FLASH II: an Overview

Size: px
Start display at page:

Download "FLASH II: an Overview"

Transcription

1 FLASH II: an Overview 1. Layout. 2. Status 1. Civil Construction 2. E-beamline 3. Photon Beamline 3. Timeplan 4. Finances 5. Personnel Situation 6. Simultaneous Operation of FLASH1 and 2 FLASH II is a combined proposal of HZB and DESY. It has been approved in Summer 2010: total Budget 29.6 M Euro. Bart Faatz FLASH II: an Overview Hamburg, September 25, 2012

2 Why FLASH II. Problem 1. FLASH is overbooked by a factor SASE principle is intrinsically unstable. 1. Time arrival jitter (partially corrected by fast feedback within pulse train). 2. Shot-to-shot fluctuation in intensity (starting from noise). 3. Wavelength variation/mode structure (coherence length versus bunch length). 3. FLASH delivers only linear polarization. Solution 1. Doubling number of experimental stations (simultaneous operation?). 2. Make an amplifier (stability/availability of seeding?). 1. HHG 2. HGHG 3. Use variable polarization undulators (Tolerances/alignment). Bart Faatz WA Page 2

3 Upgrade: layout after upgrade FLASH II. Separation FLASH and FLASH II behind last accelerator module Tunability of FLASH II by undulator gap change Extend user capacity with SASE and HHG seeding Use of existing infrastructure up to last accelerating module Gun ACC1+ACC39 ACC2&3 ACC4,5,6,7 Up to ~1.25 GeV sflash SASE ~ nm EXP. Hall 1 st BC 2 nd BC HHG Seed laser FLASH II SASE/HHG Variable gap undulator FLASH II Bart Faatz WA Page 3

4 FLASH II: Electron beam parameters. Beam parameters Beam Energy (1.6) GeV Normalized emittance (proj.) mm mrad Energy spread 0.5 MeV Peak Current 2.5 ka Bunches per second <8000 Bunch Charge nc Undulator parameters Period 31.4 mm Segments length 2.5 m Number of segments 12 Focusing Structure F0D0 Bart Faatz WA Page 4

5 Wavelength range for main energies by varyang the undulator gap mm period mm period 50 Wavelength (nm) GeV 1.00 GeV 1.25 GeV Undulator gap (mm) Wavelength (nm) Wavelength (nm) Energy (GeV) GeV GeV 1.00 GeV 1.25 GeV 22.0 mm period mm Undulator gap (mm) Undulator gap (mm) nm at 0.7 GeV with HHG seeding >40 nm with energies below 0.7 GeV Bart Faatz WA Page 5

6 Civil Construction: status September Tunnel ready for technical infrastructure (MKK): Delivery complete Tunnel: March 2013 Delivery Hall: May 2013 MKK building Seed Laser Controlled access 2x in main tunnel 1x in extraction area (separated from FLASH1) Bart Faatz WA Page 6

7 FL2SEED: Ready for cleaning end of september. Mostly temporary beamline HHG scheduled for Autumn 2014 Additional seeding options under discussion Bart Faatz WA Page 7

8 Vacuum in the SEED Section. Bart Faatz WA Page 8

9 FL2SASE: Ready for cleaning end of september. Undulators not shown Bart Faatz WA Page 9

10 Vacuum in the SASE Section. Bart Faatz WA Page 10

11 FL2EXTR: Vacuum Design ready and partially ordered. Status: critical (FLASH Shutdown needed) Priority 1. rebuild FLASH1 (~10 m) 2. add Extraction in prohibited area Bart Faatz WA Page 11

12 FL2BURN/FL2DUMP: Ready for cleaning end of september. Two supports still missing Some vacuum components not yet ready THz Undulator Project funded (N. Stojanovic) Expected in the next 3 years Bart Faatz WA Page 12

13 Photon Diagnostics Tunnel. Proposed Version of Tunnel Diagnostics Bart Faatz WA Page 13

14 Photon Diagnostics Tunnel: minimal Version. Proposed Version of Tunnel Diagnostics for July/Aug Compact Spectrometer Safety magnet Alignment laser Aperture 1 Absorber/V0 1 st differential pumping station MCP Aperture 2 YAG Absorber Bart Faatz WA Page 14

15 Tentative FLASH time schedule Jan Feb Mar Apr May Jun Jul Aug Sep Oct Nov Dec FLASH2 Tunnel Infrastructure Technical Commissioning (incl. Interlocks, Magnets) Commissioning with beam Electron beamline Undulators Photon diagnostics (Tunnel) Restarbeiten Electron beamline FLASH2 Extraction Connection FLASH1+2 Electron beamline (incl. infrastructure) Technical Commissioning (incl. Interlocks, Magnets) Commissioning with beam FLASH1 Connection FLASH1+2 Modification electron beamline (incl. Infrastructure) Commissioning with beam Accelerator and FEL Studies User run FLASH Shutdown Technical Commissioning (incl. Interlocks, Magnets) User run Experimental Hall Civil construction (incl. Infrastructure) K. Honkavaara: Bart Faatz WA Page 15

16 Tentative FLASH time schedule > Discussions ongoing TGA main tunnel until TGA MKK Building until TGA Elektronikabseite until Will be modified and discussed in detail in 2 weeks Priority on Abseite Nord : contains all personeninterlock crates for complete FLASH > FLASH1 Startup Interlock tests mid June Startup with beam first half of July Start user run beginning of October > FLASH2 Startup Technical commissioning beginning of May With beam 2 nd half of August First lasing 2 nd half of 2013 (first photon diagnostics Tunnel July/Aug. 2013) Pilot experiments starting mid-2014 Bart Faatz WA Page 16

17 Finances: Original Group Sum Bau Machine Exp Sum With HGHG, reduced undulator length Components from the Bypass Bart Faatz WA Page 17

18 Finances: Present Situation. Group Sum Bau Machine Exp Sum Full Undulator Length Synchronization system Higher demands climatization Civil Construction 3 GU 3 construction sites Improve quality soil/surface General increase in prices.. Bart Faatz WA Page 18

19 Personnel Situation. FS 2011 (2010 = 1) 2011 hatte nur FS-US Personalkosten M 2011 (2010 = 0) Aktivitätsbezeichng Kostenst. unbefristet Befristet Grand Total FLASHII Maschine MEA MDI MKK MKK MKK MKK FLASHII Maschine Total Group befristet unbefristet Sum BT 1.3 TI 0.5 US 3.5 FL ZM1: H. Damker working for FLASH II ZM3: 75% outside of DESY Group unbefristet befristet Sum MDI MEA MKK MVS? MPY? Bart Faatz WA Page 19

