Beam Dynamic Shifts 2011 C. Behrens, W. Decking, M. Dohlus, H. & D. Edwards, C. Gerth, T. Hellert, T. Limberg, P. Piot, E. Schneidmiller, M. Scholz, M.

Slides:



Advertisements
Similar presentations
FEL Beam Dynami cs FEL Beam Dynamics T. Limberg Short Bunches at FLASH.
Advertisements

Nominal and no CSR (R 56-1 = 55 mm, R 56-2 = 59 mm, R 56-3 = 0) L1 phase = 21 deg, V 3.9 = 55 MV CSR OFF BC3 OFF Elegant Tracking  z1 = mm (post.
BC System – Review Options ● BC2 working point (energy-charge-compr.) ● 2BC (rf-rf-bc-rf-bc-rf) ● table: 2BC (rf-rf-bc-rf-bc-rf) dogleg + 2BC (rf-dog-rf-rf-bc-rf-bc-rf)
Bunch Compressor 3 Torsten Limberg for Frank Stulle et al.
1 Bates XFEL Linac and Bunch Compressor Dynamics 1. Linac Layout and General Beam Parameter 2. Bunch Compressor –System Details (RF, Magnet Chicane) –Linear.
First operation of the TTF2 injector with beam Jean-Paul Carneiro DESY Hamburg TESLA COLLABORATION MEETING DESY Hamburg, 16 Sept 2003.
LOLA Measurements vs. Beam Dynamics Simulations Igor Zagorodnov DESY.
RF Tweak 5 Tool for FLASH and XFEL
E. Schneidmiller and M. Yurkov (SASE & MCP) C. Behrens, W. Decking, H. Delsim, T. Limberg, R. Kammering (rf & LOLA) N. Guerassimova and R. Treusch (PGM.
Cecile Limborg-Deprey Injector Commissioning September Injector Commissioning Plans C.Limborg-Deprey Gun exit measurements.
CTF3 commissioning status R. Corsini - CTF3 committee 17 th September 2009 Update on CTF3 Operations and schedule This time I will try to give a more complete.
ESS DTL beam commissioning
FEL Beam Dynami cs FEL Beam Dynamics T. Limberg FEL driver linac operation with very short electron bunches.
Steve LidiaICFA Workshop, Chia LagunaJuly, 2002 Flat Beam Photoinjectors for Ultrafast Synchrotron Radiation Sources Steve Lidia Lawrence Berkeley National.
Low Emittance RF Gun Developments for PAL-XFEL
TTF2 Start-to-End Simulations Jean-Paul Carneiro DESY Hamburg TESLA COLLABORATION MEETING DESY Zeuthen, 22 Jan 2004.
Yauhen Kot Current Status of XFEL Simulations.
Recent Experiments at PITZ ICFA Future Light Sources Sub-Panel Mini Workshop on Start-to-End Simulations of X-RAY FELs August 18-22, 2003 at DESY-Zeuthen,
Two Longitudinal Space Charge Amplifiers and a Poisson Solver for Periodic Micro Structures Longitudinal Space Charge Amplifier 1: Longitudinal Space Charge.
FLASH II. The results from FLASH II tests Sven Ackermann FEL seminar Hamburg, April 23 th, 2013.
Beam Dynamics and FEL Simulations for FLASH Igor Zagorodnov and Martin Dohlus Beam Dynamics Meeting, DESY.
SFLASH  SASE interference setup & optics rough estimation 1d estimation 3d estimation summary.
A bunch compressor design and several X-band FELs Yipeng Sun, ARD/SLAC , LCLS-II meeting.
CLARA Gun Cavity Optimisation NVEC 05/06/2014 P. Goudket G. Burt, L. Cowie, J. McKenzie, B. Militsyn.
Beam Dynamics Meeting Bolko Beutner, DESY Summary of new FLASH CSR studies Bolko Beutner, DESY Beam Dynamics Meeting
XFEL Beam Dynamics Meeting Bolko Beutner, DESY Velocity Bunching Studies at FLASH Bolko Beutner, DESY XFEL Beam Dynamics Meeting
