Emission-related Activities at PITZ Proposals for the DFG-Networking "Hi 2 PE"
|
|
- Bruno Ellis
- 5 years ago
- Views:
Transcription
1 Emission-related Activities at PITZ Proposals for the DFG-Networking "Hi 2 PE" Ye Chen for the PITZ team , Helmholtz-Zentrum Berlin, Germany Contents Photoemission (PE) Dark Current (DC) Other (Long-Term) Topics Literature [1] S. Schreiber, S. Lederer, FEL 2015 [2] L. Monaco, P. Michelato, et al., EPAC 2006 [3] D. Filippetto, P. Musumeci, et al., PRSTAB 17, (2014) [4] D. Lipka, et al., DIPAC 2011 [5] K. L. Jensen, Advances in Imaging and Electron Physics, Electron Emission Physics Vol.149, 2007 [6] E. Gjonaj, ICAP 2012 [7] R. Xiang, A. Arnold, T. Kamps, et al., PRSTAB 17, (2014) [8] P. Piot, et al., PRSTAB 16, (2013) [9] M. Zolotorev, SLAC-PUB-5896 (1992)
2 Photoemission (PE) Studies 1. (Cs 2 Te) Experimental & Numerical PE Studies Ongoing activity at PITZ and TU Darmstadt Impacts of full EM field (RF + space charge)@cathode on PE (Cont.) Modeling of PE in space charge dominated regime Charge production using various RF gun and measured PC laser parameters (simulation vs. measurement) Dedicated studies on bunch length, slice energy spread, etc., to explain discrepancies between simulation and measurement (e.g., Bunch length in Astra systematically longer) Further modeling requires realistic cathode laser distributions Radially uniform distribution Dynamic emission process from cathode taking into account 3D full EM fields at cathode in a Lienard-Wiechert approach Charge production per simulation time step: Measured Bunch charge Space charge dominated regime Non-uniform distribution generated according to VC2 data OSS signal with measured flattop pulse shape (old data) Quantum efficiency formulism: Measured pulse shape + length Field-induced work function modification: More precise treatments needed for the modeling in space charge dominated regime Remaining deviations w.r.t. simulations probably due to the initial ideal beam distributions plugged in the simulations Ye Chen Proposals for Hi2PE Networking: Emission-related Studies at PITZ Page 2/5 + Possible laser intensity and time dependent cathode work function variation, e.g., in [9]
3 Photoemission (PE) Studies (cont.) 2. (Cs 2 Te) Investigations of a µs-scale spiky structure during electron bunch train extraction at FLASH Ongoing activity at PITZ, INFN and FLASH Flat UV laser energy pulse train producing µs-scale spiky structure along electron bunch train Toward modeling of RF pulse and/or laser pulse heating effect Emission issue of fresh cathode 73.3 (and some others) at FLASH, , QE=10% ~8% Experiments at PITZ Fixed BSA SP mm, 43.3 MV/m vs MV/m, LT=10% Set the working point in linear emission regime ~9% Laser pulse heating? Ye Chen Proposals for Hi2PE Networking: Emission-related Studies at PITZ Page 3/5
4 Dark Current (DC) Characterization and Simulation 1. Detailed experimental DC characterization DC vs. Solenoid current, RF power, pulse length, etc. DC spectrum measurement DC transportation 2. DC monitoring method Using Faraday Cups (e.g., ~10 pc resolution) Using non-destructive resonator prototype (e.g., 0.5mV for 1µA) 3. DC modeling and simulation based on Fowler-Nordheim theory "Realistic" cathode geometry model Surface condition determination (scanning electron microscopy?) 3D dark current generator Dark current transportation studies Identify critical areas for the source of dark currents by particle tracking simulations DC on Low.Scr.1 β 0 β i uniform E 0 β 2 β 3 β 6 β 1 β 4 Cathode surface DCM at PITZ and XFEL Local field enhancement factor, Simulated DC patterns in [2] with uniform field distribution at cathode surface Microscopic nonuniform local field forming structures Resulting in nonuniform field distribution E n at cathode surface Ye Chen Proposals for Hi2PE Networking: Emission-related Studies at PITZ Page 4/5
