A Transverse Profile Imager for SwissFEL Rasmus Ischebeck

Size: px
Start display at page:

Download "A Transverse Profile Imager for SwissFEL Rasmus Ischebeck"

Transcription

1 P AUL SCHERRER INSTITUT observer 12 1 scnitillating crystal s virtual image Emittance [nm] 8 6 d 4 2 primary beam t [ps] A Transverse Profile Imager for SwissFEL

2 Transverse Profile Monitors University of Illinois 2

3 Profile Measurement in FELs 3.5 x y / mm x / mm 3

4 Profile Measurement in FELs 3.5 x y / mm x / mm 3

5 x-y Correlations > Intrinsic correlation y / mm x / mm.8 1 > Explicit x-y dependency introduced by RF deflector 4

6 2-Dimensional Profile Monitors > Optical transition radiation (OTR) > Scintillation 5

7 Imaging Scintillators a) b) c) d) e)

8 Electron Beam Profile Monitors Scintillators, OTR Screens & Wire Scanners Alignment hole and calibration scale Wire scanner Installed scintillators Ce:YAG 5 µm 2 µm 2 µm Fluorescent crystal (Ce:LuAG) Ce:LuAG 2 µm OTR screen (Al-coated Si wafer) RF shield High Energy Screen Low Energy Screen F. Piffaretti

9 Electron Beam Profile Monitors Scintillators, OTR Screens & Wire Scanners Alignment hole and calibration scale Wire scanner Installed scintillators Ce:YAG 5 µm 2 µm 2 µm Fluorescent crystal (Ce:LuAG) Ce:LuAG 2 µm OTR screen (Al-coated Si wafer) RF shield High Energy Screen Low Energy Screen F. Piffaretti

10 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

11 Scheimpflug Snell Screen Monitor > Theodor Scheimpflug ( ) > Willebrord Snellius ( ) 9

12 Imaging Scintillating Crystals observer s scnitillating crystal virtual image d primary beam 1

13 Imaging Scintillating Crystals s C B scnitillating crystal l d A primary beam 11

14 Imaging Scintillating Crystals observer s scnitillating crystal virtual image d primary beam 12

15 Imaging Scintillating Crystals ideal observation angle scintillating crystal virtual image aligned with beam axis d primary beam 13

16 Trigonometry 14

17 Observed Beam Size 4 35 apparent transverse size s / µm observation angle β / degrees 15

18 Ideal Observation Angle a) b) 16

19 Screen Monitor 17

20 Measurements with the Prototype > Emittance Measurement normalized xp x normalized x x 1 5 normalized yp x normalized y x sigma x [mm].15.1 sigma y [mm] measurement index measurement index Pull x 2 Pull y 5 The smallest beam in this measurement is 5 µm rms. Beams of 1 µm rms have been measured measurement index measurement index 18

21 Measurements with the Prototype > Slice emittance measurement of a 1 pc beam 12 1 Emittance [nm] t [ps] Eduard Prat, Marta Divall 19

22 Measurements with the Prototype > Slice emittance measurement of a 1.3 pc beam 3 Core slice emittance / nm Charge / pc Eduard Prat, Marta Divall 2

23 Thank You to > Hansueli for the technical design > The AMI team for manufacturing the components > Markus for the assembly > Markus, Albert & the Vacuum group for installation > Eduard the emittance measurement software, and for using the new profile monitor extensively for emittance measurements > Gian Luca, Marta, Simona, Carlo, Thomas & Eduard for the measurements presented in this talk > Vincent for the slide on the Schwarzschild imaging > Andrea for support with patenting the design, and with connections to industry > Helge for camera server software, and Babak for synchronized data acquisition > The entire Commissioning and Operations crew 21

A Transverse Profile Imager for SwissFEL Rasmus Ischebeck

A Transverse Profile Imager for SwissFEL Rasmus Ischebeck PAUL SCHERRER INSTITUT observer s virtual image d scnitillating crystal primary beam A Transverse Profile Imager for SwissFEL A Transverse Profile Imager for SwissFEL > Profile measurement in FELs observer

More information

Beam Diagnostics and Instrumentation JUAS, Archamps Peter Forck Gesellschaft für Schwerionenforschnung (GSI)

Beam Diagnostics and Instrumentation JUAS, Archamps Peter Forck Gesellschaft für Schwerionenforschnung (GSI) Beam Diagnostics and Instrumentation JUAS, Archamps Peter Forck Gesellschaft für Schwerionenforschnung (GSI), 2003, A dedicated proton accelerator for 1p-physics at the future GSI Demands facilities for

More information

Microbunching Workshop 2010 March 24, 2010, Frascati, Italy. Zhirong Huang

Microbunching Workshop 2010 March 24, 2010, Frascati, Italy. Zhirong Huang Measurements of the LCLS Laser Heater and its impact on the LCLS FEL Performance Z. Huang for the LCLS commissioning team LCLS 1 1 Outline Introduction LCLS setup and measurements Effects on FEL performance

More information

Femto-second FEL Generation with Very Low Charge at LCLS

Femto-second FEL Generation with Very Low Charge at LCLS Femto-second FEL Generation with Very Low Charge at LCLS Yuantao Ding, For the LCLS commissioning team X-ray Science at the Femtosecond to Attosecond Frontier workshop May 18-20, 2009, UCLA SLAC-PUB-13525;

More information

Diagnostic Systems for High Brightness Electron Injectors

Diagnostic Systems for High Brightness Electron Injectors Diagnostic Systems for High Brightness Electron Injectors Henrik Loos 48 th ICFA Advanced Beam Dynamics Workshop on Future Light Sources SLAC 2010 1 1 Henrik Loos LCLS Injector Injector Diagnostics Characterize