20 FTEs FLASH II: Annual (assume construction start 2012) Group SUM FSUS (Undulator) FSBT (HASY Vacuum) HASYLAB (HALL) F MCS MDI (Diagnostics) MEA (Magnets, drawings,..) MIN (laser, kicker, dump) MKK MKS (change He 47A) MPS MPY (Simulations) MVS (Machine Vacuum) M ZBAU (Tunnel/Hall Preparation) ZM (construction Extraction) Z Based on discussion with group leaders and Bereichsleitung Numbers for M are those needed in addition Bart Faatz WA Page 20

21 Lasing at FLASH. RF-Gun FLASH Accelerator FLASH1 Fixed Gap Undulators 5 MeV 150 MeV 450 MeV 1250 MeV > Pulse trains delivered at 10 Hz > Parameter changes requested by users Different wavelength different optics and RF settings Fine-tuning wavelength changes in dogleg and RF settings Different pulse length (=charges:p nc) different RF settings and focusing Different number of bunches ( max) different laser settings Different rep.rates (50, 100, 200, 250, 500, 1000 khz) different laser settings Different position/angle Orbit correction Small spectral width dispersion/orbit correction and????? Nice spot on YAG-screen????? Bart Faatz WA Page 21

22 Lasing of FLASH1 and FLASH2 Simultaneously RF-Gun FLASH Accelerator FLASH1 Fixed Gap Undulators 5 MeV 150 MeV 450 MeV 1250 MeV > Both running at 10 Hz fast kicker system with DC septum > Parameter changes requested by users Different wavelength different undulator gap (within limits) Different charges ( nc) different RF settings within an RF pulse Different number of bunches ( max) different laser Different rep.rates (50, 100, 200, 250, 500, 1000 khz) different laser Tunability > factor 3 Bart Faatz WA Page 22

23 Beamline switching (FLASH1 and 2/3). Within 1 RF pulse part to FLASH1 and part to FLASH2/3 800 s 99 ms 800 s 99 ms 800 s 99 ms 800 s t Requirements: Pulser/Kicker Stability to avoid orbit jitter. Flatness for long pulse trains. Rise or Fall time of <50 s. Switch length and starting point variable. 1 st part or 2 nd to FLASH2 depends on need of BAM FB without interference of background bunches Laser(s) Different repetition rates and charges. Switching to gun in <50 s at different start time (related to kicker). LLRF Different beam loading FLASH1 and 2/3. Tunability of gradient or ACC45 and ACC67 for wavelength scans FLASH1. Tunability in phases of Gun, ACC1, ACC39 and ACC23 for variation in compression FLASH1, 2 and 3. Bart Faatz WA Page 23

24 Charge dependence: 700 MeV, 0.3 nc and 0.07 nc Bart Faatz WA Page 24

25 Charge dependence: Measurements at 0.7 (solid) and 1.08 GeV (open symbols) 800 Bunch length in fs (FWHM) Bunch Length in m (FWHM) Charge (nc) SASE ( GeV SASE ( GeV / /55 35 Charge (pc) Measurement: 1. Start with HIGH charge and go down, touching only RF parameters and orbit 2. Optimize at low charge 3. Start with LOW charge and go down, touching only RF parameters and orbit Bart Faatz WA Page 25

26 Outlook. Schedule on critical path. Implementation of FLASH3 extraction postponed. Implementation of HHG Seeding postponed to 2014 (?) Construction FLASH1/FLASH2 Extraction on critical path. Shutdown needed of FLASH1. Priority at ZM may be needed for FLASH II beginning Already external personnel hired. Already 75% of hardware from outside DESY. Different works at the same time unavoidable. Necessity for more crews at the same time become likely. Because of delays conflict with XFEL and PETRA III more likely. ~14 FTE for commissioning needed in 2nd half of Only minimal version of control system will be working (?) User Operation in 2014 only without seeding thinkable. Bart Faatz WA Page 26

FLASH at DESY. FLASH. Free-Electron Laser in Hamburg. The first soft X-ray FEL operating two undulator beamlines simultaneously

FLASH at DESY. FLASH. Free-Electron Laser in Hamburg. The first soft X-ray FEL operating two undulator beamlines simultaneously FLASH at DESY The first soft X-ray FEL operating two undulator beamlines simultaneously Katja Honkavaara, DESY for the FLASH team FEL Conference 2014, Basel 25-29 August, 2014 First Lasing FLASH2 > First

More information

FLASH II. FLASH II: a second undulator line and future test bed for FEL development.

FLASH II. FLASH II: a second undulator line and future test bed for FEL development. FLASH II FLASH II: a second undulator line and future test bed for FEL development Bart.Faatz@desy.de Outline Proposal Background Parameters Layout Chalenges Timeline Cost estimate Personnel requirements

More information

FLASH 2. FEL seminar. Charge: 0.5 nc. Juliane Rönsch-Schulenburg Overview of FLASH 2 Hamburg,

FLASH 2. FEL seminar. Charge: 0.5 nc. Juliane Rönsch-Schulenburg Overview of FLASH 2 Hamburg, FLASH 2 FEL seminar Juliane Rönsch-Schulenburg Overview of FLASH 2 Hamburg, 2016-03-22 Charge: 0.5 nc Overview 1. FLASH 2 Overview 1.Layout parameters 2. Operation FLASH2. 1.Lasing at wavelengths between

More information

FLASH: Status and upgrade

FLASH: Status and upgrade : Status and upgrade The User Facility Layout Performance and operational o a issues Upgrade Bart Faatz for the team DESY FEL 2009 Liverpool, UK August 23-28, 2009 at DESY > FEL user facility since summer

More information

FLASH performance after the upgrade. Josef Feldhaus

FLASH performance after the upgrade. Josef Feldhaus FLASH performance after the upgrade Josef Feldhaus European XFEL / HASYLAB Users Meeting DESY, January 27, 2011 Upgrade 2009 / 2010 > Upgrade shutdown: September 2009 February 2010 exchanged RF stations

More information

Demonstration of exponential growth and saturation at VUV wavelengths at the TESLA Test Facility Free-Electron Laser. P. Castro for the TTF-FEL team

Demonstration of exponential growth and saturation at VUV wavelengths at the TESLA Test Facility Free-Electron Laser. P. Castro for the TTF-FEL team Demonstration of exponential growth and saturation at VUV wavelengths at the TESLA Test Facility Free-Electron Laser P. Castro for the TTF-FEL team 100 nm 1 Å FEL radiation TESLA Test Facility at DESY