5 Other (Long-Term) Topics > Charge production at theoretical space charge limitation for different PC laser pulse shapes and parameters (modeling + simulation) > Cathode brightness studies with variable beam aspect ratios > "Green photocathode" studies and tests (PITZ + INFN) > Studies of slice emittance formation for various PC laser pulse shapes and for various gun field gradients (towards SC and CW regimes) > Formation of ellipsoidal electron bunches by space charge driven expansion using PITZ Pharos laser (variable PL down to ~200 fs ) Semi-analytical solution for flattop-shaped bunch in cigar regime (in [3]), The theory may be less effective for Gaussian bunches (even more prevalent in many facilities) In the limit of cigar aspect ratio, Maximum cathode brightness for Gaussian bunches? Thank you very much! Ye Chen Proposals for Hi2PE Networking: Emission-related Studies at PITZ Page 5/5
Electron Emission Studies Using Enhanced QE Models
Y. Chen, E. Gjonaj, H. De Gersem, W.F.O. Müller, T. Weiland Computational Electromagnetics Laboratory (TEMF) Technische Universität Darmstadt, Germany Electron Emission Studies Using Enhanced QE Models
More informationSelected Beam Studies at PITZ in 2017
Selected Beam Studies at PITZ in 7 Ye Chen and Mikhail Krasilnikov for the PITZ Team TEMF-DESY Collaboration Meeting..7, TEMF, Darmstadt, Germany Contents Photoemission modeling in the gun Updates on beam
More informationBeam dynamics studies for PITZ using a 3D full-wave Lienard-Wiechert PP code
Beam dynamics studies for PITZ using a 3D full-wave Lienard-Wiechert PP code Y. Chen, E. Gjonaj, H. De Gersem, T. Weiland TEMF, Technische Universität Darmstadt, Germany DESY-TEMF Collaboration Meeting
More informationDark current at the Euro-XFEL
Dark current at the Euro-XFEL Jang-Hui Han DESY, MPY Observations at PITZ and FLASH Estimation for the European XFEL Ideas to reduce dark current at the gun DC at FLASH RF gun M1 M2 M3 M4 M5 M6 M7 6 undulator
More informationPhoto Injector Test facility at DESY, Zeuthen site
Photo Injector Test facility at DESY, Zeuthen site PITZ EXPERIENCE ON THE EXPERIMENTAL OPTIMIZATION OF THE RF PHOTO INJECTOR FOR THE EUROPEAN XFEL Mikhail Krasilnikov (DESY) for the PITZ Team FEL 2013
More informationModeling 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 informationDark Current at Injector. Jang-Hui Han 27 November 2006 XFEL Beam Dynamics Meeting
Dark Current at Injector Jang-Hui Han 27 November 2006 XFEL Beam Dynamics Meeting Considerations for the guns Ultra-low slice emittance of electron beams higher gradient at the gun cavity solenoid field
More informationMotivation 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 informationSimulations 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 informationNumerical modelling of photoemission for the PITZ photoinjector
Numerical modelling of photoemission for the PITZ photoinjector Ye Chen, Erion Gjonaj, Wolfgang Müller, Herbert De Gersem, Thomas Weiland TEMF, TU Darmstadt DESY-TEMF Collaboration Meeting DESY, Hamburg,
More informationDiagnostic 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 informationInvestigations 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 informationSwissFEL INJECTOR DESIGN: AN AUTOMATIC PROCEDURE
Proceedings of FEL03, New York, NY, USA SwissFEL INJECTOR DESIGN: AN AUTOMATIC PROCEDURE S. Bettoni, M. Pedrozzi, S. Reiche, PSI, Villigen, Switzerland Abstract The first section of FEL injectors driven
More informationIntroduction to the benchmark problem
Introduction to the benchmark problem M. Krasilnikov (DESY) Working group 4: Low emittance electron guns 37th ICFA Beam Dynamics Workshop Future Light Sources 15 19 May 6 DESY, Hamburg, Germany Outline
More informationSRF 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 informationExperimental 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 informationStart-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 informationASTRA simulations of the slice longitudinal momentum spread along the beamline for PITZ
ASTRA simulations of the slice longitudinal momentum spread along the beamline for PITZ Orlova Ksenia Lomonosov Moscow State University GSP-, Leninskie Gory, Moscow, 11999, Russian Federation Email: ks13orl@list.ru
More informationTomographic transverse phase space measurements at PITZ.