More information

Operational Performance of LCLS Beam Instrumentation. Henrik Loos, SLAC BIW 2010, Santa Fe, NM

Operational Performance of LCLS Beam Instrumentation. Henrik Loos, SLAC BIW 2010, Santa Fe, NM Editor's Note: PDF version of slides from Beam Instrumentation Workshop 21, Santa Fe, NM Operational Performance of LCLS Beam Instrumentation Henrik Loos, SLAC BIW 21, Santa Fe, NM BIW 21 1 1 Henrik Loos

More information

SwissFEL Diagnostics Layout

SwissFEL Diagnostics Layout Wir schaffen Wissen heute für morgen Paul Scherrer Institut Rasmus Ischebeck SwissFEL Diagnostics Layout PSI,May 02, 2010 P AUL SCHERRER INSTITUT SwissFEL Diagnostics Layout Rasmus Ischebeck Diagnostics

More information

Time resolved transverse and longitudinal phase space measurements at the high brightness photo injector PITZ

Time resolved transverse and longitudinal phase space measurements at the high brightness photo injector PITZ Time resolved transverse and longitudinal phase space measurements at the high brightness photo injector PITZ 1. Motivation 2. Transverse deflecting structure 3. Longitudinal phase space tomography 4.

More information

Low slice emittance preservation during bunch compression

Low slice emittance preservation during bunch compression Low slice emittance preservation during bunch compression S. Bettoni M. Aiba, B. Beutner, M. Pedrozzi, E. Prat, S. Reiche, T. Schietinger Outline. Introduction. Experimental studies a. Measurement procedure

More information

Diagnostic Systems for Characterizing Electron Sources at the Photo Injector Test Facility at DESY, Zeuthen site

Diagnostic Systems for Characterizing Electron Sources at the Photo Injector Test Facility at DESY, Zeuthen site 1 Diagnostic Systems for Characterizing Electron Sources at the Photo Injector Test Facility at DESY, Zeuthen site Sakhorn Rimjaem (on behalf of the PITZ team) Motivation Photo Injector Test Facility at

More information

II) Experimental Design

II) 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 information

Low energy high brilliance beam characterization

Low energy high brilliance beam characterization Low energy high brilliance beam characterization J. Bähr, DESY, Zeuthen, Germany Abstract Low energy high brilliance beam characterization plays an important role for electron sources and injectors of

More information

Compressor and Chicane Radiation Studies at the ATF. Gerard Andonian, UCLA High Power Workshop January 14-16, 2009 UCLA

Compressor and Chicane Radiation Studies at the ATF. Gerard Andonian, UCLA High Power Workshop January 14-16, 2009 UCLA Compressor and Chicane Radiation Studies at the ATF Gerard Andonian, UCLA High Power Workshop January 14-16, 2009 UCLA Collaboration UCLA PBPL G. Andonian, A. Cook, M. Dunning, E. Hemsing, A. Murokh, S.

More information

Generation and characterization of ultra-short electron and x-ray x pulses

Generation and characterization of ultra-short electron and x-ray x pulses Generation and characterization of ultra-short electron and x-ray x pulses Zhirong Huang (SLAC) Compact XFEL workshop July 19-20, 2010, Shanghai, China Ultra-bright Promise of XFELs Ultra-fast LCLS Methods

More information

Start-to-End Simulations

Start-to-End Simulations AKBP 9.3 Case Study for 100 µm SASE FEL Based on PITZ Accelerator for Pump-Probe Experiment at the European XFEL Start-to-End Simulations Outline Introduction Beam Optimization Beam Transport Simulation

More information

Layout of the HHG seeding experiment at FLASH

Layout 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 information

H. Maesaka*, H. Ego, T. Hara, A. Higashiya, S. Inoue, S. Matsubara, T. Ohshima, K. Tamasaku, H. Tanaka, T. Tanikawa, T. Togashi, K. Togawa, H.

H. Maesaka*, H. Ego, T. Hara, A. Higashiya, S. Inoue, S. Matsubara, T. Ohshima, K. Tamasaku, H. Tanaka, T. Tanikawa, T. Togashi, K. Togawa, H. H. Maesaka*, H. Ego, T. Hara, A. Higashiya, S. Inoue, S. Matsubara, T. Ohshima, K. Tamasaku, H. Tanaka, T. Tanikawa, T. Togashi, K. Togawa, H. Tomizawa, M. Yabashi, K. Yanagida, T. Shintake and Y. Otake

More information

Injector Experimental Progress

Injector Experimental Progress Injector Experimental Progress LCLS TAC Meeting December 10-11 2001 John Schmerge for the GTF Team GTF Group John Schmerge Paul Bolton Steve Gierman Cecile Limborg Brendan Murphy Dave Dowell Leader Laser

More information

Hiromitsu TOMIZAWA XFEL Division /SPring-8

Hiromitsu TOMIZAWA XFEL Division /SPring-8 TUPLB10 (Poster: TUPB080) Non-destructive Real-time Monitor to measure 3D- Bunch Charge Distribution with Arrival Timing to maximize 3D-overlapping for HHG-seeded EUV-FEL Hiromitsu TOMIZAWA XFEL Division

More information

Short Pulse, Low charge Operation of the LCLS. Josef Frisch for the LCLS Commissioning Team

Short Pulse, Low charge Operation of the LCLS. Josef Frisch for the LCLS Commissioning Team Short Pulse, Low charge Operation of the LCLS Josef Frisch for the LCLS Commissioning Team 1 Normal LCLS Parameters First Lasing in April 10, 2009 Beam to AMO experiment August 18 2009. Expect first user