More information

FLASH Operation at DESY From a Test Accelerator to a User Facility

FLASH Operation at DESY From a Test Accelerator to a User Facility FLASH Operation at DESY From a Test Accelerator to a User Facility Michael Bieler FLASH Operation at DESY WAO2012, SLAC, Aug. 8, 2012 Vocabulary DESY: Deutsches Elektronen-Synchrotron, Hamburg, Germany

More information

THz Pump Beam for LCLS. Henrik Loos. LCLS Hard X-Ray Upgrade Workshop July 29-31, 2009

THz Pump Beam for LCLS. Henrik Loos. LCLS Hard X-Ray Upgrade Workshop July 29-31, 2009 Beam for LCLS Henrik Loos Workshop July 29-31, 29 1 1 Henrik Loos Overview Coherent Radiation Sources Timing THz Source Performance 2 2 Henrik Loos LCLS Layout 6 MeV 135 MeV 25 MeV 4.3 GeV 13.6 GeV σ z.83

More information

3 General layout of the XFEL Facility

3 General layout of the XFEL Facility 3 General layout of the XFEL Facility 3.1 Introduction The present chapter provides an overview of the whole European X-Ray Free-Electron Laser (XFEL) Facility layout, enumerating its main components and

More information

Performance Evaluation of the Upgraded BAMs at FLASH

Performance Evaluation of the Upgraded BAMs at FLASH Performance Evaluation of the Upgraded BAMs at FLASH with a compact overview of the BAM, the interfacing systems & a short outlook for 2019. Marie K. Czwalinna On behalf of the Special Diagnostics team

More information

Status, perspectives, and lessons from FLASH and European XFEL

Status, perspectives, and lessons from FLASH and European XFEL 2014 International Workshop on EUV and Soft X-ray Sources November 3-6, 2014 Dublin, Ireland Status, perspectives, and lessons from FLASH and European XFEL R. Brinkmann, E.A. Schneidmiller, J, Sekutowicz,

More information

SwissFEL Design and Status

SwissFEL Design and Status SwissFEL Design and Status Hans H. Braun Mini Workshop on Compact X ray Free electron Lasers Eastern Forum of Science and Technology Shanghai July 19, 2010 SwissFEL, the next large facility at PSI SwissFEL

More information

LUCX - THZ PROGRAM: OVERVIEW AND PROSPECTS

LUCX - THZ PROGRAM: OVERVIEW AND PROSPECTS LUCX - THZ PROGRAM: OVERVIEW AND PROSPECTS A. Aryshev On behalf of QB group and THz collaboration 14 Outline THz project overview LUCX activity LUCX Projects Overview THz program LUCX Laser system LUCX

More information

Status of the European XFEL Accelerator Construction Project. Reinhard Brinkmann, DESY

Status of the European XFEL Accelerator Construction Project. Reinhard Brinkmann, DESY Status of the European XFEL Accelerator Construction Project Reinhard Brinkmann, DESY European XFEL Introduction Some specifications Photon energy 0.3-24 kev Pulse duration ~ 10-100 fs Pulse energy few

More information

Bioimaging of cells and tissues using accelerator-based sources

Bioimaging of cells and tissues using accelerator-based sources Analytical and Bioanalytical Chemistry Electronic Supplementary Material Bioimaging of cells and tissues using accelerator-based sources Cyril Petibois, Mariangela Cestelli Guidi Main features of Free

More information

Infrared Single Shot Diagnostics for the Longitudinal. Profile of the Electron Bunches at FLASH. Disputation

Infrared Single Shot Diagnostics for the Longitudinal. Profile of the Electron Bunches at FLASH. Disputation Infrared Single Shot Diagnostics for the Longitudinal Profile of the Electron Bunches at FLASH Disputation Hossein Delsim-Hashemi Tuesday 22 July 2008 7/23/2008 2/ 35 Introduction m eb c 2 3 2 γ ω = +

More information

Does the short pulse mode need energy recovery?

Does the short pulse mode need energy recovery? Does the short pulse mode need energy recovery? Rep. rate Beam power @ 5GeV 1nC @ 100MHz 500MW Absolutely 1nC @ 10MHz 1nC @ 1MHz 50MW 5MW Maybe 1nC @ 100kHz 0.5MW No Most applications we have heard about

More information

sflash - FIRST RESULTS OF DIRECT SEEDING AT FLASH

sflash - FIRST RESULTS OF DIRECT SEEDING AT FLASH WEOAI2 Proceedings of FEL2010, Malmö, Sweden sflash - FIRST RESULTS OF DIRECT SEEDING AT FLASH J. Bödewadt,A.Azima,F.Curbis,H.Delsim-Hashemi, M. Drescher, E. Hass, U. Hipp, T. Maltezopoulos, V. Miltchev,

More information

FLASH Upgrade. Decrease wavelength and/or increase brilliance

FLASH Upgrade. Decrease wavelength and/or increase brilliance FLASH Upgrade Far-Infrared (FIR) undulator Medium and long-term issues: Decrease wavelength and/or increase brilliance Enable quasi-simultanous operation at 2 wavelengths Provide more space for users Motivation:

More information

RF-based Synchronization of the Seed and Pump-Probe Lasers to the Optical Synchronization System at FLASH

RF-based Synchronization of the Seed and Pump-Probe Lasers to the Optical Synchronization System at FLASH RF-based Synchronization of the Seed and Pump-Probe Lasers to the Optical Synchronization System at FLASH Introduction to the otical synchronization system and concept of RF generation for locking of Ti:Sapphire

More information

Progress of the TEO experiment at FLASH

Progress of the TEO experiment at FLASH Progress of the TEO experiment at VUV-FEL at DESY - Armin Azima S. Duesterer, J. Feldhaus, H. Schlarb, H. Redlin, B. Steffen, DESY Hamburg K. Sengstock, Uni Hamburg Adrian Cavalieri, David Fritz, David

More information

Undulator K-Parameter Measurements at LCLS

Undulator K-Parameter Measurements at LCLS Undulator K-Parameter Measurements at LCLS J. Welch, A. Brachmann, F-J. Decker, Y. Ding, P. Emma, A. Fisher, J. Frisch, Z. Huang, R. Iverson, H. Loos, H-D. Nuhn, P. Stefan, D. Ratner, J. Turner, J. Wu,

