lefèvre, Romain Ruffieux, ErminioRugo, Guy Yvon, Patrick Amiot, Cathelijne Bal, Enrico Bravin, Stephane Burger,, Christian Dutriat, Morad Hamani, Phillippe Lavanchy, Thibaut Lefèvre, Romain Ruffieux, ErminioRugo, Guy Yvon, Patrick Amiot, Cathelijne Bal, Enrico Bravin, Stephane Burger,Christian Dutriat, Morad Hamani, Phillippe Lavanchy, Thibaut Lefèvre, Romain Ruffieux, ErminioRugo, Guy Yvon, Patrick Amiot, Cathelijne Bal, Enrico Bravin, Stephane Burger,, Christian Dutriat, Morad Hamani, Phillippe Lavanchy, Thibaut Lefèvre, Romain Ruffieux, ErminioRugo, Guy Yvon, Patrick Amiot, Cathelijne Bal, Enrico Bravin, Stephane Burger,, Christian Dutriat, Morad Hamani, Phillippe Lavanchy, Thibaut Lefèvre, Romain Ruffieux, ErminioRugo, Guy Yvon, Patrick Amiot, Cathelijne Bal, Enrico Bravin, Stephane Burger, Christian Dutriat, Morad Hamani, Phillippe Lavanchy, Thibaut Lefèvre, Romain Ruffieux, ErminioRugo, Guy Yvon, Patrick Amiot, Cathelijne Bal, Enrico Bravin, Stephane Burger, Christian Dutriat, Morad Hamani, Phillippe Lavanchy, Thibaut Lefèvre, Romain Ruffieux, ErminioRugo, Guy Yvon, Patrick Amiot, Cathelijne Bal, Enrico Bravin, Stephane Burger,, Christian Dutriat, Morad Hamani, Phillippe Lavanchy, Thibaut Lefèvre, Romain Ruffieux, ErminioRugo, Guy Yvon, Patrick
20 F D F D F D F D F D F D F D F D F D CLIC 07 CTF3 - Overview Thermionic gun Linac DL CR 2007 D F D D F D D F D D F D F D F F D D F D F D F D F D F D F Photo injector / laser tests from GHz production (PETS line) and test stand CLEX building in 2006 TL Beam up to here
21 CID Technology
22 Non-destructive read-out COLUMN (SENSE) ROW (DRIVE) COLUMN (SENSE) ROW (DRIVE) V INJECT V INTEGRATE V INTEGRATE 1 V INJECT V INJECT V INTEGRATE V INJECT V INTEGRATE Integrate photo-electrons. 2 1 st Sense voltage sample. Original bias conditions restored. Continue integration. COLUMN (SENSE) ROW (DRIVE) COLUMN (SENSE) ROW (DRIVE) V INJECT INTEGRATE V V INJECT V INTEGRATE 4 V INJECT V INTEGRATE V INJECT V INTEGRATE 3 Photon-generated charge injected to substrate. Alternatively, ti l perform selective pixel injection. 2 nd Sense voltage sample. Voltage difference between 2 nd sample and 1 st sample proportional to photongenerated charge.