Tomographic transverse phase space measurements at PITZ. > Photo-Injector Test facility at DESY in Zeuthen - PITZ > Tomography in beam diagnostics > Hardware > Measurements & evaluation Georgios Kourkafas,
More information1. Beam based alignment Laser alignment Solenoid alignment 2. Dark current 3. Thermal emittance
Beam based alignment, Dark current and Thermal emittance measurements J-H.Han,M.Krasilnikov,V.Miltchev, PITZ, DESY, Zeuthen 1. Beam based alignment Laser alignment Solenoid alignment 2. Dark current 3.
More informationSimulations 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 informationPhoto Injector Test facility at DESY, Zeuthen site. PITZ: facility overview
Photo Injector Test facility at DESY, Zeuthen site. PITZ: facility overview Mikhail Krasilnikov (DESY) for the PITZ Team Mini-workshop on THz option at PITZ, Zeuthen, 22.09.2015 Photo Injector Test facility
More informationSingle-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 informationThe 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 informationHigh brightness beam science
High brightness beam science P. Musumeci UCLA Department of Physics and Astronomy FEIS Workshop December 9 12th, 2013 Key West, Florida Outline Beam brightness. Useful figure of merit to compare different
More informationAccelerator Activities at PITZ
Accelerator Activities at PITZ Plasma acceleration etc. Outline > Motivation / Accelerator Research & Development (ARD) > Plasma acceleration Basic Principles Activities SINBAD > ps-fs electron and photon
More informationIntroduction. Thermoionic gun vs RF photo gun Magnetic compression vs Velocity bunching. Probe beam design options
Introduction Following the 19/05/04 meeting at CERN about the "CTF3 accelerated programme", a possible french contribution has been envisaged to the 200 MeV Probe Beam Linac Two machine options were suggested,
More informationCommissioning 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 informationStudies on charge production from Cs 2 Te photocathodes in the PITZ L-band normal conducting radio frequency photo injector
Studies on charge production from Cs 2 Te photocathodes in the PITZ L-band normal conducting radio frequency photo injector C. Hernandez-Garcia 1, M. Kraslinikov, G. Asova 2, M. Bakr 3, P. Boonpornprasert,
More informationRF Gun Photo-Emission Model for Metal Cathodes Including Time Dependent Emission
RF Gun Photo-Emission Model for Metal Cathodes Including Time Dependent Emission SLAC-PUB-117 February 6 (A) J. F. SCHMERGE, J. E. CLENDENIN, D. H. DOWELL, AND S. M. GIERMAN SLAC, Stanford University,
More informationTowards a Low Emittance X-ray FEL at PSI
Towards a Low Emittance X-ray FEL at PSI A. Adelmann, A. Anghel, R.J. Bakker, M. Dehler, R. Ganter, C. Gough, S. Ivkovic, F. Jenni, C. Kraus, S.C. Leemann, A. Oppelt, F. Le Pimpec, K. Li, P. Ming, B. Oswald,
More informationEXPERIMENTAL 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 informationDevelopment of reliable and sophisticated photo injector system and future plan
Development of reliable and sophisticated photo injector system and future plan Hiromitsu Tomizawa Accelerator Division, Japan Synchrotron Radiation Research Institute (JASRI/SPring-8) Kouto, Sayo-cho,
More informationLCLS 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 informationNeedle 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 informationTime 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 informationOverview of FEL injectors
Overview of FEL injectors Massimo Ferrario INFN - LNF VISA-DUV-HGHG 4GLS FLASH-XFEL LEUTL BESSY PAL LCLS Arc en Ciel FERMI SCSS LEG SPARX SDUV 1 SASE FEL Electron Beam Requirement: High Brightness B n
More informationPhoto Injector Test facility at DESY, Zeuthen site.