More information

ELECTRON BEAM DIAGNOSTICS AND FEEDBACK FOR THE LCLS-II*

ELECTRON BEAM DIAGNOSTICS AND FEEDBACK FOR THE LCLS-II* THB04 Proceedings of FEL2014, Basel, Switzerland ELECTRON BEAM DIAGNOSTICS AND FEEDBACK FOR THE LCLS-II* Josef Frisch, Paul Emma, Alan Fisher, Patrick Krejcik, Henrik Loos, Timothy Maxwell, Tor Raubenheimer,

More information

VUV-FEL User workshop, August 23-24, 2004

VUV-FEL User workshop, August 23-24, 2004 Layout of the user facility Kai Tiedtke Kai Tiedtke, HASYLAB@ VUV-FEL User workshop, August 23-24, 2004 Kai.Tiedtke@desy.de Kai Tiedtke, HASYLAB@ Outline Photon beam transport Layout of the experimental

More information

INSTALLATION AND FIRST COMMISSIONING OF THE LLRF SYSTEM

INSTALLATION AND FIRST COMMISSIONING OF THE LLRF SYSTEM INSTALLATION AND FIRST COMMISSIONING OF THE LLRF SYSTEM FOR THE EUROPEAN XFEL Julien Branlard, for the LLRF team TALK OVERVIEW 2 Introduction Brief reminder about the XFEL LLRF system Commissioning goals

More information

Calibrating the Cavity Voltage. Presentation of an idea

Calibrating the Cavity Voltage. Presentation of an idea Calibrating the Cavity Voltage. Presentation of an idea Stefan Wilke, DESY MHF-e 21st ESLS rf meeting Kraków, 15th/16th nov 2017 Accelerators at DESY. linear and circular Page 2 Accelerators at DESY. linear

More information

Beam Diagnostics, Low Level RF and Feedback for Room Temperature FELs. Josef Frisch Pohang, March 14, 2011

Beam Diagnostics, Low Level RF and Feedback for Room Temperature FELs. Josef Frisch Pohang, March 14, 2011 Beam Diagnostics, Low Level RF and Feedback for Room Temperature FELs Josef Frisch Pohang, March 14, 2011 Room Temperature / Superconducting Very different pulse structures RT: single bunch or short bursts

More information

FLASH. FLASH Training: RF Gun. FLASH: the first soft X-ray FEL operating two undulator beamlines simultaneously. Siegfried Schreiber, DESY

FLASH. FLASH Training: RF Gun. FLASH: the first soft X-ray FEL operating two undulator beamlines simultaneously. Siegfried Schreiber, DESY FLASH Training: RF Gun FLASH: the first soft X-ray FEL operating two undulator beamlines simultaneously Siegfried Schreiber, DESY FLASH Training DESY 17-Mar-2017 FLASH1 RF Gun History RF Guns operated

More information

Commissioning of the ALICE SRF Systems at Daresbury Laboratory Alan Wheelhouse, ASTeC, STFC Daresbury Laboratory ESLS RF 1 st 2 nd October 2008

Commissioning of the ALICE SRF Systems at Daresbury Laboratory Alan Wheelhouse, ASTeC, STFC Daresbury Laboratory ESLS RF 1 st 2 nd October 2008 Commissioning of the ALICE SRF Systems at Daresbury Laboratory Alan Wheelhouse, ASTeC, STFC Daresbury Laboratory ESLS RF 1 st 2 nd October 2008 Overview ALICE (Accelerators and Lasers In Combined Experiments)

More information

Outline of the proposed JLAMP VUV/soft X-ray FEL and the challenges for the photon beamlines and optics

Outline of the proposed JLAMP VUV/soft X-ray FEL and the challenges for the photon beamlines and optics Outline of the proposed JLAMP VUV/soft X-ray FEL and the challenges for the photon beamlines and optics J. Michael Klopf Jefferson Lab - Free Electron Laser Division Workshop on Future Light Sources SLAC

More information

synchronization system

synchronization system Status of the optical synchronization system Holger Schlarb DESY for the LbSyn team V. Arsov, M. C. Behrens, Bock, P. Gessler, M. Felber, K. Hacker, F. Loehl, F. Ludwig, K-H. Matthiesen, B. Schmidt, S.

More information

Status of the Electron Beam Transverse Diagnostics with Optical Diffraction Radiation at FLASH

Status of the Electron Beam Transverse Diagnostics with Optical Diffraction Radiation at FLASH Status of the Electron Beam Transverse Diagnostics with Optical Diffraction Radiation at FLASH M. Castellano, E. Chiadroni, A. Cianchi, K. Honkavaara, G. Kube DESY FLASH Seminar Hamburg, 05/09/2006 Work

More information

Electro-Optic Longitudinal Bunch Profile Measurements at FLASH: Experiment, Simulation, and Validation

Electro-Optic Longitudinal Bunch Profile Measurements at FLASH: Experiment, Simulation, and Validation Electro-Optic Longitudinal Bunch Profile Measurements at FLASH: Experiment, Simulation, and Validation Bernd Steffen, DESY FEL 2007 Novosibirsk, August 29th 2007 Electro-Optic Bunch Length Detection fs

More information

Drive Beam Photo-injector Option for the CTF3 Nominal Phase

Drive Beam Photo-injector Option for the CTF3 Nominal Phase CTF3 Review Drive Beam Photo-injector Option for the CTF3 Nominal Phase Motivation CTF3 Drive Beam Requirements CTF3 RF gun design The Laser (I. Ross / RAL) The Photocathode Cost estimate Possible schedule

More information

Status of the Project

Status of the Project Status of the FERMI@Elettra Project Michele Svandrlik Elettra, Trieste, Italy IPAC 2012 New Orleans May 22 nd, 2012 OUTLINE FERMI@Elettra Overview Facility Performance Recent Progress Outlook and Conclusions

More information

Commissioning of the FLASH2 Electron Beam Diagnostics in respect to its Use at the European XFEL

Commissioning of the FLASH2 Electron Beam Diagnostics in respect to its Use at the European XFEL FLASH2 Extension of the FLASH Facility Commissioning of the FLASH2 Electron Beam Diagnostics in respect to its Use at the European XFEL N. Baboi, DESY for the Diagnostics Team Contents > FLASH2 New undulator

More information

R&D Toward Brighter X-ray FELs

R&D Toward Brighter X-ray FELs Some R&D Toward Brighter X-ray FELs Zhirong Huang (SLAC) March 6, 2012 FLS2012 Workshop, Jefferson Lab Outline Introduction Seeding for temporal coherence Hard x-rays Soft x-rays Push for higher power