Cathode Ray Tube. Introduction. Functional principle
Introduction The Cathode Ray Tube or Braun s Tube was invented by the German physicist Karl Ferdinand Braun in 897 and is today used in computer monitors, TV sets and oscilloscope tubes. The path of the
More informationTowards large dynamic range beam diagnostics and beam dynamics studies. Pavel Evtushenko
Towards large dynamic range beam diagnostics and beam dynamics studies Pavel Evtushenko Motivation Linacs with average current 1-2 ma and energy 1-2.5 GeV are envisioned as drivers for next generation
More informationShort overview of TEUFEL-project
Short overview of TEUFEL-project ELAN-meeting may 2004 Frascati (I) Contents Overview of TEUFEL project at Twente Photo cathode research Recent experience Outlook Overview FEL Drive laser Photo cathode
More informationSynthetic Sensing: Proximity / Distance Sensors
Synthetic Sensing: Proximity / Distance Sensors MediaRobotics Lab, February 2010 Proximity detection is dependent on the object of interest. One size does not fit all For non-contact distance measurement,
More informationAdvanced variance reduction techniques applied to Monte Carlo simulation of linacs
MAESTRO Advanced variance reduction techniques applied to Monte Carlo simulation of linacs Llorenç Brualla, Francesc Salvat, Eric Franchisseur, Salvador García-Pareja, Antonio Lallena Institut Gustave
More informationGamma-ray Large Area Space Telescope (GLAST) Large Area Telescope (LAT) Calorimeter AFEE Board Parts Radiation Test Plan
GLAST LAT DESIGN DESCRIPTION Document Title AFEE Board Parts Radiation Test Plan Document # Date Effective LAT-SS-01890-01 1 April 2003 Prepared by(s) Supersedes James Ampe None Subsystem/Office Calorimeter
More informationEfficiency, Dispersion and Straylight Performance Tests of Immersed Gratings for High Resolution Spectroscopy in the Near Infra-red
Changing the economics of space Efficiency, Dispersion and Straylight Performance Tests of Immersed Gratings for High Resolution Spectroscopy in the Near Infra-red J. Fernandez-Saldivar 1, F. Culfaz 1,
More informationCoating Thickness and Composition Analysis by Micro-EDXRF
Application Note: XRF Coating Thickness and Composition Analysis by Micro-EDXRF www.edax.com Coating Thickness and Composition Analysis by Micro-EDXRF Introduction: The use of coatings in the modern manufacturing
More information& Tunnel Cross Section
CLIC workshop Working group: Two beam hardware and Integration ti CLIC Civil Engineering Layouts & Tunnel Cross Section John Osborne TS-CE Acknowledgements : C.Wyss, J-L Baldy, N.Baddams 17 October 2007
More informationMicro-CT for SEM Non-destructive Measurement and Volume Visualization of Specimens Internal Microstructure in SEM Micro-CT Innovation with Integrity
Micro-CT for SEM Non-destructive Measurement and Volume Visualization of Specimens Internal Microstructure in SEM Innovation with Integrity Micro-CT 3D Microscopy Using Micro-CT for SEM Micro-CT for SEM
More informationData-analysis scheme and infrastructure at the X-ray free electron laser facility, SACLA
Data-analysis scheme and infrastructure at the X-ray free electron laser facility, SACLA T. Sugimoto, T. Abe, Y. Joti, T. Kameshima, K. Okada, M. Yamaga, R. Tanaka (Japan Synchrotron Radiation Research
More informationPHOTOELECTRIC EFFECT AND DUAL NATURE OF MATTER AND RADIATIONS
PHOTOELECTRIC EFFECT AND DUAL NATURE OF MATTER AND RADIATIONS 1. Photons 2. Photoelectric Effect 3. Experimental Set-up to study Photoelectric Effect 4. Effect of Intensity, Frequency, Potential on P.E.
More informationView of ΣIGMA TM (Ref. 1)
Overview of the FESEM system 1. Electron optical column 2. Specimen chamber 3. EDS detector [Electron Dispersive Spectroscopy] 4. Monitors 5. BSD (Back scatter detector) 6. Personal Computer 7. ON/STANDBY/OFF
More informationInformation about the T9 beam line and experimental facilities
Information about the T9 beam line and experimental facilities The incoming proton beam from the PS accelerator impinges on the North target and thus produces the particles for the T9 beam line. The collisions
More informationsource at CERN G.McMonagle AB/RF
12 GHz Stand alone power source at CERN G.McMonagle AB/RF Objectives Install a 12GHz power source at CERN as soon as possible to allow high gradient structure testing independent from the CTF3 machine
More informationHIGH CURRENT OPERATION OF THE ACSI TR30 CYCLOTRON
HIGH CURRENT OPERATION OF THE ACSI TR30 CYCLOTRON 18 th International Conference on Cyclotrons and their Applications, Sicily, 2007 Vasile Sabaiduc, Project Manager, RF Senior Engineer Advanced Cyclotron
More informationproduct overview pco.edge family the most versatile scmos camera portfolio on the market pioneer in scmos image sensor technology
product overview family the most versatile scmos camera portfolio on the market pioneer in scmos image sensor technology scmos knowledge base scmos General Information PCO scmos cameras are a breakthrough