More information

Investigations on the electron bunch distribution in the longitudinal phase space at a laser driven RF-electron source for the European X-FEL

Investigations on the electron bunch distribution in the longitudinal phase space at a laser driven RF-electron source for the European X-FEL Juliane Rönsch Universität Hamburg / DESY Investigations on the electron bunch distribution in the longitudinal phase space at a laser driven RF-electron source for the European X-FEL 5/27/2009 1 Contents

More information

SRF GUN CHARACTERIZATION - PHASE SPACE AND DARK CURRENT MEASUREMENTS AT ELBE*

SRF GUN CHARACTERIZATION - PHASE SPACE AND DARK CURRENT MEASUREMENTS AT ELBE* SRF GUN CHARACTERIZATION - PHASE SPACE AND DARK CURRENT MEASUREMENTS AT ELBE* E. Panofski #, A. Jankowiak, T. Kamps, Helmholtz-Zentrum Berlin, Berlin, Germany P.N. Lu, J. Teichert, Helmholtz-Zentrum Dresden-Rossendorf,

More information

THERMAL EMITTANCE MEASUREMENTS AT THE SwissFEL INJECTOR TEST FACILITY

THERMAL EMITTANCE MEASUREMENTS AT THE SwissFEL INJECTOR TEST FACILITY THERMAL EMITTANCE MEASUREMENTS AT THE SwissFEL INJECTOR TEST FACILITY E. Prat, S. Bettoni, H. H. Braun, M. C. Divall, R. Ganter, T. Schietinger, A. Trisorio, C. Vicario PSI, Villigen, Switzerland C. P.

More information

FURTHER UNDERSTANDING THE LCLS INJECTOR EMITTANCE*

FURTHER UNDERSTANDING THE LCLS INJECTOR EMITTANCE* Proceedings of FEL014, Basel, Switzerland FURTHER UNDERSTANDING THE LCLS INJECTOR EMITTANCE* F. Zhou, K. Bane, Y. Ding, Z. Huang, and H. Loos, SLAC, Menlo Park, CA 9405, USA Abstract Coherent optical transition

More information

Simulations of the IR/THz source at PITZ (SASE FEL and CTR)

Simulations of the IR/THz source at PITZ (SASE FEL and CTR) Simulations of the IR/THz source at PITZ (SASE FEL and CTR) Introduction Outline Simulations of SASE FEL Simulations of CTR Summary Issues for Discussion Mini-Workshop on THz Option at PITZ DESY, Zeuthen

More information

PRELIMINARY TEST OF A LUMINESCENCE PROFILE MONITOR IN THE CERN SPS

PRELIMINARY TEST OF A LUMINESCENCE PROFILE MONITOR IN THE CERN SPS PRELIMINARY TEST OF A LUMINESCENCE PROFILE MONITOR IN THE CERN SPS J. Camas, R. J. Colchester, G. Ferioli, R. Jung, J. Koopman CERN, Geneva, Switzerland Abstract In order to satisfy the tight emittance

More information

Motivation of emission studies at PITZ

Motivation of emission studies at PITZ Motivation of emission studies at PITZ PITZ activities to understand the discrepancies between measurements and simulations in: Transverse phase space Optimum machine parameters Auxiliary measurements

More information

Eric R. Colby* SLAC National Accelerator Laboratory

Eric R. Colby* SLAC National Accelerator Laboratory Eric R. Colby* SLAC National Accelerator Laboratory *ecolby@slac.stanford.edu Work supported by DOE contracts DE AC03 76SF00515 and DE FG03 97ER41043 III. Overview of the Technology Likely Performance

More information

EXPERIMENTAL STUDIES WITH SPATIAL GAUSSIAN-CUT LASER FOR THE LCLS PHOTOCATHODE GUN*

EXPERIMENTAL STUDIES WITH SPATIAL GAUSSIAN-CUT LASER FOR THE LCLS PHOTOCATHODE GUN* SLAC-PUB-14571 EXPERIMETAL STUDIES WITH SPATIAL GAUSSIA-CUT LASER FOR THE LCLS PHOTOCATHODE GU* F. Zhou +, A. Brachmann, P. Emma, S. Gilevich, and Z. Huang SLAC ational Accelerator Laboratory, 575 Sand

More information

Measurement of Beam Profile

Measurement of Beam Profile Measurement of Beam Profile The beam width can be changed by focusing via quadruples. Transverse matching between ascending accelerators is done by focusing. Profiles have to be controlled at many locations.

More information

PRIOR. Proton Microscope for FAIR

PRIOR. Proton Microscope for FAIR PRIOR Proton Microscope for FAIR Proton Radiography Basics X-rays and protons ranges in matter X-rays 3-10 MeV (Flux attenuation in e times) High Energy Protons ~ GeV cm 1 cm Pb Protons Image Blurring

More information

Juliane Rönsch Hamburg University. Investigations of the longitudinal phase space at a photo injector for the X-FEL

Juliane Rönsch Hamburg University. Investigations of the longitudinal phase space at a photo injector for the X-FEL Juliane Rönsch Hamburg University Investigations of the longitudinal phase space at a photo injector for the X-FEL Juliane Rönsch 1/15/28 1 Contents Introduction PITZ Longitudinal phase space of a photoinjector

More information

Measurement of transverse Emittance

Measurement of transverse Emittance Measurement of transverse Emittance The emittance characterizes the whole beam quality, assuming linear behavior as described by second order differential equation. 1 It is defined within the phase space

More information

Simulations of the IR/THz Options at PITZ (High-gain FEL and CTR)