More information

Wisconsin FEL Initiative

Wisconsin FEL Initiative Wisconsin FEL Initiative Joseph Bisognano, Mark Bissen, Robert Bosch, Michael Green, Ken Jacobs, Hartmut Hoechst, Kevin J Kleman, Robert Legg, Ruben Reininger, Ralf Wehlitz, UW-Madison/SRC William Graves,

More information

Feedback Requirements for SASE FELS. Henrik Loos, SLAC IPAC 2010, Kyoto, Japan

Feedback Requirements for SASE FELS. Henrik Loos, SLAC IPAC 2010, Kyoto, Japan Feedback Requirements for SASE FELS Henrik Loos, SLAC, Kyoto, Japan 1 1 Henrik Loos Outline Stability requirements for SASE FELs Diagnostics for beam parameters Transverse: Beam position monitors Longitudinal:

More information

2 TTF/FLASH in the XFEL context

2 TTF/FLASH in the XFEL context 2 TTF/FLASH in the XFEL context 2.1 Historical background In the early 90s, the Tera-Electronvolt Superconducting Linear Accelerator (TESLA) Test Facility (TTF) was established by the international TESLA

More information

New generation Laser amplifier system for FEL applications at DESY.

New generation Laser amplifier system for FEL applications at DESY. New generation Laser amplifier system for FEL applications at DESY. Franz Tavella Helmholtz-Institut-Jena Merging advanced solid-state Laser technology with FEL sources Helmholtz-Institut-Jena DESY F.

More information

Frank Schmidt-Föhre, DESY

Frank Schmidt-Föhre, DESY Commissioning of the New Online- Radiation-Monitoring-System at the New European XFEL Injector with First Tests of the High-Sensitivity-Mode for Intra-Tunnel Rack Surveillance Frank Schmidt-Föhre, DESY

More information

TECHNICAL CHALLENGES OF THE LCLS-II CW X-RAY FEL *

TECHNICAL CHALLENGES OF THE LCLS-II CW X-RAY FEL * TECHNICAL CHALLENGES OF THE LCLS-II CW X-RAY FEL * T.O. Raubenheimer # for the LCLS-II Collaboration, SLAC, Menlo Park, CA 94025, USA Abstract The LCLS-II will be a CW X-ray FEL upgrade to the existing

More information

H. Weise, Deutsches Elektronen-Synchrotron, Hamburg, Germany for the XFEL Group

H. Weise, Deutsches Elektronen-Synchrotron, Hamburg, Germany for the XFEL Group 7+(7(6/$;)(/352-(&7 H. Weise, Deutsches Elektronen-Synchrotron, Hamburg, Germany for the XFEL Group $EVWUDFW The overall layout of the X-Ray FEL to be built in international collaboration at DESY will

More information

arxiv:physics/ v1 [physics.acc-ph] 18 Jul 2003

arxiv:physics/ v1 [physics.acc-ph] 18 Jul 2003 DESY 03 091 ISSN 0418-9833 July 2003 arxiv:physics/0307092v1 [physics.acc-ph] 18 Jul 2003 Two-color FEL amplifier for femtosecond-resolution pump-probe experiments with GW-scale X-ray and optical pulses

More information

Electro-optic Spectral Decoding Measurements at FLASH

Electro-optic Spectral Decoding Measurements at FLASH Electro-optic Spectral Decoding Measurements at FLASH, FLA Florian Loehl, Sebastian Schulz, Laurens Wißmann Motivation Development of a robust online bunch length monitor for FLASH and XFEL Transition

More information

BEAM DIAGNOSTICS AT THE VUV-FEL FACILITY

BEAM DIAGNOSTICS AT THE VUV-FEL FACILITY BEAM DIAGNOSTICS AT THE VUV-FEL FACILITY J. Feldhaus, D. Nölle, DESY, D-22607 Hamburg, Germany Abstract The free electron laser (FEL) at the TESLA Test facility at DESY, now called VUV-FEL, will be the

More information

Low-Level RF. S. Simrock, DESY. MAC mtg, May 05 Stefan Simrock DESY

Low-Level RF. S. Simrock, DESY. MAC mtg, May 05 Stefan Simrock DESY Low-Level RF S. Simrock, DESY Outline Scope of LLRF System Work Breakdown for XFEL LLRF Design for the VUV-FEL Cost, Personpower and Schedule RF Systems for XFEL RF Gun Injector 3rd harmonic cavity Main

More information

Installation Progress of the Laser-based Synchronization System at FLASH.

Installation Progress of the Laser-based Synchronization System at FLASH. Installation Progress of the Laser-based Synchronization System at FLASH. Overview, Experiences, Performance and Outlook Sebastian Schulz 1,2 on behalf of the FLASH LbSyn Team 1 Institute of Experimental

More information

Using Higher Order Modes in the Superconducting TESLA Cavities for Diagnostics at DESY

Using Higher Order Modes in the Superconducting TESLA Cavities for Diagnostics at DESY Using Higher Order Modes in the Superconducting TESLA Cavities for Diagnostics at FLASH @ DESY N. Baboi, DESY, Hamburg for the HOM team : S. Molloy 1, N. Baboi 2, N. Eddy 3, J. Frisch 1, L. Hendrickson

More information

Challenges of Optics for High Repetition Rate XFEL Source

Challenges of Optics for High Repetition Rate XFEL Source Challenges of Optics for High Repetition Rate XFEL Source Liubov Samoylova, European XFEL GmbH ACTOP11, DIAMOND, April 5 th, 2011 2 European XFEL photon transport system - overview X-ray optics for XFEL:

More information

arxiv: v1 [physics.acc-ph] 20 Jan 2010

arxiv: v1 [physics.acc-ph] 20 Jan 2010 DEUTSCHES ELEKTRONEN-SYNCHROTRON Ein Forschungszentrum der Helmholtz-Gemeinschaft DESY 10-004 arxiv:1001.3510v1 [physics.acc-ph] 20 Jan 2010 January 2010 Scheme for femtosecond-resolution pump-probe experiments

More information

Spectral characterization of the FERMI pulses in the presence of electron-beam phase-space modulations

Spectral characterization of the FERMI pulses in the presence of electron-beam phase-space modulations Spectral characterization of the FERMI pulses in the presence of electron-beam phase-space modulations Enrico Allaria, Simone Di Mitri, William M. Fawley, Eugenio Ferrari, Lars Froehlich, Giuseppe Penco,

More information

Supporting Planning and Engineering Processes at XFEL Examples, Benefits and Experience