More informationLaboratory #3 Guide: Optical and Electrical Properties of Transparent Conductors -- September 23, 2014
Laboratory #3 Guide: Optical and Electrical Properties of Transparent Conductors -- September 23, 2014 Introduction Following our previous lab exercises, you now have the skills and understanding to control
More informationMANUAL FOR RX700 LR and NR
MANUAL FOR RX700 LR and NR 2013, November 11 Revision/ updates Date, updates, and person Revision 1.2 03-12-2013, By Patrick M Affected pages, ETC ALL Content Revision/ updates... 1 Preface... 2 Technical
More informationTom Wilson Product Marketing Manager Delivery Systems Varian Medical Systems International AG. CERN Accelerator School, May 2015
INDUSTRIAL DESIGN Tom Wilson Product Marketing Manager Delivery Systems Varian Medical Systems International AG VARIAN ONCOLOGY SYSTEMS 1 VARIAN ONCOLOGY SYSTEMS CERN Accelerator, May 2015 Industrial Design
More informationIntroduction to CCDs and CCD Data Calibration
Introduction to CCDs and CCD Data Calibration Dr. William Welsh San Diego State University CCD: charge coupled devices integrated circuit silicon chips that can record optical (and X-ray) light pixel =
More informationChapter 3 SYSTEM SCANNING HARDWARE OVERVIEW
Qiang Lu Chapter 3. System Scanning Hardware Overview 79 Chapter 3 SYSTEM SCANNING HARDWARE OVERVIEW Since all the image data need in this research were collected from the highly modified AS&E 101ZZ system,
More informationNetwork Design. Yiannos Mylonas
Network Design Yiannos Mylonas Physical Topologies There are two parts to the topology definition: the physical topology, which is the actual layout of the wire (media), and the logical topology, which
More informationINTRODUCTION. A. Purpose
New York State Department of Health Bureau of Environmental Radiation Protection Guide for Radiation Safety/Quality Assurance Programs Computed Radiography INTRODUCTION A. Purpose This guide describes
More informationZEISS Axiocam 506 color Your Microscope Camera for Imaging of Large Sample Areas Fast, in True Color, and High Resolution
Product Information Version 1.0 ZEISS Axiocam 506 color Your Microscope Camera for Imaging of Large Sample Areas Fast, in True Color, and High Resolution ZEISS Axiocam 506 color Sensor Model Sensor Pixel
More informationFLS 2010 Storage Ring Working Group Session 4: Future ring technology and design issues
FLS 2010 Storage Ring Working Group Session 4: Future ring technology and design issues 10:45 11:10 Limits to achievable stability Glenn Decker, APS 11:10 11:35 Stability and alignment of NSLS II magnet
More informationFig.1. The DAWN spacecraft
Introduction Optical calibration of the DAWN framing cameras G. Abraham,G. Kovacs, B. Nagy Department of Mechatronics, Optics and Engineering Informatics Budapest University of Technology and Economics
More informationCyclotron Centre in Poland and 2D thermoluminescence dosimetry
Cyclotron Centre in Poland and 2D thermoluminescence dosimetry Jan Gajewski Institute of Nuclear Physics, Kraków, Poland Department of Radiation Dosimetry Nuclear Physics Institute Academy of Science of
More informationA Guide to Acousto-Optic Modulators
A Guide to Acousto-Optic Modulators D. J. McCarron December 7, 2007 1 Introduction Acousto-optic modulators (AOMs) are useful devices which allow the frequency, intensity and direction of a laser beam
More informationInterference. Physics 102 Workshop #3. General Instructions
Interference Physics 102 Workshop #3 Name: Lab Partner(s): Instructor: Time of Workshop: General Instructions Workshop exercises are to be carried out in groups of three. One report per group is due by
More informationA Polarimetry concept for the EDM experiment at COSY
A Polarimetry concept for the EDM experiment at COSY Paul Maanen JEDI Collaboration Physics Institute III B, RWTH Aachen University DPG Frühjahrstagung March 27, 2015 Outline Introduction Detector concept
More informationName: Due: September 21 st 2012. Physics 7230 Laboratory 3: High Resolution SEM Imaging
Name: Due: September 21 st 2012 Physics 7230 Laboratory 3: High Resolution SEM Imaging 1. What is meant by the term resolution? How does this differ from other image variables, such as signal to noise
More informationThe Basics of Scanning Electron Microscopy
The Basics of Scanning Electron Microscopy The small scanning electron microscope is easy to use because almost every variable is pre-set: the acceleration voltage is always 15kV, it has only a single
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 informationHow To Use Laboca
Laboca in a nutshell Total power Bolometer Array operating at 850 µm 295 pixels Field of view 11 Science: cold dust nearby and far Bolometer Principle Neutron-Transmutation-Doped (NTD) Germanium 0.25mm