Simulations of the IR/THz Options at PITZ (High-gain FEL and CTR) Case Study of IR/THz source for Pump-Probe Experiment at the European XFEL Simulations of the IR/THz Options at PITZ (High-gain FEL and CTR) Introduction Outline Simulations of High-gain FEL (SASE) Simulation

More information

LOLA: Past, present and future operation

LOLA: Past, present and future operation LOLA: Past, present and future operation FLASH Seminar 1/2/29 Christopher Gerth, DESY 8/5/29 FLASH Seminar Christopher Gerth 1 Outline Past Present Future 8/5/29 FLASH Seminar Christopher Gerth 2 Past

More information

Observation of Coherent Optical Transition Radiation in the LCLS Linac

Observation of Coherent Optical Transition Radiation in the LCLS Linac Observation of Coherent Optical Transition Radiation in the LCLS Linac Henrik Loos, Ron Akre, Franz-Josef Decker, Yuantao Ding, David Dowell, Paul Emma,, Sasha Gilevich, Gregory R. Hays, Philippe Hering,

More information

Commissioning of the new Injector Laser System for the Short Pulse Project at FLASH

Commissioning of the new Injector Laser System for the Short Pulse Project at FLASH Commissioning of the new Injector Laser System for the Short Pulse Project at FLASH Uni Hamburg tim.plath@desy.de 05.11.2013 Supported by BMBF under contract 05K10GU2 & FS FLASH 301 Motivation short pulses

More information

Status Report on the Survey and Alignment efforts at DESY

Status Report on the Survey and Alignment efforts at DESY Status Report on the Survey and Alignment efforts at DESY Johannes J. Prenting Deutsches Elektronen-Synchrotron DESY, MEA2 IWAA 2008 KEK Japan Major New Projects @ DESY - : European X-ray Free Electron

More information

Commissioning of the SNS Beam Instrumentation

Commissioning 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 information

DIAGNOSTIC TEST-BEAM-LINE FOR THE MESA INJECTOR

DIAGNOSTIC TEST-BEAM-LINE FOR THE MESA INJECTOR DIAGNOSTIC TEST-BEAM-LINE FOR THE MESA INJECTOR I.Alexander,K.Aulenbacher,V.Bechthold,B.Ledroit,C.Matejcek InstitutfürKernphysik,JohannesGutenberg-Universität,D-55099Mainz,Germany Abstract With the test-beam-line

More information

UCLA Neptune Ramped Bunch Experiment. R. Joel England UCLA Department of Physics and Astronomy Particle Beam Physics Laboratory May 19, 2004

UCLA Neptune Ramped Bunch Experiment. R. Joel England UCLA Department of Physics and Astronomy Particle Beam Physics Laboratory May 19, 2004 UCLA Neptune Ramped Bunch Experiment R. Joel England UCLA Department of Physics and Astronomy Particle Beam Physics Laboratory May 19, 2004 Outline 1. Background & Motivation 2. Neptune Dogleg Compressor

More information

STATUS OF E-157: METER-LONG PLASMA WAKEFIELD EXPERIMENT. Presented by Patrick Muggli for the E-157 SLAC/USC/LBNL/UCLA Collaboration

STATUS OF E-157: METER-LONG PLASMA WAKEFIELD EXPERIMENT. Presented by Patrick Muggli for the E-157 SLAC/USC/LBNL/UCLA Collaboration STATUS OF E-157: METER-LONG PLASMA WAKEFIELD EXPERIMENT Presented by Patrick Muggli for the E-157 SLAC/USC/LBNL/UCLA Collaboration OUTLINE Basic E-157 Acelleration, Focusing Plasma Source Diagnostics:

More information

Newport News, VA Abstract

Newport News, VA Abstract High Current CW Beam Profile Monitors Using Transition Radiation at CEBAF l?ece/ve =J P. Piot, J-C. Denard, P. Adderley, K. Capek, E. Feldl * JM. 2 5 1998 Continuous Electron Beam Accelerator Facility,

More information

Single-shot Ultrafast Electron Microscopy

Single-shot Ultrafast Electron Microscopy Single-shot Ultrafast Electron Microscopy Renkai Li and Pietro Musumeci Department of Physics and Astronomy, UCLA 25 th North American Particle Accelerator Conference Sep 30 - Oct 4, 2013, Pasadena, CA,

More information

Summary of COTR Effects.

Summary of COTR Effects. Summary of COTR Effects. Stephan Wesch Deutsches Elektronen-Synchrotron, Hamburg 10 th European Workshop on Beam Diagnostics and Instrumentation for Particle Accelerators S. Wesch (DESY) Summary of COTR

More information

Tuning Techniques And Operator Diagnostics for FACET at SLAC National Accelerator Laboratory. Chris Melton SLAC Accelerator Operations

Tuning Techniques And Operator Diagnostics for FACET at SLAC National Accelerator Laboratory. Chris Melton SLAC Accelerator Operations Tuning Techniques And Operator Diagnostics for FACET at SLAC National Accelerator Laboratory Chris Melton SLAC Accelerator Operations FACET Tuning And Diagnostics What is FACET? FACET Performance Challenges

More information

Electron Energy (MeV)

Electron Energy (MeV) A High Resolution Electron Beam Prole Monitor and its Applications W. S. Graves, E. D. Johnson, and S. Ulc Brookhaven National Laboratory, Upton, NY 11973 USA Abstract. A beam diagnostic to measure transverse

More information

LCLS Injector Straight Ahead Spectrometer C.Limborg-Deprey Stanford Linear Accelerator Center 8 th June 2005

LCLS Injector Straight Ahead Spectrometer C.Limborg-Deprey Stanford Linear Accelerator Center 8 th June 2005 LCLS Injector Straight Ahead Spectrometer C.Limborg-Deprey Stanford Linear Accelerator Center 8 th June 2005 Summary The spectrometer design was modified to allow the measurement of uncorrelated energy