Supporting Planning and Engineering Processes at XFEL Examples, Benefits and Experience Supporting Planning and Engineering Processes at XFEL Examples, Benefits and Experience Lars Hagge, Benno List SLAC, 31.03.2014 Agenda > Introduction: Collaborative Engineering > Collaborative Design &

More information

Beam Arrival Time Monitors. Josef Frisch, IBIC Sept. 15, 2015

Beam Arrival Time Monitors. Josef Frisch, IBIC Sept. 15, 2015 Beam Arrival Time Monitors Josef Frisch, IBIC Sept. 15, 2015 Arrival Time Monitors Timing is only meaningful relative to some reference, and in general what matters is the relative timing of two different

More information

Performance of the TTF Photoinjector Laser System

Performance of the TTF Photoinjector Laser System Performance of the TTF Photoinjector Laser System S. Schreiber, DESY Laser Issues for Electron Photoinjectors, October 23-25, 22, Stanford, California, USA & I. Will, A. Liero, W. Sandner, MBI Berlin Overview

More information

ALICE SRF SYSTEM COMMISSIONING EXPERIENCE A. Wheelhouse ASTeC, STFC Daresbury Laboratory

ALICE SRF SYSTEM COMMISSIONING EXPERIENCE A. Wheelhouse ASTeC, STFC Daresbury Laboratory ALICE SRF SYSTEM COMMISSIONING EXPERIENCE A. Wheelhouse ASTeC, STFC Daresbury Laboratory ERL 09 8 th 12 th June 2009 ALICE Accelerators and Lasers In Combined Experiments Brief Description ALICE Superconducting

More information

Physics Requirements Document Document Title: SCRF 1.3 GHz Cryomodule Document Number: LCLSII-4.1-PR-0146-R0 Page 1 of 7

Physics Requirements Document Document Title: SCRF 1.3 GHz Cryomodule Document Number: LCLSII-4.1-PR-0146-R0 Page 1 of 7 Document Number: LCLSII-4.1-PR-0146-R0 Page 1 of 7 Document Approval: Originator: Tor Raubenheimer, Physics Support Lead Date Approved Approver: Marc Ross, Cryogenic System Manager Approver: Jose Chan,

More information

Zhirong Huang. May 12, 2011

Zhirong Huang. May 12, 2011 LCLS R&D Program Zhirong Huang May 12, 2011 LCLS 10 10 LCLS-II Light Sou urces at ~1 Å Peak Brightness (phot tons/s/mm 2 /mrad 2 /0.1%-BW) H.-D. Nuhn, H. Winnick storag e rings FWHM X-Ray Pulse Duration

More information

KU-FEL Facility. Status Report. Konstantin Torgasin PhD Student Graduate School of Energy Science Kyoto University

KU-FEL Facility. Status Report. Konstantin Torgasin PhD Student Graduate School of Energy Science Kyoto University KU-FEL Facility Status Report Konstantin Torgasin PhD Student Graduate School of Energy Science Kyoto University KU-FEL(Kyoto University FEL) A mid-infrared free electron laser (MIR-FEL) facility KU-FEL

More information

Participant institutions: other INFN sections (Mi, RM1, RM2, Ba, Ca, Pi, Ts, Fe, Le, Fi, Na, LNS), ENEA-Frascat

Participant institutions: other INFN sections (Mi, RM1, RM2, Ba, Ca, Pi, Ts, Fe, Le, Fi, Na, LNS), ENEA-Frascat The THOMSON SOURCE AT SPARC_LAB C. Vaccarezza (Resp. Naz.), M.P. Anania (Ass. Ric.), M. Bellaveglia (Art. 23), M. Cestelli Guidi (Art. 23), D. Di Giovenale (Art. 23) G. Di Pirro, A. Drago, M. Ferrario,

More information

The ILC Accelerator Complex

The ILC Accelerator Complex The ILC Accelerator Complex Nick Walker DESY/GDE UK LC meeting 3 rd September 2013 Oxford University, UK. 1 ILC in a Nutshell 200-500 GeV E cm e + e - collider L ~2 10 34 cm -2 s -1 upgrade: ~1 TeV central

More information

System Integration of the TPS. J.R. Chen NSRRC, Hsinchu

System Integration of the TPS. J.R. Chen NSRRC, Hsinchu System Integration of the TPS J.R. Chen NSRRC, Hsinchu OUTLINE I. Main features of the TPS II. Major concerns and intersystem effects of an advanced synchrotron light source III. Subsystems and intersystem

More information

Introduction to the Physics of Free-Electron Lasers

Introduction to the Physics of Free-Electron Lasers Introduction to the Physics of Free-Electron Lasers 1 Outline Undulator Radiation Radiation from many particles The FEL Instability Advanced FEL concepts The X-Ray Free-Electron Laser For Angstrom level

More information

The Potential for the Development of the X-Ray Free Electron Laser

The Potential for the Development of the X-Ray Free Electron Laser The Potential for the Development of the X-Ray Free Electron Laser TESLA-FEL 2004-02 E.L. Saldin, E.A. Schneidmiller, and M.V. Yurkov Deutsches Elektronen-Synchrotron (DESY), Notkestrasse 85, Hamburg,

More information

Installation of the Optical Replica Synthesizer (ORS) at FLASH

Installation of the Optical Replica Synthesizer (ORS) at FLASH Installation of the Optical Replica Synthesizer (ORS) at FLASH Who and What? G. Angelova, V. Ziemann- Task: Modulator and radiator undulators, participating in the Theoretical simulations with Genesis

More information

Dark Current Kicker Studies at FLASH

Dark Current Kicker Studies at FLASH Dark Current Kicker Studies at FLASH F. Obier, J. Wortmann, S. Schreiber, W. Decking, K. Flöttmann FLASH Seminar, DESY, 02 Feb 2010 History of the dark current kicker 2005 Vertical kicker was installed

More information

LLRF Operation and Performance of the European XFEL. An overview

LLRF Operation and Performance of the European XFEL. An overview LLRF Operation and Performance of the European XFEL. An overview Mathieu Omet LLRF, Barcelona, 16.10.2017 Contents > Introduction > LLRF commissioning > Energy Reach > LLRF performance > Summary / Outlook

More information

CEBAF Overview June 4, 2010

CEBAF Overview June 4, 2010 CEBAF Overview June 4, 2010 Yan Wang Deputy Group Leader of the Operations Group Outline CEBAF Timeline Machine Overview Injector Linear Accelerators Recirculation Arcs Extraction Systems Beam Specifications

More information

Borut Baricevic. Libera LLRF. 17 September 2009

Borut Baricevic. Libera LLRF. 17 September 2009 Borut Baricevic Libera LLRF borut.baricevic@i-tech.si 17 September 2009 Outline Libera LLRF introduction Libera LLRF system topology Signal processing structure GUI and signal acquisition RF system diagnostics

More information

Photon Diagnostics. FLASH User Workshop 08.