More informationCLIC accelerator and detector
CLIC accelerator and detector CLIC/CTF3 accelerator R&D CLIC detector study http://cern.ch/clic-study http://lcd.web.cern.ch/lcd/ Many thanks to Anne Dabrowski, Jean-Pierre Delahaye, Frank Tecker and others
More informationDigital vs. Analogue Control Systems
Digital vs. Analogue Control Systems Presented at the 2011 Annual Meeting of the American College of Medical Physics, Chattanooga, TN, May 1, 2011 Ivan A. Brezovich, PhD, Dept. of Rad Onc, Univ of Alabama
More informationIndirect X-ray photon counting image sensor with 27T pixels and 15 electrons RMS accurate threshold
Indirect X-ray photon counting image sensor with 27T pixels and 15 electrons RMS accurate threshold B. Dierickx 1,2, B. Dupont 1,3, A. Defernez 1, N. Ahmed 1 1 Caeleste, Antwerp, Belgium 2 Vrije Universiteit
More informationColor holographic 3D display unit with aperture field division
Color holographic 3D display unit with aperture field division Weronika Zaperty, Tomasz Kozacki, Malgorzata Kujawinska, Grzegorz Finke Photonics Engineering Division, Faculty of Mechatronics Warsaw University
More informationHigh speed infrared camera for contactless temperature measurement on rotating tires
DIAS Infrared GmbH Publications No. 9 1 High speed infrared camera for contactless temperature measurement on rotating tires Helmut Budzier, Dresden University of Technology, Institute for Solid-State
More information11th International Computational Accelerator Physics Conference (ICAP) August 19 24, 2012, Rostock-Warnemünde (Germany)
Numerical Modeling of RF Electron Sources for FEL-Accelerators Erion Gjonaj Computational Electromagetics Laboratory (TEMF), Technische Universität Darmstadt, Germany 11th International Computational Accelerator
More informationSolid State Devices 4B6
Solid State Devices 4B6 Lecture 13 Projection and 3D displays: LCD, DLP and LCOS Daping Chu Lent 2015 (LCD) A 105 inch TFT-LCD 4k2k curved panel by Samsung January 2014 A 105 inch OLED 3k2k curved panel
More informationStatus of the FERMI@Elettra Free Electron Laser
Status of the FERMI@Elettra Free Electron Laser E. Allaria on behalf of the FERMI team Work partially supported by the Italian Ministry of University and Research under grants FIRB-RBAP045JF2 and FIRB-RBAP06AWK3
More informationAxioCam MR The All-round Camera for Biology, Medicine and Materials Analysis Digital Documentation in Microscopy
Microscopy from Carl Zeiss AxioCam MR The All-round Camera for Biology, Medicine and Materials Analysis Digital Documentation in Microscopy New Dimensions in Performance AxioCam MR from Carl Zeiss Both
More informationSingle photon detection with H8500 MAPMTs for the CBM RICH detector*
Single photon detection with H8500 MAPMTs for the CBM RICH detector* Christian Pauly for the CBM collaboration Introduction The CBM experiment The CBM RICH detector Single Photon detection with H8500 MAPMTs
More informationInstitute of Accelerator Technologies of Ankara University and TARLA Facility
Institute of Accelerator Technologies of Ankara University and TARLA Facility Avni Aksoy Ankara University avniaksoy@ankara.edu.tr On behalf of IAT & TARLA Team Contents Brief history of TAC project Institute
More informationOptical Fibres. Introduction. Safety precautions. For your safety. For the safety of the apparatus
Please do not remove this manual from from the lab. It is available at www.cm.ph.bham.ac.uk/y2lab Optics Introduction Optical fibres are widely used for transmitting data at high speeds. In this experiment,
More informationPowder diffraction and synchrotron radiation
Powder diffraction and synchrotron radiation Gilberto Artioli Dip. Geoscienze UNIPD CIRCe Center for Cement Materials single xl diffraction powder diffraction Ideal powder Powder averaging Textured sample
More informationProper Implementation of Industrial CT Scanning to Reduce Inspection Costs & Get to Production Faster. Jesse Garant, JG&A Metrology Center
Proper Implementation of Industrial CT Scanning to Reduce Inspection Costs & Get to Production Faster Jesse Garant, JG&A Metrology Center Traditional Metrology and Inspection Tactile Devices (Touch Probe)
More informationX- and Gamma Ray Imaging Systems based on CdTe-CMOS Detector Technology
X- and Gamma Ray Imaging Systems based on dte-mos Detector Technology Konstantinos Spartiotis, Ray Durrant, nssi Leppänen, Henrik Lohman, Olli Männistö, Tuomas Pantsar, Jouni Pyyhtiä, Tom Schulman, Oy
More informationFiber optic communication
Fiber optic communication Fiber optic communication Outline Introduction Properties of single- and multi-mode fiber Optical fiber manufacture Optical network concepts Robert R. McLeod, University of Colorado
More informationIEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 52, NO. 5, OCTOBER 2005 1. A. Warner, G. Kazakevich, S. Nagaitsev, G. Tassotto, W. Gai, and R.
TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 52, NO. 5, OCTOBER 2005 1 Beam Profile Diagnostics for the Fermilab Medium Energy Electron Cooler A. Warner, G. Kazakevich, S. Nagaitsev, G. Tassotto, W. Gai, and
More informationAutomation System TROVIS 6400 TROVIS 6493 Compact Controller
Automation System TROVIS 6400 TROVIS 6493 Compact Controller For panel mounting (front frame 48 x 96 mm/1.89 x 3.78 inch) Application Digital controller to automate industrial and process plants for general
More informationLBS-300 Beam Sampler for C-mount Cameras. YAG Focal Spot Analysis Adapter. User Notes
LBS-300 Beam Sampler for C-mount Cameras P/N SP90183, SP90184, SP90185 and SP90186 YAG Focal Spot Analysis Adapter P/N SP90187, SP90188, SP90189, SP90190, SP90191 User Notes Ophir-Spiricon Inc. 60 West
More informationIMPROVED CCD DETECTORS FOR HIGH SPEED, CHARGE EXCHANGE SPECTROSCOPY STUDIES ON THE DIII D TOKAMAK
IMPROVED CCD DETECTORS FOR HIGH SPEED, CHARGE EXCHANGE SPECTROSCOPY STUDIES ON THE TOKAMAK by K.H. Burrell P. Gohil, R.J. Groebner, D.H. Kaplan, D.G. Nilson,* J.I. Robinson, and D.M. Thomas General Atomics,
More informationStudy of electron cloud at MI and slip stacking process simulation
Study of electron cloud at MI and slip stacking process simulation Alexandr S. Valkovich Purpose 1.Understand the slip stacking process which happens in the Main Injector. 2. Calculation of bunch distortion
More informationUsers Manual Model #93711. English
Users Manual Model #93711 English Congratulations on your purchase of the Celestron NexImage 5 Solar System imaging camera. Your NexImage camera comes with the following: + NexImage 5 Camera + 1.25 nose
More informationIntegrated Photonic. Electronic. Optics. Optoelettronics. Integrated Photonic - G. Breglio L1. Quantum Mechanics Materials Science Nano/Bio-photonic
Integrated Photonic Quantum Mechanics Materials Science Nano/Bio-photonic Optoelettronics Optics Electronic Applications of Optoelectronic Systems Solar cells OLED display LED Laser diodes Flexible OLED
More informationSpecifications Summary. Active pixels 2048 x 2048. Pixel size (W x H) 13.5 x 13.5 µm. Active area pixel well depth (typical) 100,000 e -
High Energy Detection XD Powder diffraction image courtesy of NASA AMES, USA Features and Benefits Open front end 1 6 CF152 flange and knife-edge sealing provided as standard for direct interfacing to
More informationFully Automated Imaging Spectrometer User Manual
Fully Automated Imaging Spectrometer User Manual Part Number 81092 Revision 2 Copyright February, 06 HORIBA Jobin Yvon Inc., Optical Spectroscopy Division. All rights reserved. Portions of the software
More informationPoS(PhotoDet 2012)068
Characterization of the Hamamatsu R11265 multi-anode photomultiplier tube with single photon signals Luca CADAMURO, Marta CALVI, Andrea GIACHERO,, Matteo MAINO, Clara MATTEUZZI, Gianluigi PESSINA Dipartimento
More informationModule 13 : Measurements on Fiber Optic Systems
Module 13 : Measurements on Fiber Optic Systems Lecture : Measurements on Fiber Optic Systems Objectives In this lecture you will learn the following Measurements on Fiber Optic Systems Attenuation (Loss)
More informationProjects and R&D activities
Projects and R&D activities J.M. Jimenez On behalf of the Vacuum, Surface and Coatings Group (VSC) Vacuum, Surface and Coatings group* Mandate Design, construction, operation, maintenance and upgrade of
More informationCONCEPT OF DETERMINISTIC ION IMPLANTATION AT THE NANOSCALE
CONCEPT OF DETERMINISTIC ION IMPLANTATION AT THE NANOSCALE Daniel Spemann Jan Meijer 1, Jürgen W. Gerlach, Paul Räcke 1, Susann Liedtke, Stephan Rauschenbach 2, Bernd Rauschenbach 1 University of Leipzig,