Photo Injector Test facility at DESY, Zeuthen site. Tunable IR/THz source based on PITZ (-like) accelerator for pump probe experiments at the European XFEL Mikhail Krasilnikov (DESY) for the PITZ Team
More informationJlab FEL Photoemission DC Guns
Jlab FEL Photoemission DC Guns Fay Hannon On behalf of the FEL team FLS 2010, 2 nd March 2 Operational Guns 1. FEL Gun 60m Gun Test Stand (GTS) 2. Backup gun, test stand with beam characterization beamline
More informationDESY/TEMF Meeting - Status 2011
Erion Gjonaj Technische Universität Darmstadt, Computational Electromagetics Laboratory (TEMF) Schlossgartenstr. 8 64289 Darmstadt, Germany DESY/TEMF Meeting - Status 211 DESY, Hamburg, 16.12.211 Contents
More informationAREAL. Test Facility for Advanced Accelerator and Radiation Sources Concepts. Part.1 Introduction. V. Tsakanov CANDLE SRI
AREAL Test Facility for Advanced Accelerator and Radiation Sources Concepts Part.1 Introduction V. Tsakanov CANDLE SRI 01 October 2015 2 nd European Advanced Accelerator Concepts 13-19 Sep 2015, Isola
More informationSTART-TO-END SIMULATIONS FOR IR/THZ UNDULATOR RADIATION AT PITZ
Proceedings of FEL2014, Basel, Switzerland MOP055 START-TO-END SIMULATIONS FOR IR/THZ UNDULATOR RADIATION AT PITZ P. Boonpornprasert, M. Khojoyan, M. Krasilnikov, F. Stephan, DESY, Zeuthen, Germany B.
More informationLow 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 informationWhat 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 informationTomography module for transverse phase-space measurements at PITZ.
Tomography module for transverse phase-space measurements at PITZ. > Photo-Injector Test facility @ DESY in Zeuthen - PITZ > Tomography module > Measurement results > Conclusions and outlook G. Asova for
More informationCurrent Status of Bunch Emission Simulation for the PITZ Gun
TUD-DESY Meeting 2013 ROOM 114, Darmstadt, Germany, 19.12.2013 Current Status of Bunch Emission Simulation for the PITZ Gun Ye Chen, Erion Gjonaj, Wolfgang Müller,Thomas Weiland 19. Dec. 2013 TU Darmstadt
More informationAREAL Test Facility for Advanced Accelerator and Radiation Sources Concepts
2 nd European Advanced Accelerator Concepts AREAL Test Facility for Advanced Accelerator and Radiation Sources Concepts V. Tsakanov CANDLE SRI 13-19 Sep 2015, La Biodola, Isola d'elba Introduction 2nd
More informationCsK 2 Sb PHOTOCATHODE DEVELOPMENT FOR. Martin Schmeißer, Julius Kühn, Thorsten Kamps, Andreas Jankowiak Helmholtz-Zentrum Berlin
CsK 2 Sb PHOTOCATHODE DEVELOPMENT FOR Martin Schmeißer, Julius Kühn, Thorsten Kamps, Andreas Jankowiak Helmholtz-Zentrum Berlin 1 PHOTOCATHODES Photoinjector for berlinpro Aim: 0.5 mm mrad emittance from
More informationDiagnostic 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 informationSimulations for a bunch compressor at PITZ Study of high transformer ratios
Simulations for a bunch compressor at PITZ Study of high transformer ratios G.Asova, A.Oppelt Zeuthen, 22.09.2015 Transformer Ratio (TR) Bunches with symmetric current profile drive pulse witness pulse
More informationTTF and VUV-FEL Injector Commissioning
TESLA Collaboration Meeting Sep. 6-8, 2004 Orsay TTF and VUV-FEL Injector Commissioning Siegfried Schreiber, Klaus Floettmann DESY Brief description of the injector Basic measurements Preliminary results
More informationBasic Energy Science Workshop on Future Electron Sources
Basic Energy Science Workshop on Future Electron Sources Workshop Co-Organizers Pietro Musumeci (UCLA) & Xijie Wang (SLAC) DOE BES contact: Eliane Lessner Workshop charge Electron sources represent a critical
More informationTransverse emittance measurements on an S-band photocathode rf electron gun * Abstract
SLAC PUB 8963 LCLS-01-06 October 2001 Transverse emittance measurements on an S-band photocathode rf electron gun * J.F. Schmerge, P.R. Bolton, J.E. Clendenin, F.-J. Decker, D.H. Dowell, S.M. Gierman,
More informationPhase space measurements with tomographic reconstruction at PITZ.
