Ideas for medium and long term facility upgrade Roberto Corsini for the CLIC Accelerator Collaboration.

Slides:



Advertisements
Similar presentations
Tessa Charles Australian Synchrotron / Monash University 1 Bunch Compression Schemes for X-band FELs.
Advertisements

Chris Tennant Jefferson Laboratory March 15, 2013 “Workshop to Explore Physics Opportunities with Intense, Polarized Electron Beams up to 300 MeV”
Frank Tecker - BE/OP for the CTF3 Team IWLC 2010, Frank Tecker Critical Review of CTF3 performance Introduction Beam phase Improved operation.
1 Enhancements to the Linac Coherent Light Source.
E. Bong, SLACLCLS FAC Meeting - April 29, 2004 Linac Overview E. Bong LCLS FAC Meeting April 29, 2004 LCLS.
R. Corsini, CLIC Project Meeting - 24 th May 2013 CTF3 1 CTF3: Highlights of the 1 st run R. Corsini for the CTF3 Team 1.
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.
AWAKE electron source New Electron Source WP at CERN
7.8GHz Dielectric Loaded High Power Generation And Extraction F. Gao, M. E. Conde, W. Gai, C. Jing, R. Konecny, W. Liu, J. G. Power, T. Wong and Z. Yusof.
Test Stands Roger Ruber Uppsala University ESS TAC4 16 Feb
R&D proposals for EuCard 2 EuCard2, April 21Steffen Döbert, BE-RF  SRF basic research (W. Weingarten)  CTF3 and CTF3+, possible infra - structure for.
CTF3 photo injector laser status CERN 17 July 2009 CLIC meeting.
Low Emittance RF Gun Developments for PAL-XFEL
IWLC - 21st october 2010Califes CTF3 probe beam - Wilfrid Farabolini1 CTF3 Probe Beam Status 1.
TBL as a 12 GHz power source, overview and first results from commissioning IWLC 2010 workshopSteffen Döbert, BE-RF  Current status of TBL  Status of.
PSB C04 RF system Consolidation or upgrade? M. Paoluzzi – CERN BE-RF 11/23/20151.
W.S. Graves ASAC Review Sept 18-19, 2003 R&D at Bates William S. Graves MIT-Bates Laboratory Presentation to MIT X-ray laser Accelerator Science Advisory.
R. Corsini, CLIC Project Meeting October 24, 2012 CTF3 Experimental program for end 2012 R. Corsini for the CTF3 Team 1.
1 Plan and Opportunities for Migration and Integration of the Photoinjector into New Muon Lab Mike Church AAC Review - 12/5/06.
FLASH II. The results from FLASH II tests Sven Ackermann FEL seminar Hamburg, April 23 th, 2013.
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.
CLIC08 workshop CLIC module layout and main requirements G. Riddone, on behalf of the CMWG Home page of the TBM WG:
12 GHz Stand alone power source at CERN G.McMonagle AB/RF.
The SPS as a Damping Ring Test Facility for CLIC March 6 th, 2013 Yannis PAPAPHILIPPOU CERN CLIC Collaboration Working meeting.
LHC-CC Validity Requirements & Tests LHC Crab Cavity Mini Workshop at CERN; 21. August Remarks on using the LHC as a test bed for R&D equipment.
Electron Sources for ERLs – Requirements and First Ideas Andrew Burrill FLS 2012 “The workshop is intended to discuss technologies appropriate for a next.
LINAC4 and the Upgrade of the LHC Injector Complex R. Garoby 26 February, 2013.
Erik Adli CLIC Project Meeting, CERN, CH 1 Erik Adli Department of Physics, University of Oslo, Norway Input from: Steffen Doebert, Wilfried Farabolini,
The Next Generation Light Source Test Facility at Daresbury Jim Clarke ASTeC, STFC Daresbury Laboratory Ultra Bright Electron Sources Workshop, Daresbury,
Valery Telnov Budker INP, Novosibirsk IWLC2010, CERN October 21, 2010 A FEL pumped solid state laser system for the photon collider at CLIC.
S. Bettoni, R. Corsini, A. Vivoli (CERN) CLIC drive beam injector design.
김 귀년 CHEP, KNU Accelerator Activities in Korea for ILC.
Awake electron beam requirements ParameterBaseline Phase 2Range to check Beam Energy16 MeV MeV Energy spread (  ) 0.5 %< 0.5 % ? Bunch Length (
Drive Beam Injector Drive Beam Accelerator X 2 Delay Loop X 5 Combiner Ring Two-beam Test Area 3.5 A  s 150 MeV 35 A ns 150 MeV 150 MV/m 30.
C/S band RF deflector for post interaction longitudinal phase space optimization (D. Alesini)
European Advanced Accelerator Concepts Workshop, Elba, September 14 th -18 th, 2015Steffen Döbert, BE-RF Electron accelerator for the AWAKE experiment.
X-band Based FEL proposal
CLIC DB injector facility, photo-injector option studies LCWS, Granada, September 26 th -30 th,2011Steffen Döbert, BE-RF  CLIC DB injector  Thermionic.
Bunch Shaping for Future Dielectric Wakefield Accelerators W. Gai Mini-Workshop on Deflecting/Crabbing RF Cavity Research and application in Accelerators.
AWAKE Run 2 : 1) Interstage considerations 2) CALIFES as plasma technology test facility Erik Adli and Carl A. Lindstrøm University of Oslo, Norway AWAKE.
11th February th CTF3 Committee - Wilfrid Farabolini1 Status and progress of the CTF3 probe beam 1.
TBL experimental program, evolution to RF power testing in TBL ACE 2011, February 2-3Steffen Döbert, BE-RF  Current status of TBL  Experimental program.
CALIFES A proposed electron beam test facility at CERN
Multi-bunch Operation for LCLS, LCLS_II, LCLS_2025
Beam dynamics for an X-band LINAC driving a 1 keV FEL
Abstract EuSPARC and EuPRAXIA projects
Input to Strategy currently planned
Uppsala Commitment to ESS and FREIA Planning
An X-band system for phase space linearisation on CLARA
CLEX* Status and Plans CTF3 complex CLEX
Status and Interest of the X-ray FEL SINAP
Have a chance to operate your own beam at CERN
Timing and synchronization at SPARC
Application of the moderate peak power (6 MW) X-band klystron’s cluster for the CLIC accelerating structures testing program. I. Syratchev.
WP11: electron and proton beam testing
EuPRAXIA working package report
How to run ions in the future?
Instrumentation CALIFES ideal for tests and development that requires frequent access to test setup. CERN BI members already using CALIFES and want to.
CLIC Drive Beam Klystron Modulators
Cost Comparison of Undulator and e-Driven Systems
F. Villa Laboratori Nazionali di Frascati - LNF On behalf of Sparc_lab
ATF 120 Hz Photocathode RF Gun Injection System Design Studies
SLAC ARD Test Facilities
LCLS Commissioning Parameters
Advanced Research Electron Accelerator Laboratory
SLHC-PP kick-off meeting, CERN 9 April 2008
Explanation of the Basic Principles and Goals
CLIC Feasibility Demonstration at CTF3
Proposal for Smith-Purcell radiation experiment at SPARC_LAB
Presentation transcript:

Ideas for medium and long term facility upgrade Roberto Corsini for the CLIC Accelerator Collaboration

Short term upgrade Present Future: CALIFES minimum upgrade configuration RF deflector Test Area Spectrometer Add an available S-band klystron + modulator (N.B.: present one goes to AWAKE!) More RF power (beam energy), more operational flexibility (power in 1st structure, phase in structures 2 and 3), shorter bunches, possibility of running without RF pulse compression Option: use another S-band klystron + modulator to power existing RF deflector (bunch length measurements) Reconfigure present TBM area as test area Most (all) hardware already existing

Present CALIFES RF network Building 2010 CLEX 2009-2016

RF Upgrade KLYSTRONS AND MODULATORS 1st FLOOR G. McMonagle Building 2001 Building 2010 Implementation of Klystrons and Modulators in CTF3 Building 2013 MKS 30 Implementation of Klystrons and Modulators in CTF3 KLYSTRONS AND MODULATORS 1st FLOOR BUILDINGS 2001, 2013 and 2010

RF upgrade – present status MKS 30 Existing CALIFES set up 5 Hz repetition rate MKS30 will be transferred to AWAKE G. McMonagle

RF Upgrade – constraints & options Some modulators will not be supported by TE-EPC and BE-CO next year What can be reused for CALIFES to give more flexible performance and higher energy if necessary? 1st step: use compatible modulators in existing position, no upgrade for rep rate 2nd optional step: rep rate upgrade, optimize position Other considerations to be taken into account Main water cooling station must be kept operational Two water temperature stabilization stations to be kept operational Pulse compressor temperature control station to be operational Low Level RF and high power RF (klystrons) spares available from the other CTF3 modulators G. McMonagle