More informationOptical coherence tomography as a tool for non destructive quality control of multi-layered foils
Optical coherence tomography as a tool for non destructive quality control of multi-layered foils Günther Hannesschläger, Alexandra Nemeth, Christian Hofer, Christian Goetzloff, Jens Reussner, Karin Wiesauer,
More informationWorld-first Proton Pencil Beam Scanning System with FDA Clearance
Hitachi Review Vol. 58 (29), No.5 225 World-first Proton Pencil Beam Scanning System with FDA Clearance Completion of Proton Therapy System for MDACC Koji Matsuda Hiroyuki Itami Daishun Chiba Kazuyoshi
More informationHow To Use A Ds340 (Dsp)
Ideal for monitoring dust levels in the exhaust gas of industrial combustion or air filtration processes. Innovative Dynamic Detection Principle (DDP) measurement technique Immune to gradual reductions
More informationVeraview IC5 HD High definition, digital imaging excellence. Thinking ahead. Focused on life.
Veraview IC5 HD High definition, digital imaging excellence Thinking ahead. Focused on life. Thinking ahead. Focused on life. 2 3 IC5 HD Super High-Speed with High Definition Clarity For dental radiology
More informationInfrared Viewers. Manual
Infrared Viewers Manual Contents Introduction 3 How it works 3 IR viewer in comparison with a CCD camera 4 Visualization of infrared laser beam in mid-air 4 Power Density 5 Spectral sensitivity 6 Operation
More informationHow To Use A Sound Card With A Subsonic Sound Card
!"## $#!%!"# &"#' ( "#' )*! #+ #,# "##!$ -+./0 1" 1! 2"# # -&1!"#" (2345-&1 #$6.7 -&89$## ' 6! #* #!"#" +" 1##6$ "#+# #-& :1# # $ #$#;1)+#1#+
More informationFundamentals of Cone-Beam CT Imaging
Fundamentals of Cone-Beam CT Imaging Marc Kachelrieß German Cancer Research Center (DKFZ) Heidelberg, Germany www.dkfz.de Learning Objectives To understand the principles of volumetric image formation
More informationWe bring quality to light. MAS 40 Mini-Array Spectrometer. light measurement
MAS 40 Mini-Array Spectrometer light measurement Features at a glance Cost-effective and robust CCD spectrometer technology Standard USB interface Compatible with all Instrument Systems measuring adapters
More informationRecent Measurements and Plans for the SLAC Compton X- Ray Source
SLAC-PUB-11689 Recent Measurements and Plans for the SLAC Compton X- Ray Source A.E. Vlieks*, R. Akre*, G. Caryotakis*, C. DeStefano #, W.J. Frederick #, J.P. Heritage #, N.C. Luhmann Jr. #, D. Martin*,
More informationLesson 10:DESIGN PROCESS EXAMPLES Automatic Chocolate vending machine, smart card and digital camera
Lesson 10:DESIGN PROCESS EXAMPLES Automatic Chocolate vending machine, smart card and digital camera 1 Automatic Chocolate Vending Machine (ACVM) 2 Diagrammatic representation of ACVM Keypad for user Interface
More informationNano Meter Stepping Drive of Surface Acoustic Wave Motor
Proc. of 1st IEEE Conf. on Nanotechnology, Oct. 28-3, pp. 495-5, (21) Maui, Hawaii Nano Meter Stepping Drive of Surface Acoustic Wave Motor Takashi Shigematsu*, Minoru Kuribayashi Kurosawa*, and Katsuhiko
More informationFast Varifocal Lenses Based on KTa 1-x Nb x O 3 (KTN) Single Crystals
: Crystal Technologies Fast Varifocal Lenses Based on KTa 1-x Nb x O 3 () Single Crystals Tadayuki Imai, Shogo Yagi, Seiji Toyoda, and Masahiro Sasaura Abstract NTT Photonics Laboratories has recently
More informationSTUDY OF THE TRANSVERSE BEAM EMITTANCE OF THE BERN MEDICAL CYCLOTRON
Proceedings of IBIC15, Melbourne, Australia - Pre-Release Snapshot 17-Sep-15 1:3 MOPB41 STUDY OF THE TRANSVERSE BEAM EMITTANCE OF THE BERN MEDICAL CYCLOTRON K. P. Nesteruka,, M. Augera, S. Braccinia, T.