Phase space measurements with tomographic reconstruction at PITZ. > PITZ Photo-Injector Test facility @ DESY in Zeuthen > Emittance measurements at PITZ > Tomographic reconstruction with 2 quadrupoles
More informationX-band Photoinjector Beam Dynamics
X-band Photoinjector Beam Dynamics Feng Zhou SLAC Other contributors: C. Adolphsen, Y. Ding, Z. Li, T. Raubenheimer, and A. Vlieks, Thank Ji Qiang (LBL) for help of using ImpactT code ICFA FLS2010, SLAC,
More informationLinac optimisation for the New Light Source
Linac optimisation for the New Light Source NLS source requirements Electron beam requirements for seeded cascade harmonic generation LINAC optimisation (2BC vs 3 BC) CSR issues energy chirp issues jitter
More informationPhoto Injector Test facility at DESY, Zeuthen site.
Photo Injector Test facility at DESY, Zeuthen site. Update on THz studies at PITZ Tunable IR/THz source based on PITZ-like accelerator for pump probe experiments at the European XFEL Mikhail Krasilnikov
More informationEmittance and Quantum Efficiency Measurements from a 1.6 cell S- Band Photocathode RF Gun with Mg Cathode *
LCLS-TN-4-3 SLAC PUB 763 September, 4 Emittance and Quantum Efficiency Measurements from a.6 cell S- Band Photocathode RF Gun with Mg Cathode * J.F. Schmerge, J.M. Castro, J.E. Clendenin, D.H. Dowell,
More informationMULTI-DIMENSIONAL FREE-ELECTRON LASER SIMULATION CODES: A COMPARISON STUDY *
SLAC-PUB-9729 April 2003 Presented at 21st International Conference on Free Electron Laser and 6th FEL Applications Workshop (FEL 99, Hamburg, Germany, 23-28 Aug 1999. MULTI-DIMENSIONAL FREE-ELECT LASER
More informationEllipsoidal Laser Status & Results Introduction Laser system & on-table data Results Redesign Outlook
Ellipsoidal Laser Status & Results Introduction Laser system & on-table data Results Redesign Outlook James Good PITZ Collaboration Meeting 14 Jun 2017 Introduction > Motivation: Further improvement of
More informationLongitudinal Measurements at the SLAC Gun Test Facility*
SLAC-PUB-9541 September Longitudinal Measurements at the SLAC Gun Test Facility* D. H. Dowell, P. R. Bolton, J.E. Clendenin, P. Emma, S.M. Gierman, C.G. Limborg, B.F. Murphy, J.F. Schmerge Stanford Linear
More informationOptimum 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 informationDESY/TEMF Meeting Status 2012
DESY/TEMF Meeting Status 2012 PIC Simulation for the Electron Source of PITZ DESY, Hamburg, 17.12.2012 Ye Chen, Erion Gjonaj, Wolfgang Müller,Thomas Weiland Technische Universität Darmstadt, Computational
More informationHigh average current photo injector (PHIN) for the CLIC Test Facility at CERN
High average current photo injector (PHIN) for the CLIC Test Facility at CERN CLIC and CTF3 motivation Photo injectors, PHIN Emittance measurements Long pulse operation, time resolved measurements Cathode
More informationFemto-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 informationMicrobunching 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 informationTHE LCLS-II INJECTOR DESIGN*
THE LCLS-II INJECTOR DESIGN* J.F. Schmerge #, A. Brachmann, D. Dowell, A. Fry, R.K. Li, Z. Li, T. Raubenheimer, T. Vecchione, F. Zhou, SLAC, Menlo Park, CA 94025, USA A. Bartnik, I. Bazarov, B. Dunham,
More informationElectron Linear Accelerators & Free-Electron Lasers
Electron Linear Accelerators & Free-Electron Lasers Bryant Garcia Wednesday, July 13 2016. SASS Summer Seminar Bryant Garcia Linacs & FELs 1 of 24 Light Sources Why? Synchrotron Radiation discovered in
More informationDeveloping an Eletron source for the XFEL -
Developing an Eletron source for the XFEL - the Photo Injector Test Facility at Zeuthen, PITZ Introduction, Motivation & Parameters Examples of International Experimental Results on Photo Injector Developments
