Emission-related Activities at PITZ Proposals for the DFG-Networking "Hi 2 PE"

Size: px
Start display at page:

Download "Emission-related Activities at PITZ Proposals for the DFG-Networking "Hi 2 PE""

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

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 information

Selected Beam Studies at PITZ in 2017

Selected 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 information

Beam 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 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 information

Dark current at the Euro-XFEL

Dark 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 information

Photo Injector Test facility at DESY, Zeuthen site

Photo 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 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

Dark 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 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 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

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

Numerical modelling of photoemission for the PITZ photoinjector

Numerical 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 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

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

SwissFEL INJECTOR DESIGN: AN AUTOMATIC PROCEDURE

SwissFEL 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 information

Introduction to the benchmark problem

Introduction 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 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

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

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

ASTRA 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 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 information

Tomographic transverse phase space measurements at PITZ.

Tomographic 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 information

1. Beam based alignment Laser alignment Solenoid alignment 2. Dark current 3. Thermal emittance

1. 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 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

Photo Injector Test facility at DESY, Zeuthen site. PITZ: facility overview

Photo 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 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

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

High brightness beam science

High 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 information

Accelerator Activities at PITZ

Accelerator 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 information

Introduction. Thermoionic gun vs RF photo gun Magnetic compression vs Velocity bunching. Probe beam design options

Introduction. 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 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

Studies 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 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 information

RF Gun Photo-Emission Model for Metal Cathodes Including Time Dependent Emission

RF 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 information

Towards a Low Emittance X-ray FEL at PSI

Towards 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 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

Development of reliable and sophisticated photo injector system and future plan

Development 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 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

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

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

Overview of FEL injectors

Overview 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 information

Photo Injector Test facility at DESY, Zeuthen site.

Photo 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 information

Jlab FEL Photoemission DC Guns

Jlab 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 information

DESY/TEMF Meeting - Status 2011

DESY/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 information

AREAL. 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 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 information

START-TO-END SIMULATIONS FOR IR/THZ UNDULATOR RADIATION AT PITZ

START-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 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

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

Tomography module for transverse phase-space measurements at PITZ.

Tomography 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 information

Current Status of Bunch Emission Simulation for the PITZ Gun

Current 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 information

AREAL Test Facility for Advanced Accelerator and Radiation Sources Concepts

AREAL 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 information

CsK 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 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 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

Simulations for a bunch compressor at PITZ Study of high transformer ratios

Simulations 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 information

TTF and VUV-FEL Injector Commissioning

TTF 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 information

Basic Energy Science Workshop on Future Electron Sources

Basic 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 information

Transverse emittance measurements on an S-band photocathode rf electron gun * Abstract

Transverse 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 information

Phase space measurements with tomographic reconstruction at PITZ.

Phase 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 information

X-band Photoinjector Beam Dynamics

X-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 information

Linac optimisation for the New Light Source

Linac 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 information

Photo Injector Test facility at DESY, Zeuthen site.

Photo 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 information

Emittance and Quantum Efficiency Measurements from a 1.6 cell S- Band Photocathode RF Gun with Mg Cathode *

Emittance 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 information

MULTI-DIMENSIONAL FREE-ELECTRON LASER SIMULATION CODES: A COMPARISON STUDY *

MULTI-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 information

Ellipsoidal 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 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 information

Longitudinal Measurements at the SLAC Gun Test Facility*

Longitudinal 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 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

DESY/TEMF Meeting Status 2012

DESY/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 information

High 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 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 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

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

THE LCLS-II INJECTOR DESIGN*

THE 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 information

Electron Linear Accelerators & Free-Electron Lasers

Electron 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 information

Developing an Eletron source for the XFEL -

Developing 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 information

High Gradient Tests of Dielectric Wakefield Accelerating Structures

High 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 information

Simulations for photoinjectors C.Limborg

Simulations 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 information

Reduction of thermal emittance of rf guns *

Reduction 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 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

Development 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 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 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

Experimental Measurements of the ORION Photoinjector Drive Laser Oscillator Subsystem

Experimental 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 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

Alignment 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 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 information

Present 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 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 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

Analysis of Slice Transverse Emittance Evolution in a Photocathode RF Gun. Abstract

Analysis 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 information

BERLinPro. An ERL Demonstration facility at the HELMHOLTZ ZENTRUM BERLIN

BERLinPro. 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 information

Fast Simulation of FEL Linacs with Collective Effects. M. Dohlus FLS 2018

Fast 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 information

Experimental Path to Echo-75 at NLCTA

Experimental 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 information

Bunch Separation with Reconance Island Buckets

Bunch 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 information

FLASH/DESY, Hamburg. Jörg Rossbach University of Hamburg & DESY, Germany - For the FLASH Team -

FLASH/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 information

ICFA 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 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 information

New Electron Source for Energy Recovery Linacs

New 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 information

Emittance Compensation. J.B. Rosenzweig ERL Workshop, Jefferson Lab 3/20/05

Emittance 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 information

Normal-conducting RF Photo Injectors for Free Electron Lasers

Normal-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 information

Photoinjector design for the LCLS

Photoinjector 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 information

OVERVIEW OF FEL INJECTORS

OVERVIEW 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 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

Beam Dynamics and SASE Simulations for XFEL. Igor Zagorodnov DESY

Beam 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 information

SPARCLAB. Source For Plasma Accelerators and Radiation Compton. On behalf of SPARCLAB collaboration

SPARCLAB. 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 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

X-ray Free-electron Lasers

X-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 information

Present 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 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 information

arxiv: v2 [physics.acc-ph] 10 Aug 2012

arxiv: 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 information

Design of Electron Gun

Design 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