More informationHigh Resolution Spatial Electroluminescence Imaging of Photovoltaic Modules
High Resolution Spatial Electroluminescence Imaging of Photovoltaic Modules Abstract J.L. Crozier, E.E. van Dyk, F.J. Vorster Nelson Mandela Metropolitan University Electroluminescence (EL) is a useful
More informationID Objective Requirements Description of Test Date & Examiner 15 Verify that the optics?? OMC
NAOMI OMC/NCU Acceptance Tests at the University of Durham ATC Document number AOW/GEN/RAH/15.0/06/00 OMC/NCU acceptance tests DRAFT (Version date: 2 nd June 2000) wht-naomi-44 The ID numbers are those
More informationThe accurate calibration of all detectors is crucial for the subsequent data
Chapter 4 Calibration The accurate calibration of all detectors is crucial for the subsequent data analysis. The stability of the gain and offset for energy and time calibration of all detectors involved
More informationCHAPTER 3: DIGITAL IMAGING IN DIAGNOSTIC RADIOLOGY. 3.1 Basic Concepts of Digital Imaging
Physics of Medical X-Ray Imaging (1) Chapter 3 CHAPTER 3: DIGITAL IMAGING IN DIAGNOSTIC RADIOLOGY 3.1 Basic Concepts of Digital Imaging Unlike conventional radiography that generates images on film through
More informationIntroduction to acoustic imaging
Introduction to acoustic imaging Contents 1 Propagation of acoustic waves 3 1.1 Wave types.......................................... 3 1.2 Mathematical formulation.................................. 4 1.3
More informationTSL213 64 1 INTEGRATED OPTO SENSOR
TSL 64 INTEGRATED OPTO SENSOR SOES009A D4059, NOVEMBER 99 REVISED AUGUST 99 Contains 64-Bit Static Shift Register Contains Analog Buffer With Sample and Hold for Analog Output Over Full Clock Period Single-Supply
More informationCalorimetry in particle physics experiments
Calorimetry in particle physics experiments Unit n. 8 Calibration techniques Roberta Arcidiacono Lecture overview Introduction Hardware Calibration Test Beam Calibration In-situ Calibration (EM calorimeters)
More informationThe Focused Ion Beam Scanning Electron Microscope: A tool for sample preparation, two and three dimensional imaging. Jacob R.
The Focused Ion Beam Scanning Electron Microscope: A tool for sample preparation, two and three dimensional imaging Jacob R. Bowen Contents Components of a FIB-SEM Ion interactions Deposition & patterns
More informationScripps Proton Therapy Center: Configuration and Implementation
Scripps Proton Therapy Center: Configuration and Implementation Anthony Mascia Proton Symposium 2013 Annual AAPM Meeting Indianapolis, Indiana USA Facility Configuration Scripps Proton Therapy Center ***All
More informationEncoders for Linear Motors in the Electronics Industry
Technical Information Encoders for Linear Motors in the Electronics Industry The semiconductor industry and automation technology increasingly require more precise and faster machines in order to satisfy
More informationDamping Wigglers in PETRA III
Damping Wigglers in PETRA III WIGGLE2005, Frascati 21-22.2.2005 Winni Decking, DESY-MPY Introduction Damping Wiggler Parameters Nonlinear Dynamics with DW Operational Aspects Summary DESY and its Accelerators
More informationAn Overview of Digital Imaging Systems for Radiography and Fluoroscopy
An Overview of Digital Imaging Systems for Radiography and Fluoroscopy Michael Yester, Ph.D. University of Alabama at Birmingham Outline Introduction Imaging Considerations Receptor Properties General
More informationAN1200.04. Application Note: FCC Regulations for ISM Band Devices: 902-928 MHz. FCC Regulations for ISM Band Devices: 902-928 MHz
AN1200.04 Application Note: FCC Regulations for ISM Band Devices: Copyright Semtech 2006 1 of 15 www.semtech.com 1 Table of Contents 1 Table of Contents...2 1.1 Index of Figures...2 1.2 Index of Tables...2
More informationPerformance of the Vidar Red LED Dosimetry Pro Advantage : A scanner optimized for use with GAFCHROMIC EBT Dosimetry Film.