More informationHigh Gradient Tests of Dielectric Wakefield Accelerating Structures
High Gradient Tests of Dielectric Wakefield Accelerating Structures John G. Power, Sergey Antipov, Manoel Conde, Felipe Franchini, Wei Gai, Feng Gao, Chunguang Jing, Richard Konecny, Wanming Liu, Jidong
More informationSimulations for photoinjectors C.Limborg
Simulations for photoinjectors C.Limborg 1- GTF Simulations Parmela modeling improvements Comparison to experimental results: 2ps & 4ps Sensitivity study Plans for future simulations 2- LCLS Injector Simulations
More informationReduction of thermal emittance of rf guns *
SLAC-PUB-884 LCLS TN 99-8 October 1999 Reduction of thermal emittance of rf guns * J. E. Clendenin, T. Kotseroglou, G. A. Mulhollan, D. T. Palmer, and J. F. Schmerge Stanford Linear Accelerator Center,
More informationJuliane 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 informationDevelopment of Cs 2 Te photocathode RF gun system for compact THz SASE-FEL
Development of Cs 2 Te photocathode RF gun system for compact THz SASE-FEL R. Kuroda, H. Ogawa, N. Sei, H. Toyokawa, K. Yagi-Watanabe, M. Yasumoto, M. Koike, K. Yamada, T. Yanagida*, T. Nakajyo*, F. Sakai*
More informationRF-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 informationExperimental Measurements of the ORION Photoinjector Drive Laser Oscillator Subsystem
Experimental Measurements of the ORION Photoinjector Drive Laser Oscillator Subsystem D.T Palmer and R. Akre Laser Issues for Electron RF Photoinjectors October 23-25, 2002 Stanford Linear Accelerator
More informationLow 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 informationAlignment requirement for the SRF cavities of the LCLS-II injector LCLSII-TN /16/2014
Alignment requirement for the SRF cavities of the LCLS-II injector LCLS-II TN-14-16 12/16/2014 R. K. Li, C. Papadopoulos, T. O. Raubenheimer, J. F. Schmerge, and F. Zhou December 16, 2014 LCLSII-TN-14-16
More informationPresent status and future of DC photoemission electron guns for high power, high brightness applications
Present status and future of DC photoemission electron guns for high power, high brightness applications DC photoemission electron guns using GaAs cathodes have been in use to produce polarized electrons
More informationTHERMAL 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 informationAnalysis of Slice Transverse Emittance Evolution in a Photocathode RF Gun. Abstract
SLAC PUB 868 October 7 Analysis of Slice Transverse Emittance Evolution in a Photocathode RF Gun Z. Huang, Y. Ding Stanford Linear Accelerator Center, Stanford, CA 9439 J. Qiang Lawrence Berkeley National
More informationBERLinPro. An ERL Demonstration facility at the HELMHOLTZ ZENTRUM BERLIN
BERLinPro An ERL Demonstration facility at the HELMHOLTZ ZENTRUM BERLIN BERLinPro: ERL demonstration facility to prepare the ground for a few GeV ERL @ Berlin-Adlershof Goal: 100MeV, 100mA beam Small emittance,
More informationFast Simulation of FEL Linacs with Collective Effects. M. Dohlus FLS 2018
Fast Simulation of FEL Linacs with Collective Effects M. Dohlus FLS 2018 A typical X-FEL gun environment photo cathode cavity, solenoid, drift straight cavity, quadrupole, drift dispersive bend, quadrupole,
More informationExperimental Path to Echo-75 at NLCTA
Experimental Path to Echo-75 at NLCTA Erik Hemsing on behalf of the ECHO group at SLAC NLCTA ICFA Workshop on Future Light Sources March 5-9, 2012 Thomas Jefferson National Accelerator Facility Motivation
More informationBunch Separation with Reconance Island Buckets
Bunch Separation with Reconance Island Buckets P.Goslawski, J.Feikes, T.Goetsch, J.Li, M.Ries, M.Ruprecht, A.Schälicke, G.Wüstefeld and the BESSY VSR design team Helmholtz-Zentrum Berlin November 26th,
