Beam/ Halo Diagnostics R. Fiorito, A. Shkvarunets, H. Zhang Institute for Research in Electronics and Applied Physics University of Maryland Presented.

Slides:



Advertisements
Similar presentations
Observation of beam halo with corona graph
Advertisements

Thomas Stalcup June 15, 2006 Laser Guidestar System Status.
1 Laser Beam Coherence Purpose: To determine the frequency separation between the axial modes of a He-Ne Laser All sources of light, including lasers,
James Welch October 30, FEL Commissioning Plans J. Welch, et. al. FEL Commissioning Plans J. Welch, et. al. Accelerator.
Electron dynamics and molecular Coulomb explosion: critical radius vs dynamic screening Kun Zhao, III Hill (University of Maryland) Session H4. Intense-Field.
Overview of ILC Plans D.Rubin April 17, D. Rubin2 ILC R&D Activities and Plans 1.Positron Source 2.Damping Ring 3.Low Emittance Transport - damping.
Tight environment high radiation area non-serviceable area passive components optics only, no active electronics transmit image through flexible fiber.
IMAGE 1 An image is a two dimensional Function f(x,y) where x and y are spatial coordinates And f at any x,y is related to the brightness at that point.
Two-dimensional and wide dynamic range profile monitor using OTR/fluorescence screens for diagnosing beam halo of intense proton beam Y. Hashimoto, T.
LEC ( 2 ) RAD 323. Reconstruction techniques dates back to (1917), when scientist (Radon) developed mathematical solutions to the problem of reconstructing.
Matching and Synchrotron Light Diagnostics F.Roncarolo, E.Bravin, S.Burger, A.Goldblatt, G.Trad.
Digital Imaging Systems –I/O. Workflow of digital imaging Two Competing imaging format for motion pictures Film vs Digital Video( TV) Presentation of.
Os, 9/16/99 MICROMACHINING AND MICROFABRICATION TECHNOLOGY FOR ADAPTIVE OPTICS Olav Solgaard Acknowledgements: P.M. Hagelin, K. Cornett, K. Li, U. Krishnamoorthy,
1 Imaging Techniques for Flow and Motion Measurement Lecture 5 Lichuan Gui University of Mississippi 2011 Imaging & Recording Techniques.
Status Report on Mk.II Pepperpot Simon Jolly Imperial College 13 th June 2007.
Beam Diagnostics Collaboration Meeting March 18 th 2015 at Australian Synchrotron Mario Ferianis – Elettra.
Image Formation Dr. Chang Shu COMP 4900C Winter 2008.
Transverse emittance Two different techniques were used to measure the transverse emittance. The multislit mask in the injector 9 MeV Quadrupole scan for.
Optical diagnostics for beam halo (I) Coronagraph (II) OTR halo monitor for J-PARC T. Mitsuhashi, KEK.
Copyright Prentice-Hall Chapter 29 Fabrication of Microelectromechanical Devices and Systems (MEMS)
05/05/2004Cyrille Thomas DIAMOND Storage Ring Optical and X-ray Diagnostics.
October 4-5, Electron Lens Beam Physics Overview Yun Luo for RHIC e-lens team October 4-5, 2010 Electron Lens.
Winni Decking XFEL Beam Collimation and Switchyard Review Introduction FEL-Beam-Dynamics Group
C. Fischer – LHC Instrumentation Review – 19-20/11/2001 Gas Monitors for Transverse Distribution Studies in the LHC LHC Instrumentation Review Workshop.
Arbitrary and Dynamic Patterning in a Programmable Array Microscope
A Transverse Profile Imager for SwissFEL Rasmus Ischebeck.
G5 Beam Instrumentation D. Gassner, E. Pozdeyev 4-09.
Current Status of Pepperpot Emittance Measurement System Simon Jolly Imperial College FETS Meeting, 22/02/06.
Use of a Digital Micromirror Array as a Configurable Mask in Optical Astronomy Shawn Gilliam Advisor: Dr. William Hetherington Research Associate: Teal.
Display Technology INFO410 & INFO350 S Jack Pinches INFORMATION
G. Ferioli, R. Jung - LHC-BI Review Workshop November 19&20 LHC Screen Profile Monitors G. Ferioli, R. Jung Introduction BTV LHC layout Monitor set-up.
October, 2009 Internal Review Beam Instrumentation David Gassner.
High Dynamic Range Beam Imaging with a Digital Optical Mask* Presented by Tim Koeth (UMD) on behalf of R.B. Fiorito, H.D. Zhang, A. Shkvarunets UMD, College.
Beam Halo Monitoring using Optical Diagnostics Hao Zhang University of Maryland/University of Liverpool/Cockcroft Institute.
NMX Instrument Layout and End-station Giuseppe Aprigliano Lead Instrument Engineer NMX IKON 7 September 15 th, 2014.
Calibration and production of PRAXIAL (*) sensors for the ATLAS muon spectrometer Optical Metrology - SPIE Optical Measurement Systems for Industrial Inspection.
Digital Cinema From Motion JPEG to Film projection A presentation by: Maxime Cassan Florent Rioult Neil Sinclair December 2008.
A Transverse Profile Imager for SwissFEL Rasmus Ischebeck
Status of the AWAKE Control System Edda Gschwendtner, Janet Schmidt, Marine Gourber-Pace, Roman Gorbonosov, Peter Sherwood AWAKE Technical Board, 27 January.
L4 BCC – 1 Sep 2011 F. Roncarolo, U. Raich L.Soby, J.Tan, C.Zamantzas, F. Lenardon, C.Vuitton, G-J.Focker.
ARIEL Building Pierre Bricault. Proton Beam specification The proton beam energy must be between 450 to 500 MeV. 200 µA with proton beam intensity losses.
Measurements of Intense Proton Beams using Optical Transition Radiation Vic Scarpine, Fermilab TIPP 2011 Chicago, IL June 10, 2011.
Adaptive Optical Masking Method and Its Application to Beam Halo Imaging Ralph Fiorito H. Zhang, A. Shkvarunets, I. Haber, S. Bernal, R. Kishek, P. O’Shea.
LARP Additions to the LHC Synchrotron-Light Monitors Alan Fisher SLAC National Accelerator Laboratory LARP CM18 Fermilab 2012 May 8.
For the FLASH Collaboration by Taiwan CosPA Members W-Y.Pauchy Hwang, Guey-Lin Lin, Ming-Heuy Huang, Chien-Wen Chen, Feng-Yin Chang, Chih-Ching Chen, Yu-Chung.
Wir schaffen Wissen – heute für morgen PSI, March 2013 Paul Scherrer Institut PSI / DESY / KIT Mini-Workshop on Longitudinal Diagnostics for FELs.
Alushta 2014 Measurement of the electron beam transverse emittance at the JINR LHEP photoinjector test bench M. Nozdrin Conference-school of Young Scientists.
Nonlinear Dynamics with Space-Charge in a Small Electron Recirculator Santiago Bernal on behalf of UMER group, IREAP, University of Maryland, College Park,
ODR Diagnostics for Hadron Colliders Tanaji Sen APC.
Beard & McLain, “Small Unmanned Aircraft,” Princeton University Press, 2012, Chapter 13: Slide 1 Chapter 13 Vision Based Guidance.
Emittance measurements for LI2FE electron beams
Options and Recommendations for TL and Dumps
AVA Liverpool Carsten Welsch.
BUNCH LENGTH MEASUREMENT SYSTEM FOR 500 KV PHOTOCATHODE DC GUN AT IHEP
Tango status at Elettra
ODR/OTR emittance station at ATF2 (KEK)
OTR based measurements for ELI-NP Gamma Beam Source
Paul Scherrer Institut
Application of a Streak camera at PITZ
MICROMACHINING AND MICROFABRICATION TECHNOLOGY FOR ADAPTIVE OPTICS
Status of Equatorial CXRS System Development
Proton Beam Diagnostics
Basic of Light & Optics
Beam size diagnostics using diffraction radiation
Injector Setup for G0 and HAPPEX & Lessons Learned
The Image The pixels in the image The mask The resulting image 255 X
Experience with photoinjector at ATF
Alignment, Scanning Malcolm Guthrie
CLIC luminosity monitoring/re-tuning using beamstrahlung ?
Automatic operation IR rework system Automatic Component placement 2 x K-type thermocouples IR-pyro sensor RPC-camera.
Presentation transcript:

Beam/ Halo Diagnostics R. Fiorito, A. Shkvarunets, H. Zhang Institute for Research in Electronics and Applied Physics University of Maryland Presented (with apologies) Michelle Shinn (JLab) 1 Goals: measure low intensity halo properties (distribution and emittance) in presence of high intensity but low emittance core Approach: use OTR or OSR and optical masking to separate out halo and core Two masking methods : I. Fixed (pinhole or stop); II. Adaptive (programable digital micromirror array)

OTR and OSR Halo Imaging Systems installed at FEL Site of OTR and OSR diagnostics experiments

Electron beam OTR Camera 2 Mask beam imaging camera OTR farfield imaging camera beam ( pinhole or stop ) (farfield OTR gives localized divergence within pinhole or outside stop) I. Fixed Optical Mask (used with OTR station at FEL beam dump) polarizer

II. Adaptive masking using digital micro-mirror array* *DLP TM 1100 Texas Instruments Inc micromirror size:  m x  m No of elements: 1024 X 768 pixels Array switching rate: 9600 patterns / sec PC interface: USB 2.0 micromirror Rotation axis

DMA Imaging System Developed at UMD/ UMER 180 Frames 32 mm 900 Frames 32 mm 5

Halo measurements at UMER (7 mA beam) using DMA Screen boundary

Dynamic Range Test of DMD with intense UMER beam and circular mask Integration Frames: 7 32mm

Dynamic Range Measurement using Circular Mask and intense 23 mA beam: DR ~10(5) mm 8 Reconstructed beam profile

1000 mm 500 mm OSR Port (2F06) Gallery optics: top view 1219 mm 457 mm DMA Camera 24 o Optics for DMA Halo Experiment using OSR (Installed at FEL 8/2010 ) Vault Optics: side view 5 m PVC tube FEL Vault ceiling Gallery optics: side view