Brief review of past studies on Wakefield ATF2 Proj. Mtg. 201502 K.Kubo.

Slides:



Advertisements
Similar presentations
Emittance dilution due to misalignment of quads and cavities of ILC main linac revised K.Kubo For beam energy 250 GeV,
Advertisements

Emittance dilution due to misalignment of quads and cavities of ILC main linac K.Kubo For beam energy 250 GeV, TESLA-type optics for 24MV/m.
Summary of the discussion for the commissioning session 2 nd ATF2 Project Meeting KEK, Tsukuba, Japan 6/ 1/ 2006 T.Okugi (KEK)
Update of EXT Stripline BPM Electronics with LCLS-style Digital BPM Processors Glen White, with slides by Steve Smith 15 December 2009 ATF2.
Testing and Development of Feed-Forward System for ATF2 A. Kalinin Accelerator Science and Technology Centre, Daresbury Laboratory, UK Fifth ATF2 Project.
Main Linac Simulation - Main Linac Alignment Tolerances - From single bunch effect ILC-MDIR Workshop Kiyoshi KUBO References: TESLA TDR ILC-TRC-2.
Effects of wake fields in ATF2 low aperture kicker and IP nano-BPMs Karl Bane April 19, 2005.
Crab cavity location for 2-mrad x-ing December 7, 2004 A.S.
1 M. Woods, SLACMDI SLAC WORKSHOP Machine-Detector Interface at the International Linear Collider Jan. 6-8, 2005SLAC Introduction to Topic of.
Feed forward orbit corrections for the CLIC RTML R. Apsimon, A. Latina.
-brief report of October runs and some inputs for the Nov/Dec planning – Nobuhiro Terunuma, KEK, ATF ATF session on LCWS13, Tokyo Univ., Nov. 13, 2013.
Simulation of IP beam size with orbit jitter + wakefield in EXT-FF ATF2 Project Meeting K.Kubo.
ATF2 Progress Report For CLIC Workshop Kiyoshi KUBO.
Analysis of ATF EXT/FF Orbit Jitter and extrapolation to IP (Data of ) ATF2 Project Meeting K. Kubo.
ATF2 Status and Plan K. Kubo ATF2, Final Focus Test for LC Achievement of 37 nm beam size (Goal 1) – Demonstration of a compact final focus.
F Specifications for the dark current kicker for the NML test facility at Fermilab S. Nagaitsev, M. Church, P. Piot, C.Y. Tan, J. Steimel Fermilab May.
1.Beam Tuning Simulation 2.IP Beam Position Stability 2-1 ) Magnet Vibration 2-2 ) IP position jitter subtraction for 2 nd bunch with FONT feedback 2-3.
Salzau M. Körfer, DESY 1 Layout and Functionality of Collimator System Purpose of the Collimator System Layout Sub-Systems Transversal/ Energy.
Direct Wakefield measurement of CLIC accelerating structure in FACET Hao Zha, Andrea Latina, Alexej Grudiev (CERN) 28-Jan
ATF2 Javier Resta Lopez (JAI, Oxford University) for the FONT project group 5th ATF2 project meeting, KEK December 19-21, 2007.
Personal strategy for ATF2 beam operation in 2009 Toshiyuki OKUGI 2009 / 7 /22 ATF2 weekly meeting.
Influence of the Third Harmonic Module on the Beam Size Maria Kuhn University of Hamburg Bachelor Thesis Presentation.
BPM Orbit Data Analysis with Wakefields Glen White, SLAC January 2013.
17 th ATF2 Collaboration Meeting Summary Glen White, SLAC Feb 14, 2014.
Beam dynamics on damping rings and beam-beam interaction Dec 포항 가속기 연구소 김 은 산.
Continuous Run in May K.Kubo. Final Focus Test Line IP; ~40 nm beam ATF Linac (1.3 GeV) ATF Damping Ring (140 m) Extraction Line Photo-cathode.
ATF2 beam commissioning status and beam time request Toshiyuki Okugi 2008 / 11 / 12 ATF2 Commissioning Meeting.
Commissioning Status of Shintake Monitor (IP-BSM) T. Yamanaka, M. Oroku, Y. Yamaguchi, Y. Kamiya, S. Komamiya (Univ. of Tokyo), T. Okugi, N. Terunuma,
Wakefield Calculations for the ATF2 Beamline A. Lyapin, Wakefield Calculations for the ATF2 Beamline 1 S. Boogert, J. Snuverink (JAI/RHUL, UK)
ILC Beam Delivery System / MDI Issues for LCC-phase (~