RF upgrade – proposal G. McMonagle

RF upgrade – proposal G. McMonagle

By using suggested modulators No support from TE-EPC needed for high power RF Removes incompatibility with future controls interface Using MKS31 all in place just waveguide configuration to change Most waveguides are available somewhere in the CTF3 facility Using MKS07 Modification of waveguide configuration Movement of charging supplies, PLC etc. from MKS 11, cabling costs manpower Keeps all CALIFES modulators in buildings 2010 and building 2013 Using MKS11 (instead of 07) Just waveguide modifications But modulator situated in building 2001 Using MKS30 area Transfer solid state modulator 21 from building 2001 to building 2010, allows 50Hz rep rate for structure testing. Waveguide modifications G. McMonagle

Other upgrades (or consolidation issues) Driven by: Experimental needs (assessment to be done after workshop – need information!) Practical considerations (reliability and availability, ease of maintenance, running cost…) Driven by experimental requirements I, beam parameter improvements: Shorter bunches Higher charge per bunch Higher total charge / longer trains Smaller emittance Higher rep rate Higher beam energy Driven by experimental requirements II, operational Pump and probe capability (independent tuning of time/position of two or more bunches) X-band RF power Available space for experiments Multiple beam lines Timing, synchronization, others

Beam parameters, wish list Bunch length 100 fs range most users Charge per bunch up to 5 nC THz, beam loading Train length 200 ns range beam loading Emittance < 1um plasma Energy up to 500 MeV Synchrotron rad down to 5-10 MeV VESPER Rep rate 25 Hz X-band Double bunch impedance, plasma Pulse shaping plasma, X-FEL … to be completed

CALIFES laser issues Issues: long (70 m) optical transfer line (pointing instability, power losses, aberrations) Photoinjector laser lab (1st floor) and optical transfer line to PHIN and CALIFES Front End Harmonic- generation Amplifier CALIFES PHIN Issues: quite complex no turn-key system, not optimized to CALIFES (new) needs. Maintenance/spares to be checked.

CALIFES laser Today’s CALIFES setup Pulse-picker with step size >1 bunch Today’s CALIFES setup

CALIFES laser, issues and upgrades Laser pulse shape Pointing instability Curtesy of W. Farabolini Curtesy of W. Farabolini Consider to: Move laser lab closer to CALIFES gun Simplify/consolidate present system Change laser to new one (commercial?) Others… Need input on parameters (pulse length, rep rate, stability, pulse shaping)

Laser upgrades Many applications need/would prefer improved laser parameters, e.g.: Shorter pulses (< 1 ps) Bunch comb (16 bunches…) Pulse shaping Higher power/pulse Consider also the possibility of double pulse with tunable distance Some proposed applications would need a different dedicated laser system Other don’t strictly need it, but may profit Need to understand parameters range, cost, infrastructure, manpower and maintenance needs, as well as potential synergies

X band capability - BOX1 connection Availability of X-band high power RF is an asset for CALIFES XBOX1 obvious choice Actually feed CTF2 test area and/or Dogleg beam loading experiment Low-loss RF line may be readapted and moved Alternative: move XBOX1 on top of desired location XBOX1 Low-loss RF transfer Drive beam, 1-3A, 100-50 MeV  50 mm circular waveguide CTF2 test area Dogleg experiment

Space availability The present CALIFES beam line is quite crowded. Even completely dismantling the Two-Beam Module, only a few meters will be available for equipment May sacrifice matching sections, instrumentation, spectrometers, but… Need to understand space requirements, typical times for installation and turnaround, compatibility, synergies Option: second beam line

Space availability

Options for a second beam line In CLEX there’s plenty of (transverse) space for a 2nd beam line (and possibly a 3rd one as well) Plenty of hardware to recuperate Dogleg can be used for compression Longitudinal space still limited May consider to extend towards CTF2

New source/gun Pump and probe experiments (Plasma, THz, impedance) would profit from a second independent electron source. A new source can also be optimized for short bunches and low emittance, beyond reach of the present CALIFES gun. A new source would not only be a tool, but an R&D goal in itself Some attractive possibilities: X-band photoinjector, plasma-based source Possible synergy with AWAKE (100 fs, ~ 400 A peak current, 50 MeV) See Steffen’s talk

Options for a second beam line + source 2nd line (alternative) New source Test area CALIFES 2nd line CLEX