INTERNATIONAL SPECIALTY PRODUCTS 1361 Alps Road Wayne NJ 07470 Tel: 973-628-4000 Performance of the Vidar Red LED Dosimetry Pro Advantage : A scanner optimized for use with GAFCHROMIC EBT Dosimetry Film.
More informationHow To Make A Plasma Control System
XXII. Erfahrungsaustausch Mühlleiten 2015 Plasmaanalyse und Prozessoptimierung mittels spektroskopischem Plasmamonitoring in industriellen Anwendungen Swen Marke,, Lichtenau Thomas Schütte, Plasus GmbH,
More informationResults from first tests of TRD prototypes for CBM. DPG Frühjahrstagung Münster 2011 Pascal Dillenseger Institut für Kernphysik Frankfurt am Main
Results from first tests of TRD prototypes for CBM DPG Frühjahrstagung Münster 2011 Pascal Dillenseger Institut für Kernphysik Contents Overview of the CBM experiment CBM-TRD General TRD requirements The
More informationResults: Low current (2 10 12 ) Worst case: 800 MHz, 12 50 GeV, 4 turns Energy oscillation amplitude 154 MeV, where
Status Focus has shifted to a neutrino factory Two comprehensive designs of acceleration (liancs, arcs) Jefferson Lab, for Fermilab Study CERN (Keil et al.) Jefferson Lab study Low (2 10 12 ) charge per
More informationFundamentals of modern UV-visible spectroscopy. Presentation Materials
Fundamentals of modern UV-visible spectroscopy Presentation Materials The Electromagnetic Spectrum E = hν ν = c / λ 1 Electronic Transitions in Formaldehyde 2 Electronic Transitions and Spectra of Atoms
More informationPUMPED Nd:YAG LASER. Last Revision: August 21, 2007
PUMPED Nd:YAG LASER Last Revision: August 21, 2007 QUESTION TO BE INVESTIGATED: How can an efficient atomic transition laser be constructed and characterized? INTRODUCTION: This lab exercise will allow
More informationT(CR)3IC Testbed for Coherent Radio Cherenkov Radiation from Cosmic-Ray Induced Cascades
T(CR)3IC Testbed for Coherent Radio Cherenkov Radiation from Cosmic-Ray Induced Cascades R. Milinčić1, P. Gorham1, C. Hebert1, S. Matsuno1, P. Miočinović1, M. Rosen1, D. Saltzberg2, G. Varner1 1 University
More informationAcousto-optic modulator
1 of 3 Acousto-optic modulator F An acousto-optic modulator (AOM), also called a Bragg cell, uses the acousto-optic effect to diffract and shift the frequency of light using sound waves (usually at radio-frequency).
More informationRevision 1.10 April 7, 2015 Method of Implementation (MOI) for 100BASE-TX Ethernet Cable Tests Using Keysight E5071C ENA Option TDR
Revision 1.10 April 7, 2015 Method of Implementation (MOI) for 100BASE-TX Ethernet Cable Tests Using Keysight E5071C ENA Option TDR 1 Table of Contents 1. Revision History... 3 2. Purpose... 3 3. References...
More informationTOSHIBA CCD Image Sensor CCD (charge coupled device) TCD2955D
Preliminary TOSHIBA CCD Image Sensor CCD (charge coupled device) TCD2955D The TCD2955D is a high sensitive and low dark current 4240 elements 6 line CCD color image sensor which includes CCD drive circuit
More information