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.

Slides:



Advertisements
Similar presentations
Erdem Oz* USC E-164X,E167 Collaboration Plasma Dark Current in Self-Ionized Plasma Wake Field Accelerators
Advertisements

Kevin Kelly Mentor: Peter Revesz.  Importance of Project: Beam stability is crucial in CHESS, down to micron-level precision  The beam position is measured.
Parameters to choose the CCD The CCD test bench *Temperature range : -55 to +40°C. *Stabilization : < 0.05°C/hour. *5 temperature probes : CCD and electronics.
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,
The Origins of X-Rays. The X-Ray Spectrum The X-Ray Spectrum (Changes in Voltage) The characteristic lines are a result of electrons ejecting orbital.
Two-dimensional and wide dynamic range profile monitor using OTR/fluorescence screens for diagnosing beam halo of intense proton beam Y. Hashimoto, T.
October 1 -10, 2014JEM-EUSO Workshop - Toulouse1 Balloon – EUSO Xenon / UV LED Flasher Calibration Evgeny Kuznetsov for UAH / MSFC GLS team University.
CCD testing Enver Alagoz 12 April CCD testing goals CCD testing is to learn how to – do dark noise characterization – do gain measurements – determine.
UVP BioImaging Systems Solutions for the Science of Life Digital CCD Cameras 101.
Overview of Scientific Imaging using CCD Arrays Jaal Ghandhi Mechanical Engineering Univ. of Wisconsin-Madison.
Performances of a pixel ionization chamber to monitor a voxel scan hadron beam A.Boriano 3, F.Bourhaleb 2,3, R. Cirio 3, M. Donetti 2,3, F. Marchetto 3,
Matching and Synchrotron Light Diagnostics F.Roncarolo, E.Bravin, S.Burger, A.Goldblatt, G.Trad.
Laser news AWAKE performance meeting Overview There was a meeting on with the supplier of the laser system (AMPLITUDE) No new information.
A. Homs, BLISS Day Out – 15 Jan 2007 CCD detectors: spying with the Espia D. Fernandez A. Homs M. Perez C. Guilloud M. Papillon V. Rey V. A. Sole.
Test of Silicon Photomultipliers (SiPM) at Liquid Nitrogen Temperature Yura Efremenko, Vince Cianciolo nEDM CalTech Meeting 02/14/2007.
Setup of Gain Monitoring System with Mr. Uozumi Kobe Univ. Hiroko Ikeda 18,May 2007.
9/25/031 First Tests of an Optical Transition Radiation Detector for High-Intensity Proton Beams at FNAL September 25, 2003 Vic Scarpine.
SBIG ST-7XME CCD Presentation by Keith Rickard. And now for something completely different… What colour is a rainbow? It’s red!
PITZ – Introduction to the Video System Stefan Weiße DESY Zeuthen June 10, 2003.
Performances of the COROT CCDs for high accuracy photometry Pernelle Bernardi and the CCD team From Meudon : Tristan Buey, Vincent Lapeyrere, Régis Schmidt,
Eusoballoon optics test Baptiste Mot, Gilles Roudil, Camille Catalano, Peter von Ballmoos Test configuration Calibration of the light beam Exploration.
Observation of Bioluminescence in ANTARES J. Brunner.
Development of a high-speed single photon pixellated detector for visible wavelengths Introduction A photon incident on the photocathode produces a photoelectron.
Wireless Security System Group #14 Yuncheng Wang Chris Overcash John Petty Chun Hong Lin.
Developments of Photon Beam Monitors in NSRRC (TLS) J.R. Chen, C.K. Kuan, T.C. Tseng, and G.Y. Hsiung National Synchrotron Radiation Research Center XBPM.
Development of a Gamma-Ray Beam Profile Monitor for the High-Intensity Gamma-Ray Source Thomas Regier, Department of Physics and Engineering Physics University.
G5 Beam Instrumentation D. Gassner, E. Pozdeyev 4-09.
Laser beam diagnostics : BEAMDIAG program. Stéphan Del Burgo CERN PS/LP 30 January 1998 DBS 01/
Matching monitors for SPS and LHC E. Bravin 31 March 2011.
PCAL Strips light transmission properties April 25, 2011April 26, 20111April 27,
Beam/ Halo Diagnostics R. Fiorito, A. Shkvarunets, H. Zhang Institute for Research in Electronics and Applied Physics University of Maryland Presented.
Gain stability and the LYSO beam radiation monitor measurements
NON-INTERCEPTING DIAGNOSTIC FOR HIGH BRIGHTNESS ELECTRON BEAMS USING OPTICAL DIFFRACTION RADIATION INTERFERENCE (ODRI) A. Cianchi #1,2, M. Castellano 3,
Calibration and production of PRAXIAL (*) sensors for the ATLAS muon spectrometer Optical Metrology - SPIE Optical Measurement Systems for Industrial Inspection.
Time and amplitude calibration of the Baikal-GVD neutrino telescope Vladimir Aynutdinov, Bair Shaybonov for Baikal collaboration S Vladimir Aynutdinov,
Bubble Chamber Radiator Thermal Analysis 5.0 MeV, 9.5 MeV Beam Energy Fredrik Fors Mechanical Engineering 8/20/2015.
Preliminary Profile Reconstruction of EA Hybrid Showers Bruce Dawson & Luis Prado Jr thanks to Brian Fick & Paul Sommers and Stefano Argiro & Andrea de.
Electron Spectrometer: Status July 14 Simon Jolly, Lawrence Deacon 1 st July 2014.
1 PP Minimum Bias Triggering Simulations Alan Dion Stony Brook University.
Compressor Helium filled optional equivalent plane imaging laser beam dump hole in mirror for e-beam SSA and more.
Measurements of Intense Proton Beams using Optical Transition Radiation Vic Scarpine, Fermilab TIPP 2011 Chicago, IL June 10, 2011.
Beam Profile Monitor for Spot-Scanning System Yoshimasa YUASA.
Elena Rocco Nikhef, The Netherlands On behalf of the ALICE Utrecht-Nikhef group Jamboree – Utrecht December 2012.
Bioanalytik detect and identify Over 25 years experience in Imaging Benefits of NightOWL.
Four OTRs for ATF2 OTR History Current OTR setup New OTR design.
Solid-state Laser Crystal and Device Laboratory Yen-Yin Li Speaker : Yen-Yin Li Adviser : Sheng-Lung Huang Topic Report Graduate Institute of Photonics.
Date of download: 9/19/2016 Copyright © 2016 SPIE. All rights reserved. (a) A pulsatile flow bioreactor for in vitro incubation of bioengineered carotid.
Bioanalytik detect and identify Over 25 years experience in Imaging Benefits of NightOWL.
Activities and Results from PNPI GATCHINA
Analysis of LumiCal data from the 2010 testbeam
Fabio, Francesco, Francesco and Nicola INFN and University Bari
A 3D design model of the apparatus for the Laser Wakefield Acceleration of electrons at ELI-NP S. Balascuta1 , R. Dinca1 1) “Horia Hulubei” National.
E. Ponce2-1, G. Garipov2, B. Khrenov2, P. Klimov2, H. Salazar1
Experimental Demonstration of High-Order
Marcin Chrząszcz Cracow University of Technology Itamar Levy
Start Detector for pion experiments
Four OTR Tasks.
Summary of experience with Tevatron synchrotron light diagnostics
CLAS12 software workshop
LumiCal mechanical design, integration with LDC and laser alignment
The Pixel Hybrid Photon Detectors of the LHCb RICH
Proton Beam Diagnostics
Basic of Light & Optics
Beam Test Results for the CMS Forward Pixel Detector
A # Gasket spacing between flanges are not included in dimensions.
The LHCb Front-end Electronics System Status and Future Development
Diagnostics overview Beam profile monitors Cherenkov radiators Summary
Computed Tomography (C.T)
Volume 98, Issue 9, Pages (May 2010)
Experience with photoinjector at ATF
Presentation transcript:

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 Chen, Staff Member :Maggie Wang The Design of Beam Profile Monitor and the test at SRRC Chien-Wen Chen

PC2 WINDOWS XP (LAPTOP) CAMERA PC1 WINDOWS XP (WORKSTATION) SLAC TRIGGER SYSTEM TUNNELCONTROL ROOM LAN CAMERA CONTROL, IMAGE DOWNLOAD, DATA ANALYSE MONITORING, REMOTE CONTROL TRANSFER DATA OF & POSITION TITANIUM FOIL DESIGN OF BEAM PROFILE MONITOR ELECTRON BEAM

total 64cm object distance 35cm 29cm Trigger circuit tube lens CCDIEEE 1394 titanic foil beam pipe six way cube beam axis

16cm

7cm (inner) 8cm (outer) screw holes 1.3cm

2 ft optical table Cable tray/Wall 6 inch beam pipe e- 25 inches (wall-to-wall) ~ 63.5 cm OTR “cube” 28 inches (wall-to-beam-axis) Top view – not to scale Beam line flange.

Pixels1360x 1036 Well size10000 e Pixel size4.65x 4.65 Digital output 8/12 Bit Readout noise 9 e Dark current1.3/pix/s Cooling25C below ambient Integration time Ambient operating temperature 0 to 35C

ROI Full Frame Spot 3x3 binning

OTR efficiency transmission efficiency quantum efficiency pixels readout noise dark current distribution# of electrons OTR efficiency and angular distribution of a single electron for a metal foil:

The Algorithm Integrating over one axis 200

centerσ 10^ ^ In SLAC 30GeV 10^8 e/bunch Maximum intensity can be analysed :1.05x10^9 e/bunch Signals per Pixel Plotted by Feng-Yin pixel photoelectron

maxσ 10^ ^ In SLAC 30GeV 10^8 e/bunch Signal (Integrating over One Axis) photoelectron pixel

maxσ 10^795 10^ photoelectron pixel Center(93) In SLAC 30GeV 10^8 e/bunch Signal to Noise Ratio per Pixel

centerσ 10^ ^ In SLAC 30GeV 10^8 e/bunch photoelectron pixel Signal to Noise Ratio (Integrating over One Axis)

triggerexposurereadoutdownload the image analysetransfer download the analysed data 360GB / 80KB = 4.5x10^6 (events)

BPM

aluminum coating mirror beam pipe stainless window

Data captured in SRRC Signals = photoelectrons σ x = 1.22 mm 1.5 GeV photoelectron pixel

Theoretical calculation in SRRC 1.5 GeV e/bunch Total photoelectrons = photoelectron pixel σ x = 1.22 mm

Experimental : photoelectrons Theoretical : photoelectrons photoelectron (one metal surface) (two metal surface) / = Factors which may had made the difference: twice OTR, instability of the current, interference of the twice OTR.

Conclusions 1.We have captured and downloaded the image of OTR at SRRC. 2.The S/N ratio seems to be big enough, so that we may sacrifice some of it to increase the MAX intensity of events which can be analysed. 3. The code to analyse and transfer data is yet to be accomplished.