Photon Diagnostics. FLASH User Workshop 08. Photon Diagnostics FLASH User Workshop 08 Kai.Tiedtke@desy.de Outline What kind of diagnostic tools do user need to make efficient use of FLASH? intensity (New GMD) beam position intensity profile on the

More information

Extreme Light Infrastucture (ELI) Science and Technology at the ultra-intense Frontier. Bruno Le Garrec

Extreme Light Infrastucture (ELI) Science and Technology at the ultra-intense Frontier. Bruno Le Garrec SPIE Photonics West 2.2.2014 Extreme Light Infrastucture (ELI) Science and Technology at the ultra-intense Frontier Bruno Le Garrec bruno.legarrec@eli-beams.eu On behalf of Georg Korn, Bedrich Rus and

More information

LCLS-II-HE Instrumentation

LCLS-II-HE Instrumentation LCLS-II-HE Instrumentation Average Brightness (ph/s/mm 2 /mrad 2 /0.1%BW) LCLS-II-HE: Enabling New Experimental Capabilities Structural Dynamics at the Atomic Scale Expand the photon energy reach of LCLS-II

More information

Shintake Monitor Nanometer Beam Size Measurement and Beam Tuning

Shintake Monitor Nanometer Beam Size Measurement and Beam Tuning Shintake Monitor Nanometer Beam Size Measurement and Beam Tuning Technology and Instrumentation in Particle Physics 2011 Chicago, June 11 Jacqueline Yan, M.Oroku, Y. Yamaguchi T. Yamanaka, Y. Kamiya, T.

More information

INTRA-TRAIN LONGITUDINAL FEEDBACK FOR BEAM STABILIZATION AT FLASH

INTRA-TRAIN LONGITUDINAL FEEDBACK FOR BEAM STABILIZATION AT FLASH INTRA-TRAIN LONGITUDINAL FEEDBACK FOR BEAM STABILIZATION AT FLASH W. Koprek*, C. Behrens, M. K. Bock, M. Felber, P. Gessler, K. Hacker, H. Schlarb, C. Schmidt, B. Steffen, S. Wesch, DESY, Hamburg, Germany

More information

Spectral Phase Modulation and chirped pulse amplification in High Gain Harmonic Generation

Spectral Phase Modulation and chirped pulse amplification in High Gain Harmonic Generation Spectral Phase Modulation and chirped pulse amplification in High Gain Harmonic Generation Z. Wu, H. Loos, Y. Shen, B. Sheehy, E. D. Johnson, S. Krinsky, J. B. Murphy, T. Shaftan,, X.-J. Wang, L. H. Yu,

More information

OVERVIEW OF SEEDING METHODS FOR FELS

OVERVIEW OF SEEDING METHODS FOR FELS OVERVIEW OF SEEDING METHODS FOR FELS S. Reiche Paul Scherrer Institut, Villigen PSI, 5232, Switzerland Abstract In recent years enormous progress has been achieved in the theoretical understanding and

More information

Femtosecond-stability delivery of synchronized RFsignals to the klystron gallery over 1-km optical fibers

Femtosecond-stability delivery of synchronized RFsignals to the klystron gallery over 1-km optical fibers FEL 2014 August 28, 2014 THB03 Femtosecond-stability delivery of synchronized RFsignals to the klystron gallery over 1-km optical fibers Kwangyun Jung 1, Jiseok Lim 1, Junho Shin 1, Heewon Yang 1, Heung-Sik

More information

Note on the LCLS Laser Heater Review Report

Note on the LCLS Laser Heater Review Report Note on the LCLS Laser Heater Review Report P. Emma, Z. Huang, C. Limborg, J. Schmerge, J. Wu April 15, 2004 1 Introduction This note compiles some initial thoughts and studies motivated by the LCLS laser

More information

Grounding for EMC at the European XFEL

Grounding for EMC at the European XFEL Grounding for EMC at the European XFEL Herbert Kapitza, Hans-Jörg Eckoldt, Markus Faesing Deutsches Elektronensynchrotron (DESY) D-22603 Hamburg, Germany Email: herbert.kapitza@desy.de Abstract The European

More information

ERL based FELs. Todd I Smith Hansen Experimental Physics Laboratories (HEPL) Stanford University Stanford, CA

ERL based FELs. Todd I Smith Hansen Experimental Physics Laboratories (HEPL) Stanford University Stanford, CA ERL based FELs Todd I Smith Hansen Experimental Physics Laboratories (HEPL) Stanford University Stanford, CA 94305-4085 Todd.Smith@Stanford.edu Electrostatic ERL-FELs University of California Santa Barbara

More information

Engineering Challenges and Solutions for MeRHIC. Andrew Burrill for the MeRHIC Team

Engineering Challenges and Solutions for MeRHIC. Andrew Burrill for the MeRHIC Team Engineering Challenges and Solutions for MeRHIC Andrew Burrill for the MeRHIC Team Key Components Photoinjector Design Photocathodes & Drive Laser Linac Cavities 703.75 MHz 5 cell cavities 3 rd Harmonic

More information

Acceleration of High-Intensity Protons in the J-PARC Synchrotrons. KEK/J-PARC M. Yoshii

Acceleration of High-Intensity Protons in the J-PARC Synchrotrons. KEK/J-PARC M. Yoshii Acceleration of High-Intensity Protons in the J-PARC Synchrotrons KEK/J-PARC M. Yoshii Introduction 1. J-PARC consists of 400 MeV Linac, 3 GeV Rapid Cycling Synchrotron (RCS) and 50 GeV Main synchrotron

More information

LUSI Pulse Picker System

LUSI Pulse Picker System ENGINEERING SPECIFICATION DOCUMENT (ESD) Doc. No. SP-391-001-50 R0 LUSI SUB-SYSTEM DCO LUSI Pulse Picker System Rick Jackson Design Engineer, Author Signature Date Marc Campell DCO Design Engineer Signature

More information

Available online at ScienceDirect. Physics Procedia 84 (2016 )

Available online at  ScienceDirect. Physics Procedia 84 (2016 ) Available online at www.sciencedirect.com ScienceDirect Physics Procedia 84 (2016 ) 8 112 International Conference "Synchrotron and Free electron laser Radiation: generation and application", SFR-2016,

More information

Status of the APEX Project at LBNL

Status of the APEX Project at LBNL at LBNL Fernando Sannibale K. Baptiste, B. Bailey, D. Colomb, C. Cork, J. Corlett, S. De Santis, J. Feng, D. Filippetto, G.Huang, R. Kraft, S. Kwiatkowski, D. Li, M. Messerly, R. Muller, W. E. Norum, H.