More information

GTF Transverse and Longitudinal Emittance Data Analysis Technique * J.F. Schmerge, J.E. Clendenin, D.H. Dowell and S.M. Gierman

GTF Transverse and Longitudinal Emittance Data Analysis Technique * J.F. Schmerge, J.E. Clendenin, D.H. Dowell and S.M. Gierman LCLS-TN-5-19 July 5 GTF Transverse and Longitudinal Emittance Data Analysis Technique * J.F. Schmerge, J.E. Clendenin, D.H. Dowell and S.M. Gierman Abstract The SSRL Gun Test Facility (GTF) was built to

More information

The ISIS Penning H - SPS and Diagnostic Developments at RAL

The ISIS Penning H - SPS and Diagnostic Developments at RAL The ISIS Penning H - SPS and Diagnostic Developments at RAL D.C. Faircloth 1, A.P. Letchford 1, J. Pozimski 1+2, M.O. Whitehead 1, T. Wood 1, S. Jolly 2, P. Savage 2, M. Haigh 3, J. Morrison 3, I. Yew

More information

Experimental Optimization of Electron Beams for Generating THz CTR and CDR with PITZ

Experimental Optimization of Electron Beams for Generating THz CTR and CDR with PITZ Experimental Optimization of Electron Beams for Generating THz CTR and CDR with PITZ Introduction Outline Optimization of Electron Beams Calculations of CTR/CDR Pulse Energy Summary & Outlook Prach Boonpornprasert

More information

New Versatile Platform Based on the Low Energy Electron Beam Delivered by the PHIL Photoinjector

New Versatile Platform Based on the Low Energy Electron Beam Delivered by the PHIL Photoinjector WDS'13 Proceedings of Contributed Papers, Part III, 33 38, 2013. ISBN 978-80-7378-252-8 MATFYZPRESS New Versatile Platform Based on the Low Energy Electron Beam Delivered by the PHIL Photoinjector S. Barsuk,

More information

SURVEY AND ALIGNMENT FOR THE SYNCHROTRON LIGHT SOURCE ELETTRA

SURVEY AND ALIGNMENT FOR THE SYNCHROTRON LIGHT SOURCE ELETTRA I/49 SURVEY AND ALIGNMENT FOR THE SYNCHROTRON LIGHT SOURCE ELETTRA ABSTRACT: F.Wei, A.Bergamo, P.Furlan, J.Grgic, A.Wrulich Sincrotrone Trieste Padriciano 99, 34012 Trieste, Italy ELETTRA is a third generation

More information

ENERGY DEPOSITION EFFECTS OF THE X PHOTON BEAM ON THE MIRROR OF PLASMON-X EXPERIMENT AT LI2FE. Francesco Broggi, Luca Serafini

ENERGY DEPOSITION EFFECTS OF THE X PHOTON BEAM ON THE MIRROR OF PLASMON-X EXPERIMENT AT LI2FE. Francesco Broggi, Luca Serafini SPARC-EBD -10/01 21 Luglio 2010 ENERGY DEPOSITION EFFECTS OF THE X PHOTON BEAM ON THE MIRROR OF PLASMON-X EXPERIMENT AT LI2FE Francesco Broggi, Luca Serafini INFN-LASA-Sezione di Milano, Via F.ll icervi

More information

Development of Large Scale Optimization Tools for Beam Tracking Codes

Development of Large Scale Optimization Tools for Beam Tracking Codes Development of Large Scale Optimization Tools for Beam Tracking Codes 42 nd ICFA Advanced Beam Dynamics Workshop: High-Intensity, High-Brightness Hadron Beams HB-2008, August 25-29, 2008 Nashville, Tennessee,

More information

Laser Heater Integration into XFEL. Update. Yauhen Kot XFEL Beam Dynamics Meeting

Laser Heater Integration into XFEL. Update. Yauhen Kot XFEL Beam Dynamics Meeting Laser Heater Integration into XFEL. Update. Yauhen Kot XFEL Beam Dynamics Meeting 5..8 Outline Overview about the main components and space margins Optics at the laser heater and diagnostics - FODO + parabola-like

More information

What have we learned from the LCLS injector?*

What have we learned from the LCLS injector?* SLAC-PUB-14644 LCLS-TN-11-4 October 19, 2011 What have we learned from the LCLS injector?* Feng Zhou and Axel Brachmann for the LCLS injector team The LCLS injector reliably delivered a high quality electron

More information

The Second Half Year 2017 PAL-XFEL Call for Proposals

The Second Half Year 2017 PAL-XFEL Call for Proposals The Second Half Year 2017 PAL-XFEL Call for Proposals Summary Information for Submitting Proposals We encourage scientists from all over the world to submit applications for beam time proposal to utilize

More information

Emittance and photocathodes

Emittance and photocathodes Cornell Laboratory for Accelerator-based ScienceS and Education () Emittance and photocathodes Ivan Bazarov Where we are today Injector performance Ongoing work Venues for improvements Next generation

More information

Progress towards slice emittance measurements at PITZ. Raffael Niemczyk for the PITZ team, Würzburg, March 20 th 2018

Progress towards slice emittance measurements at PITZ. Raffael Niemczyk for the PITZ team, Würzburg, March 20 th 2018 Progress towards slice emittance measurements at PITZ Raffael Niemczyk for the PITZ team, Würzburg, March 20 th 2018 PITZ Overview Photo-Injector Test Facility at DESY, Zeuthen Site > Three Emittance Measurement