T. Limberg Position of the 3rd Harmonic System. Injector (with first Bunch Compression Stage) 2 European XFEL MAC May 2010 T. Limberg.
3D codes: TraFiC4 and CSRtrack Torsten Limberg DESY Zeuthen 2003.
‘S2E’ Study of Linac for TESLA XFEL P. Emma SLAC  Tracking  Comparison to LCLS  Re-optimization  Tolerances  Jitter  CSR Effects.
S2E (start-to-end) Simulations at DESY T. Limberg TESLA Collaboration Meeting in Frascati, May 2003.
Twin bunches at FACET-II Zhen Zhang, Zhirong Huang, Ago Marinelli … FACET-II accelerator physics workshop Oct. 12, 2015.
Round-to-Flat Beam Transformation and Applications
What did we learn from TTF1 FEL? P. Castro (DESY).
Operational experience and recent results from FLASH (VUV FEL at DESY) E. Saldin, E. Schneidmiller and M. Yurkov for FLASH team Milestones Parameters of.
XFEL Beam Dynamics Meeting Bolko Beutner, DESY First results of micro-bunching and COTR experiments at FLASH Bolko Beutner, Winfried Decking,
SL_THOMSON C. Vaccarezza on behalf of the SL_Thomson team.
PAL-XFEL Commissioning Plan ver. 1.1, August 2015 PAL-XFEL Beam Dynamics Group.
A single-shot method for measuring fs bunches in linac-based FELs Z. Huang, K. Bane, Y. Ding, P. Emma.
B. Marchetti R. Assmann, U. Dorda, J. Grebenyuk, Y. Nie, J. Zhu Acknowledgements: C. Behrens, R. Brinkmann, K. Flöttmann, M. Hüning,
Bunch Shaping for Future Dielectric Wakefield Accelerators W. Gai Mini-Workshop on Deflecting/Crabbing RF Cavity Research and application in Accelerators.
Minjie Yan Ch. Gerth, E. Hass Deutsches Elektronen-Synchrotron (DESY)
Eduard Prat / Sven Reiche :: Paul Scherrer Institute
Sara Thorin, MAX IV Laboratory
Slice Parameter Measurements at the SwissFEL Injector Test Facility
Tunable Electron Bunch Train Generation at Tsinghua University
Longitudinal Diagnostics for start-up
Beyond the RF photogun Jom Luiten Seth Brussaard
Review of Application to SASE-FELs
F. Villa Laboratori Nazionali di Frascati - LNF On behalf of Sparc_lab
XFEL Bunch Compression System Tuning
MON TUE WED THU
OBSERVATION OF FEMTOSECOND BUNCH LENGTH USING A TRANSVERSELY DEFLECTING STRUCTURE Markus Hüning*, Andy Bolzmann, Holger Schlarb (DESY, Hamburg), Josef.
Simulation Calculations
Advanced Research Electron Accelerator Laboratory
Z. Huang LCLS Lehman Review May 14, 2009
Sun Mon Tue Wed Thu Fri Sat
Linac/BC1 Commissioning P
Modified Beam Parameter Range
Sun Mon Tue Wed Thu Fri Sat
Linac Physics, Diagnostics, and Commissioning Strategy P
First results of micro-bunching and COTR experiments at FLASH
COMB beam: TSTEP simulations up to THz station
1/○~1/○ weekly schedule MON TUE WED THU FRI SAT SUN MEMO
2016 | 10 OCT SUN MON TUE WED THU FRI SAT
Sun Mon Tue Wed Thu Fri Sat
Introduction to Free Electron Lasers Zhirong Huang
Review of the European XFEL Bunch Compression System: Introduction and Concept Torsten Limberg.
Bunch Compression Experiment in VUV-FEL BC3
New VUV-FEL Simulation results
S2E Meeting on Yauhen Kot.
Presentation transcript:

Beam Dynamic Shifts 2011 C. Behrens, W. Decking, M. Dohlus, H. & D. Edwards, C. Gerth, T. Hellert, T. Limberg, P. Piot, E. Schneidmiller, M. Scholz, M. Vogt, S. Wesch, M. Yurkov, I. Zagorodnov

Schedule ShiftPerson in ScheduleSubjectComments Sun Jan 16 nP. Piot (12h)Linearly ramped current profile done Mon Jan 17 nP. Piot (12h)Linearly ramped current profile done Tue Jan 18 nP. Piot (12h)Linearly ramped current profile Wed Jan 19 aB. FaatzSASE tuningE. Schneidmiller: Set-up for different charges Wed Jan 19 nC. BehrensLong. Phase space vs. SASE LOLA studies, SASE vs. bunch given charge

ShiftPerson in ScheduleSubjectComments Thu Jan 20 m 7-11SASE Characterization (Bunch length etc.) M. Yurkov Thu Jan 20 m 11-3TL/WD (4 h)Optics and Beam-DEmittance and optics measurement, Dog-leg dispersion measurement and adjustment Thu Jan 20 aTLBC StudiesImpact of dog-leg on LOLA profile and SASE Thu Jan 20 nC. BehrensLong. Phase space vs. SASE Fri Jan 21 mSASE Characterization (Bunch length etc.) M. Yurkov

ShiftPerson in ScheduleSubjectComments Fri Jan 21 mTL/WD (4 h)Optics and Beam-DOrbit response, ACC1 beam dynamic Fri Jan 21 aTLBC StudiesVary ACC567 energy, observe LOLA Fri Jan 21 nC. BehrensLong. Phase space vs. SASE Sat Jan 22 m 7-11Contingency SASE characterization M. Yurkov Sat Jan 22 nC. BehrensLong. Phase space vs. SASE

Generation of electron bunches with linearly-ramped current profile ACC39 gradient limit was increased to ~21-22 MV; we decrease the BC2 energy to 140 MeV With this setup could produce linearly-ramped bunches with two type of slopes (rising and falling) starting from setup devised from rftweak and a tracking code from M. Dohlus. We demonstrated the tunability of the ramp steepness and associated peak current (max peak current was of the order of 1 kA). We collected data for compression in BC2 only (BC3 R56 decreased to 15 mm) and with some compression in BC3 (BC3 `R56~32 mm)

Peak current vs. emittance

3 rd Shift * CTR bunch spectra were taken for different bunch profiles. Thanks for parasitic measurements! (S.Wesch) * Linearly-ramped current profile for different charges and iris settings taken * Laser attenuator was broken => temporarily 2-nd installed (taken from Laser 1) by Sebastian Schulz (one of the few down times)

SASE tuning (E. Schneidmiller) Set on crest phases for ACC23, ACC45 to zero 225 uJ (GMD-B, 10/10 mm) at 14.6 nm for 5 bunches, 1 MHz, 1 nC 210 uJ for 0.5 nC 35 uJ for 0.25 nC 1 uJ for 0.1 nC Change between these 4 regimes is done with the help of very few knobs (pyro BC2 target, solenoid, launch steerers)

Electron bunch characterization We recovered all of Evgeny's SASE WP with the same level of SASE. In two directions, going from 1nC to 0.1nC and back again from 0.1nC to 1nC.! We measured long. phase space and THz spectra for all SASE WP and took a lot of data for post-analysis. The rms values for bunch lenghts are between 60 and 110fs, but looking into the long. phase space, much shorter lasing parts can be expected! As expected the long. phase space and finally SASE is pretty sensitive to phase variations of the order of 0.1deg. The measurements resp. the behavior of the long. phase on the 0.1deg phase variations match with first simple simulations we did in the control room. 3 x LOLA time resolution record: 11fs, 9fs, and finally 8fs.

The other direction: Before and after SASE optimization

Q3ECOL Scan (here: 118 A and 121 A)

Performed studies of bunch shape vs. rf acc1/acc39 knob settings.

Optics and transverse beam dynamics Response matrix data taking Commissioned emittance measurement data taking for both ORS screen sections.