More information

EMMA the World's First Non-Scaling FFAG Accelerator

EMMA the World's First Non-Scaling FFAG Accelerator EMMA the World's First Non-Scaling FFAG Accelerator Susan Smith STFC Daresbury Laboratory CONTENTS Introduction Contents What are ns-ffags? and Why EMMA? The international collaboration EMMA goals and

More information

CLARA: A new particle accelerator test facility for the UK

CLARA: A new particle accelerator test facility for the UK CLARA: A new particle accelerator test facility for the UK Jim Clarke STFC Daresbury Laboratory and The Cockcroft Institute on behalf of the CLARA & VELA Project Teams RHUL Particle Physics Seminar, 25

More information

R. Assmann, CERN/AB. for the Collimation Project 7/12/2007 LHC MAC RWA, LHC MAC 12/07

R. Assmann, CERN/AB. for the Collimation Project 7/12/2007 LHC MAC RWA, LHC MAC 12/07 Plan for Collimator Commissioning R. Assmann, CERN/AB 7/12/2007 for the Collimation Project LHC MAC RWA, LHC MAC 12/07 1) Installation Planning and Performance Reach Collimation is an performance-driven

More information

COMMISSIONING STATUS AND FURTHER DEVELOPMENT OF THE NOVOSIBIRSK MULTITURN ERL*

COMMISSIONING STATUS AND FURTHER DEVELOPMENT OF THE NOVOSIBIRSK MULTITURN ERL* COMMISSIONING STATUS AND FURTHER DEVELOPMENT OF THE NOVOSIBIRSK MULTITURN ERL* O.A.Shevchenko #, V.S.Arbuzov, E.N.Dementyev, B.A.Dovzhenko, Ya.V.Getmanov, E.I.Gorniker, B.A.Knyazev, E.I.Kolobanov, A.A.Kondakov,

More information

A high resolution bunch arrival time monitor system for FLASH / XFEL

A high resolution bunch arrival time monitor system for FLASH / XFEL A high resolution bunch arrival time monitor system for FLASH / XFEL K. Hacker, F. Löhl, F. Ludwig, K.H. Matthiesen, H. Schlarb, B. Schmidt, A. Winter October 24 th Principle of the arrival time detection

More information

LEAPS Accelerator Domain Technology Roadmap

LEAPS Accelerator Domain Technology Roadmap LEAPS Accelerator Domain Technology Roadmap Andreas Jankowiak Head Institute for Accelerator Physics Helmholtz-Zentrum Berlin RULe (WP7) Topical Workshop Injection & Injections Systems 30.08.2017 1 LEAPS

More information

Timing Issues for the BESSY Femtoslicing Source

Timing Issues for the BESSY Femtoslicing Source ICFA Workshop on Future Light Sources, Hamburg, May 15-19th, 2006 Timing Issues for the BESSY Femtoslicing Source Shaukat Khan, University of Hamburg R. Mitzner, University of Münster T. Quast, BESSY/Berlin

More information

Plan for Accelerator Beam Study Towards J-PARC Muon Project. Koji YOSHIMURA (KEK) for KEK Muon Working Group at NuFACT08 July 2nd, 2008

Plan for Accelerator Beam Study Towards J-PARC Muon Project. Koji YOSHIMURA (KEK) for KEK Muon Working Group at NuFACT08 July 2nd, 2008 Plan for Accelerator Beam Study Towards J-PARC Muon Project Koji YOSHIMURA (KEK) for KEK Muon Working Group at NuFACT08 July 2nd, 2008 Contents Introduction Muon Project at J-PARC Beam Requirements R&D

More information

Development of utca Hardware for BAM system at FLASH and XFEL

Development of utca Hardware for BAM system at FLASH and XFEL Development of utca Hardware for BAM system at FLASH and XFEL Samer Bou Habib, Dominik Sikora Insitute of Electronic Systems Warsaw University of Technology Warsaw, Poland Jaroslaw Szewinski, Stefan Korolczuk

More information

Commissioning the Echo-Seeding Experiment ECHO-7 at NLCTA

Commissioning the Echo-Seeding Experiment ECHO-7 at NLCTA Commissioning the Echo-Seeding Experiment ECHO-7 at NLCTA Stephen Weathersby for the ECHO-7 team D. Xiang, E. Colby, M. Dunning, S. Gilevich, C. Hast, K. Jobe, D. McCormick, J. Nelson, T.O. Raubenheimer,

More information

Light at the FLASH FIR beamline second coming. DESY.DE

Light at the FLASH FIR beamline second coming. DESY.DE Light at the FLASH FIR beamline second coming Michael.Gensch @ DESY.DE Status of the beamline Comissioning Next Steps 2 FIR beamline commissioning: Motivation timeschedule as presented to PSC in 09/2007

More information

Laser systems for science instruments

Laser systems for science instruments European XFEL Users Meeting 27-20 January 2016, Main Auditorium (Bldg. 5), DESY, Hamburg Laser systems for science instruments M. J. Lederer WP78, European XFEL GmbH, Albert-Einstein-Ring 19, 22761 Hamburg,

More information

Single Bunch Impurity Measurement at SPring-8 8 Storage Ring

Single Bunch Impurity Measurement at SPring-8 8 Storage Ring Single Bunch Impurity Measurement at SPring-8 8 Storage Ring Kazuhiro TAMURA (JASRI/SPring-8) 1 Outlilne Overview of SPring-8 accelerator complex operation modes Bunch Purity Monitor light shutter system

More information

THE ORION PHOTOINJECTOR: STATUS and RESULTS

THE ORION PHOTOINJECTOR: STATUS and RESULTS THE ORION PHOTOINJECTOR: STATUS and RESULTS Dennis T. Palmer SLAC / ARDB ICFA Sardinia 4 July 2002 1. Introduction 2. Beam Dynamics Simulations 3. Photoinjector 1. RF Gun 2. Solenoidal Magnet 3. Diagnostics

More information