More information

Dielectric Meta-Reflectarray for Broadband Linear Polarization Conversion and Optical Vortex Generation

Dielectric Meta-Reflectarray for Broadband Linear Polarization Conversion and Optical Vortex Generation Supporting Information Dielectric Meta-Reflectarray for Broadband Linear Polarization Conversion and Optical Vortex Generation Yuanmu Yang, Wenyi Wang, Parikshit Moitra, Ivan I. Kravchenko, Dayrl P. Briggs,

More information

Spectroscopy with Free Electron Lasers. David Bernstein SASS Talk January 28 th, 2009

Spectroscopy with Free Electron Lasers. David Bernstein SASS Talk January 28 th, 2009 Spectroscopy with Free Electron Lasers David Bernstein SASS Talk January 28 th, 2009 Overview Who am I?! What is FLASH?! The promise of Free Electron Lasers (FELs) The Trouble with Spectroscopy Sample

More information

Linac Based Photon Sources: XFELS. Coherence Properties. J. B. Hastings. Stanford Linear Accelerator Center

Linac Based Photon Sources: XFELS. Coherence Properties. J. B. Hastings. Stanford Linear Accelerator Center Linac Based Photon Sources: XFELS Coherence Properties J. B. Hastings Stanford Linear Accelerator Center Coherent Synchrotron Radiation Coherent Synchrotron Radiation coherent power N 6 10 9 incoherent

More information

LCLS Commissioning Status

LCLS Commissioning Status LCLS Commissioning Status Paul Emma (for the LCLS Commissioning Team) June 20, 2008 LCLS ANL LLNL UCLA FEL Principles Electrons slip behind EM wave by λ 1 per undulator period ( (λ u ) x K/γ e λ u v x

More information

Photon Instrumentation. First Mexican Particle Accelerator School Guanajuato Oct 6, 2011

Photon Instrumentation. First Mexican Particle Accelerator School Guanajuato Oct 6, 2011 Photon Instrumentation First Mexican Particle Accelerator School Guanajuato Oct 6, 2011 Outline The Electromagnetic Spectrum Photon Detection Interaction of Photons with Matter Photoelectric Effect Compton

More information

Emittance (Profile) Measurements in the Proton Accelerators at DESY

Emittance (Profile) Measurements in the Proton Accelerators at DESY Emittance (Profile) Measurements in the Proton Accelerators at DESY Kay Wittenburg, MDI Deutsches Electronen Synchrotron Hamburg, Germany Profile Monitors in the Proton Accelerators DESY III:» Wire Scanner,

More information

LCLS Injector Prototyping at the GTF

LCLS Injector Prototyping at the GTF LCLS Injector Prototyping at at the GTF John John Schmerge, SLAC SLAC November 3, 3, 23 23 GTF GTF Description Summary of of Previous Measurements Longitudinal Emittance Transverse Emittance Active LCLS

More information

(M. Bowler, C. Gerth, F. Hannon, H. Owen, B. Shepherd, S. Smith, N. Thompson, E. Wooldridge, N. Wyles)

(M. Bowler, C. Gerth, F. Hannon, H. Owen, B. Shepherd, S. Smith, N. Thompson, E. Wooldridge, N. Wyles) Optics considerations for ERL test facilities Bruno Muratori ASTeC Daresbury Laboratory (M. Bowler, C. Gerth, F. Hannon, H. Owen, B. Shepherd, S. Smith, N. Thompson, E. Wooldridge, N. Wyles) Overview Optics

More information

First observation of Current Filamentation Instability (CFI)

First observation of Current Filamentation Instability (CFI) First observation of Current Filamentation Instability (CFI) PI - Patric Muggli: University of Southern California Vitaly Yakimenko, Mikhail Fedurin, Karl Kusche, Marcus Babzien: Brookhaven National Laboratory

More information

L. Bobb 1, 2, M. Billing 3, N. Chritin 2, P. Karataev 1, T. Lefevre 2

L. Bobb 1, 2, M. Billing 3, N. Chritin 2, P. Karataev 1, T. Lefevre 2 L. Bobb 1, 2, M. Billing 3, N. Chritin 2, P. Karataev 1, T. Lefevre 2 1. John Adams Institute at Royal Holloway, Egham, Surrey, United Kingdom 2. CERN European Organisation for Nuclear Research, CERN,

More information

MEASURING AND CONTROLLING ENERGY SPREAD IN CEBAF

MEASURING AND CONTROLLING ENERGY SPREAD IN CEBAF MEASURING AND CONTROLLING ENERGY SPREAD IN CEBAF Abstract G. A. Krafft, J.-C. Denard, R. W. Dickson, R. Kazimi, V. A. Lebedev, and M. G. Tiefenback TJNAF, Newport News, VA2366, USA As compared to electron

More information

Two Dimensional SR-Interferometer at PETRA III. Artem Novokshonov DESY, Tomsk Polytechnic University

Two Dimensional SR-Interferometer at PETRA III. Artem Novokshonov DESY, Tomsk Polytechnic University Two Dimensional SR-Interferometer at PETRA III Artem Novokshonov DESY, Tomsk Polytechnic University First Part: Two Dimensional Interferometer at Petra III Interferometer principal Schematic of the Interferometer

More information

An Adventure in Marrying Laser Arts and Accelerator Technologies

An Adventure in Marrying Laser Arts and Accelerator Technologies An Adventure in Marrying Laser Arts and Accelerator Technologies Dao Xiang Beam Physics Dept, SLAC, Stanford University Feb-28-2012 An example sample Probe (electron) Pump (laser) Typical pump-probe experiment