Rough Estimation of energy spread produced in Final Focus line and effects to chromatic correction in ILC and ATF minor change Kiyoshi.
ATF2 Kiyoshi KUBO Accelerator Test Facility (ATF) at KEK ATF – Designed as a prototype of damping ring and injector of LC – Achieved low vertical.
IPBSM response to non-Gaussian beam K. KUBO.
Results on recent technology developments at ATF - Beam extraction study by a Fast Kicker - N. Terunuma, KEK LER11, Heraklion, Crete, Greece, 2011/Oct/5.
Plan in summer shutdown Magnet -SF1FF -Swap of QEA magnet - Multipole field of Final Doublet IP-BSM improvement.
J. Pfingstner, LCWS13 Jitter and ground motion studies November 13, 2013 Beam jitter at ATF2: A. Source localisation and B. Ground motion correlation Jürgen.
Multibunch beam stability in damping ring (Proposal of multibunch operation week in October) K. Kubo.
Collimator design and short range wakefields Adriana Bungau University of Manchester CERN, Dec 2006.
Beam stability in damping ring - for stable extracted beam for ATF K. Kubo.
Beam Delivery System collimators J. L. Fernandez-Hernando STFC/ASTeC Daresbury Lab.
Beam Test status and Plans of the ILC Main LINAC BPM
ATF2 Tuning Summary Nov & Dec 2010 Glen White, SLAC 11 th ATF2 Project Meeting, SLAC Jan
J. Pfingstner Imperfections tolerances for on-line DFS Improved imperfection tolerances for an on-line dispersion free steering algorithm Jürgen Pfingstner.
Kiyoshi Kubo Electron beam in undulators of e+ source - Emittance and orbit angle with quad misalignment and corrections - Effect of beam pipe.
ATF2 Report ALCW Kiyoshi KUBO, for ATF2 Collaboration.
Main Linac Tolerances What do they mean? ILC-GDE meeting Beijing Kiyoshi Kubo 1.Introduction, review of old studies 2.Assumed “static” errors.
Task Lists of ATF2 commissioning Toshiyuki Okugi ATF2 Project Meeting 12 / 17 / 2008.
ATF2 beam operation status Toshiyuki OKUGI, KEK The 9 th TB&SGC meeting KEK, 3-gokan Seminar Hall 2009/ 12/ 16.
IPBSM Operation 11th ATF2 Project Meeting Jan. 14, 2011 SLAC National Accelerator Laboratory Menlo Park, California Y. Yamaguchi, M.Oroku, Jacqueline Yan.
Summary of Tuning, Corrections, and Commissioning ( Short summary of ATF2 meeting at SLAC in March 2007 ) and Hardware Issues for beam Tuning Toshiyuki.
FONT GROUP MEETING ATF JUNE SUMMARY Neven & Talitha Talitha Bromwich - Friday, 26 June 2015.
FJPPL-FKPPL ATF2 Workshop Jitter studies March 18, 2014 Beam jitter localization and identification at ATF2 Marcin Patecki Jürgen Pfingstner 18 th of March.
Wakefield effect in ATF2 Kiyoshi Kubo
Direct Wakefield measurement of CLIC accelerating structure in FACET Hao Zha, Andrea Latina, Alexej Grudiev (CERN) 18/06/2015 High Gradient work shop 2015.
Technical Board Summary Preliminary Philip Bambade Laboratoire de l’Accélérateur Linéaire Université Paris 11, Orsay, France ATF2 project meeting, Technical.
Progress in CLIC DFS studies Juergen Pfingstner University of Oslo CLIC Workshop January.
Wakefield of cavity BPM In ATF2 ATF2 Project Meeting K.Kubo.
ILC Main Linac Beam Dynamics Review K. Kubo.
ATF2 Status N.Terunuma, KEK
Beam jitter experiment of exchanging power supplies
Intensity dependence of Beam size at IP and Wakefield in ATF2
Wakefield Effect at ATF2
For Discussion Possible Beam Dynamics Issues in ILC downstream of Damping Ring LCWS2015 K. Kubo.
Emittance Dilution and Preservation in the ILC RTML
Beam Dynamics in Curved ILC Main Linac (following earth curvature)
Wakefield simulations for ILC cavity
ATF2 Recent Wakefield (Beam size Intensity dependence) Studies
Summary of the ATF2 project meeting at LAL (Jan.13-15, 2016)
Cavity BPMs at Diamond S. Boogert, A. Lyapine (UCL), G. Rehm
Bunch Tiltmeter Steve Smith SLAC Snowmass July 16, 2001 Update date
Presentation transcript:

Brief review of past studies on Wakefield ATF2 Proj. Mtg K.Kubo

Intensity dependence of IP beam size Studies using on-mover structures – Beam size at IP – Orbit change OTR chamber wake

IPBSM modulation as function of bunch population. Measured with crossing angle 174 degrees (left) and 30 degrees (right). Beam Size Depends on Bunch Intensity Presented in IPAC14

This calc. Included cavity BPMs only. May underestimate wakefield. But factor 6 difference seems too much. Okugi’s slide in proj. mtg. Feb (19 nm/nC)

Calc. by A. Lyapin More calculations Examples of wake calculations

J.Snuverink, et.al., LCWS2014 Wake source on mover experiment -- orbit change

C-band ref.No mask Bellows Masked Bellows Experiment 5547~507 Calc ? IP beam size vs mover position experiment and calc. Effect of wake source at the mover, offset 1 mm, bunch charge 1 nC. IP beam size increase (nm/mm/nC) ATF2 weekly meeting K.Kubo Factor 1.7 – 2.2 larger than calculation consistent wit orbit change measurement

Effect of OTR monitor chamber (beam size monitor in EXT line) to IP vertical beam size was found (June 2014) IPBSM 174 degrees N~0.3E10

Before OTR2X position optimization After optimization (174 deg mode) 100 nm/nC  58 nm/nC By Okugi, Removal of all OTRs 121 nm/nC  76 nm/nC (30 deg mode) Okugi, ATF Op. meeting Dependence reduced by optimizing position or removing chamber. (similar effect) (30 deg mode tend to give stronger dependence than 174 deg mode.) Slide by K.Kubo in ATF operation meeting Nov 7, 2014

Photo by D. McCormick OTR monitor View Port Shield No shield With shield by A. Lyapin Remove vertical asymmetry Reduce position dependent wake (factor 0.6) 0.08 V/pC/mm  0.05 V/pC/mm

Okugi, June 6, ATF Operation meeting

Orbit Change vs. OTR chamber position (Okugi, ATF Op. meeting) About 6-10 times bigger than expected from calculation (OTR chamber only) Peak ~0.05 V/pC/mm Kick angle/offset (urad/mm) Wake (average in a bunch) (V/pC/mm) OTR OTR OTR OTR (Oct. 28, 2014, one BPM) (Nov. 11, 2014, many downstream BPMs ) (Kubo, owl shift log)

Experiments compare with calculations Position of Wake source Reference cavity on mover – Factor 1.8~2 larger (Both IP beam size and Orbit) OTR chamber wake – Factor 6~10 larger (Both IP beam size and Orbit) Need to consider other moving parts. But discrepancy of OTR chamber effect is too large. Strong intensity dependence after optimizing cavity and chamber positions Not understood yet

Wakefield in ILC FF Effects of transverse wakefield will be much smaller than in ATF2 – High energy, short bunch length – Beam pipe aperture will be similar Except for collimators (special care will be necessary) – Careful design of beam pipe and structures in the beam line But, solving the apparent discrepancies between observations and calculations is still important