More informationFLASH/DESY, Hamburg. Jörg Rossbach University of Hamburg & DESY, Germany - For the FLASH Team -
First Lasing below 7nm Wavelength at FLASH/DESY, Hamburg Jörg Rossbach University of Hamburg & DESY, Germany - For the FLASH Team - email: joerg.rossbach@desy.de FLASH: The first FEL user facility for
More informationICFA ERL Workshop Jefferson Laboratory March 19-23, 2005 Working Group 1 summary Ilan Ben-Zvi & Ivan Bazarov
ICFA ERL Workshop Jefferson Laboratory March 19-23, 2005 Working Group 1 summary Ilan Ben-Zvi & Ivan Bazarov Sincere thanks to all WG1 participants: Largest group, very active participation. This summary
More informationNew Electron Source for Energy Recovery Linacs
New Electron Source for Energy Recovery Linacs Ivan Bazarov 20m Cornell s photoinjector: world s brightest electron source 1 Outline Uses of high brightness electron beams Physics of brightness High brightness
More informationEmittance Compensation. J.B. Rosenzweig ERL Workshop, Jefferson Lab 3/20/05
Emittance Compensation J.B. Rosenzweig ERL Workshop, Jefferson Lab 3//5 Emittance minimization in the RF photoinjector Thermal emittance limit Small transverse beam size Avoid metal cathodes? " n,th #
More informationNormal-conducting RF Photo Injectors for Free Electron Lasers
Normal-conducting RF Photo Injectors for Free Electron Lasers Frank Stephan (DESY, Zeuthen site) for the PITZ team Content: Introduction: FELs and their electron sources Different NC photo injectors at
More informationPhotoinjector design for the LCLS
SLAC-PUB-8962 LCLS-TN-01-05 Revised November 2001 Photoinjector design for the LCLS P.R. Bolton a, J.E. Clendenin a, D.H. Dowell a, M. Ferrario b, A.S. Fisher a, S.M. Gierman a, R.E. Kirby a, P. Krejcik
More informationOVERVIEW OF FEL INJECTORS
OVERVIEW OF FEL INJECTORS M. Ferrario, INFN-LNF, Frascati, Italy Abstract Future light sources based on high gain free electron lasers, require the production, acceleration and transport up to the undulator
More informationEmittance 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 informationBeam Dynamics and SASE Simulations for XFEL. Igor Zagorodnov DESY
Beam Dynamics and SASE Simulations for XFEL Igor Zagorodnov 4.. DESY Beam dynamics simulations for the European XFEL Full 3D simulation method ( CPU, ~ hours) Gun LH M, M,3 E = 3 MeV E = 7 MeV E 3 = 4
More informationSPARCLAB. Source For Plasma Accelerators and Radiation Compton. On behalf of SPARCLAB collaboration
SPARCLAB Source For Plasma Accelerators and Radiation Compton with Laser And Beam On behalf of SPARCLAB collaboration EMITTANCE X X X X X X X X 2 BRIGHTNESS (electrons) B n 2I nx ny A m 2 rad 2 The current
More informationInjector 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 informationX-ray Free-electron Lasers
X-ray Free-electron Lasers Ultra-fast Dynamic Imaging of Matter II Ischia, Italy, 4/30-5/3/ 2009 Claudio Pellegrini UCLA Department of Physics and Astronomy Outline 1. Present status of X-ray free-electron
More informationPresent status and future of DC photoemission electron guns for high power, high brightness applications
Present status and future of DC photoemission electron guns for high power, high brightness applications DC photoemission electron guns using GaAs cathodes have been in use to produce polarized electrons
More informationarxiv: v2 [physics.acc-ph] 10 Aug 2012
DARK CURRENT STUDIES FOR SWISSFEL arxiv:125.398v2 [physics.acc-ph] 1 Aug 212 Abstract F. Le Pimpec, R. Zennaro, S. Reiche, E. Hohmann, A. Citterio, A. Adelmann Paul Scherrer Institut, 5232 Villigen, Switzerland
More informationDesign of Electron Gun
Design of Abhay Deshpande Scientist, Medical ics Division Society for Applied Microwave ics Engineering and Research SAMEER, IIT-B Campus, Powai Mumbai 400 076 abhay@sameer.gov.in Introduction of SAMEER
More information