More information

SCSS Prototype Accelerator -- Its outline and achieved beam performance --

SCSS Prototype Accelerator -- Its outline and achieved beam performance -- SCSS Prototype Accelerator -- Its outline and achieved beam performance -- Hitoshi TANAKA RIKEN, XFEL Project Office 1 Content 1. Light Quality; SPring-8 v.s. XFEL 2. What are the critical issues? 3. Mission

More information

Small Isochronous Ring (SIR) project at NSCL, MSU. Eduard Pozdeyev NSCL, Michigan Sate University

Small Isochronous Ring (SIR) project at NSCL, MSU. Eduard Pozdeyev NSCL, Michigan Sate University Small Isochronous Ring (SIR) project at NSCL, MSU Eduard Pozdeyev NSCL, Michigan Sate University Talk Outline Isochronous regime in accelerators, application to Isochronous Cyclotrons Space charge effects

More information

SLS at the Paul Scherrer Institute (PSI), Villigen, Switzerland

SLS at the Paul Scherrer Institute (PSI), Villigen, Switzerland SLS at the Paul Scherrer Institute (PSI), Villigen, Switzerland Michael Böge 1 SLS Team at PSI Michael Böge 2 Layout of the SLS Linac, Transferlines Booster Storage Ring (SR) Beamlines and Insertion Devices

More information

Diagnostics Requirements for the ARIEL Low Energy Beam Transport

Diagnostics Requirements for the ARIEL Low Energy Beam Transport Document-121991 Diagnostics Requirements for the ARIEL Low Energy Beam Transport Document Type: Requirement Document Release: 02 Release Date: 2017-03-22 Authors: S. Saminathan, M. Marchetto, C. Barquest

More information

Needle cathodes for high-brightness beams. Chase Boulware Jonathan Jarvis Heather Andrews Charlie Brau

Needle cathodes for high-brightness beams. Chase Boulware Jonathan Jarvis Heather Andrews Charlie Brau Needle cathodes for high-brightness beams Chase Boulware Jonathan Jarvis Heather Andrews Charlie Brau Outline of the talk What is brightness? Definition Sources Why is brightness important? Light sources

More information

RF-Gun Experience at PITZ - Longitudinal Phase Space

RF-Gun Experience at PITZ - Longitudinal Phase Space - Collaboration meeting 9th of October 2006 Hamburg University Juliane Rönsch 1 Motivation special device to measure the longitudinal phase space at low momentum typical high energy diagnostics can not

More information

Transverse Beam Optics of the FLASH Facility

Transverse Beam Optics of the FLASH Facility Transverse Beam Optics of the FLASH Facility ( current status and possible updates ) Nina Golubeva and Vladimir Balandin XFEL Beam Dynamics Group Meeting, 18 June 2007 Outline Different optics solutions

More information

Status of the LHCb RICH detector and the HPD

Status of the LHCb RICH detector and the HPD Beauty 2005 Status of the LHCb RICH detector and the HPD Tito Bellunato Università degli Studi di Milano Bicocca & INFN On behalf of the LHCb RICH group Assisi 23 June Assisi 2005 23 June Tito Bellunato

More information

Comparison of the APS Upgrade to

Comparison of the APS Upgrade to Comparison of the APS Upgrade to ERL@APS Michael Borland Argonne National Laboratory March 2010 The submitted manuscript has been created by UChicago Argonne, LLC, Operator of Argonne National Laboratory

More information

Modeling of the secondary electron emission in rf photocathode guns

Modeling of the secondary electron emission in rf photocathode guns Modeling of the secondary electron emission in rf photocathode guns J.-H. Han, DESY Zeuthen 8 June 2004 Joint Uni. Hamburg and DESY Accelerator Physics Seminar Contents 1. Necessity of secondary electron

More information

SL_COMB. The SL_COMB experiment at SPARC_LAB will operate in the so-called quasinonlinear regime, defined by the dimensionless charge quantity

SL_COMB. The SL_COMB experiment at SPARC_LAB will operate in the so-called quasinonlinear regime, defined by the dimensionless charge quantity SL_COMB E. Chiadroni (Resp), D. Alesini, M. P. Anania (Art. 23), M. Bellaveglia, A. Biagioni (Art. 36), S. Bini (Tecn.), F. Ciocci (Ass.), M. Croia (Dott), A. Curcio (Dott), M. Daniele (Dott), D. Di Giovenale

More information

The Cylindrical GEM detector for the KLOE-2 Inner Tracker

The Cylindrical GEM detector for the KLOE-2 Inner Tracker The Cylindrical GEM detector for the KLOE-2 Inner Tracker G. Morello on behalf of the KLOE-2 IT group Exploring Hadron Structure with Tagged Structure Functions, January 18th, Newport News (VA) KLOE-2

More information

LCLS Undulators Present Status and Future Upgrades

LCLS Undulators Present Status and Future Upgrades LCLS Undulators Present Status and Future Upgrades Heinz-Dieter Nuhn LCLS Undulator Group Leader 1 1 Heinz-Dieter Nuhn Linac Coherent Light Source INJECTOR LINAC BEAM TRANSPORT UNDULATOR HALL 2 2 Heinz-Dieter

More information

PoS(EPS-HEP2017)533. First Physics Results of AWAKE, a Plasma Wakefield Acceleration Experiment at CERN. Patric Muggli, Allen Caldwell

PoS(EPS-HEP2017)533. First Physics Results of AWAKE, a Plasma Wakefield Acceleration Experiment at CERN. Patric Muggli, Allen Caldwell First Physics Results of AWAKE, a Plasma Wakefield Acceleration Experiment at CERN Patric Muggli, Max Planck Institute for Physics E-mail: muggli@mpp.mpg.de AWAKE is a plasma wakefield acceleration experiment

More information

Update on Timepix3 Telescope & Grazing Angles Results

Update on Timepix3 Telescope & Grazing Angles Results Update on Timepix Telescope & Grazing Angles Results on behalf of the VELO Testbeam Group th Beam Telescopes and Test Beams workshop Barcelona -7//7 Timepix Telescope th BTTB - //7 Timepix Telescope Device

More information

The New Superconducting RF Photoinjector a High-Average Current & High-Brightness Gun

The New Superconducting RF Photoinjector a High-Average Current & High-Brightness Gun The New Superconducting RF Photoinjector a High-Average Current & High-Brightness Gun Jochen Teichert for the BESSY-DESY-FZD-MBI collaboration and the ELBE crew High-Power Workshop, UCLA, Los Angeles 14

More information

Alpha particle scintillation detector based on micro pixel avalanche photodiode and LYSO crystal

Alpha particle scintillation detector based on micro pixel avalanche photodiode and LYSO crystal Alpha particle scintillation detector based on micro pixel avalanche photodiode and LYSO crystal G.S. Ahmadov, F.I. Ahmadov Institute of Radiation Problems of ANAS, Baku, Azerbaijan C. Granja, S. Pospíšil

More information

Charge for WG2 (Optics and Beams)

Charge for WG2 (Optics and Beams) Charge for WG2 (Optics and Beams) Georg H. Hoffstaetter (Cornell University / Physics) on behalf of the conveners of WG2: Vladimir Litvinenko (BNL / Accelerator Physics) Hywel Owen (Daresbury / ASTeC)

More information

arxiv: v2 [physics.acc-ph] 21 Jun 2017

arxiv: v2 [physics.acc-ph] 21 Jun 2017 Pulsed Beam Tests at the SANAEM RFQ Beamline arxiv:1705.06462v2 [physics.acc-ph] 21 Jun 2017 G Turemen 1,2, Y Akgun 1, A Alacakir 1, I Kilic 1, B Yasatekin 1,2, E Ergenlik 3, S Ogur 3, E Sunar 3, V Yildiz

More information

Free-electron laser SACLA and its basic. Yuji Otake, on behalf of the members of XFEL R&D division RIKEN SPring-8 Center

Free-electron laser SACLA and its basic. Yuji Otake, on behalf of the members of XFEL R&D division RIKEN SPring-8 Center Free-electron laser SACLA and its basic Yuji Otake, on behalf of the members of XFEL R&D division RIKEN SPring-8 Center Light and Its Wavelength, Sizes of Material Virus Mosquito Protein Bacteria Atom

More information

Optimum beam creation in photoinjectors using spacecharge expansion II: experiment

Optimum beam creation in photoinjectors using spacecharge expansion II: experiment Optimum beam creation in photoinjectors using spacecharge expansion II: experiment J. Rosenzweig, A. Cook, M. Dunning, R.J. England, G. Travish, UCLA P. Musumeci, C. Vicario, D. Filippetto, M. Ferrario,

More information

REVIEW OF DIAGNOSTICS FOR NEXT GENERATION LINEAR ACCELERATORS

REVIEW OF DIAGNOSTICS FOR NEXT GENERATION LINEAR ACCELERATORS REVIEW OF DIAGNOSTICS FOR NEXT GENERATION LINEAR ACCELERATORS M. Ross, Stanford Linear Accelerator Center, Stanford, CA 9439, USA Abstract New electron linac designs incorporate substantial advances in

More information

THE LASER HEATER SYSTEM OF SWISSFEL

THE LASER HEATER SYSTEM OF SWISSFEL THE LASER HEATER SYSTEM OF SWISSFEL M. Pedrozzi, M. Calvi, R. Ischebeck, S. Reiche, C. Vicario, PSI, Villigen, Switzerland B. D. Fell, N. Thompson, STFC/DL/ASTeC, Daresbury, UK Short wavelength FELs are

More information

Radiation Protection Considerations for the Cryogenic In-Vacuum Undulator of the EMIL Project at BESSY

Radiation Protection Considerations for the Cryogenic In-Vacuum Undulator of the EMIL Project at BESSY Radiation Protection Considerations for the Cryogenic In-Vacuum Undulator of the EMIL Project at BESSY Yvonne Bergmann, Klaus Ott Helmholtz- Zentrum Berlin BESSY II Radiation Protection Department yvonne.bergmann@helmholtz-berlin.de

More information

X-TOD Update. Facility Advisory Committee Photon Breakout Session. October 30, 2007

X-TOD Update. Facility Advisory Committee Photon Breakout Session. October 30, 2007 XTOD Update Facility Advisory Committee Photon Breakout Session LCLS Layout Linac Undulator Hall FEE (Front-End-Enclosure) Diagnostics SOMS HOMS X-Ray Tunnel FEH (Far Experimental Hall) NEH (Near Experimental

More information

X-ray fluorescence analysis - calibration of the X-ray energy detector

X-ray fluorescence analysis - calibration of the X-ray energy detector X-ray fluorescence analysis - TEP Related topics Bremsstrahlung, characteristic X-radiation, energy levels, fluorescence radiation, conduction processes in semiconductors, doping of semiconductors, pin-diodes,

More information

Fast Neutron and Gamma-Ray Detectors for the CSIRO Air Cargo Scanner

Fast Neutron and Gamma-Ray Detectors for the CSIRO Air Cargo Scanner Fast Neutron and Gamma-Ray Detectors for the CSIRO Air Cargo Scanner J.E. Eberhardt, A.J. McEwan, D. Milinkovic, V. Sharp, * and J.R. Tickner CSIRO Minerals, Private Mail Bag 5, Menai NSW 2234 Australia

More information