ATF2:Summary of Tolerance

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.
Sha Bai, Philip Bambade, Glen White FJPPL – FKPPL ATF2 workshop LAL, 11~13 February, 2013 Orthogonality of beam waist corrections in the presence of IPBSM.
ILC BDS Alignment and Tuning Studies Glen White SLAC/QMUL 8 November 2005 Progress report and ongoing plans for BDS alignment and tuning strategy.
ATF2 FB/FF layout Javier Resta Lopez (JAI, Oxford University) for the FONT project group FONT meeting January 11, 2007.
Some simulation results on FF/FB system for ATF2 Javier Resta Lopez (JAI, Oxford University) for the FONT project group FONT meeting January 25, 2008.
Optics for Skew Correction and Emittance Measurement Leo Jenner This talk is going to look familiar if you were at the recent LC-ABD meeting in Manchester…
A.Seryi, Nov 22, 2005, slide 1 Evaluation of Aug9 2mrad Use 2mrad extraction, version Aug 9, Use high.
BROOKHAVEN SCIENCE ASSOCIATES Abstract Magnetic Specifications and Tolerances Weiming Guo, NSLS-II Project In this presentation I briefly introduced the.
-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.
LCLS-II Transverse Tolerances Tor Raubenheimer May 29, 2013.
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.
Status of very high priority beam tuning software Special ATF2 project meeting, Korea, 1 st October 2008 Cécile Rimbault, on behalf of High Priority task.
Alignment and Beam Stability
ATF2 Javier Resta Lopez (JAI, Oxford University) for the FONT project group 5th ATF2 project meeting, KEK December 19-21, 2007.
Trajectory Correction and Tuning James Jones Anthony Scarfe.
ATF2 ILC Final Focus Test Beam Line at KEK-ATF References : ATF2 Proposal, KEK Report ATF2 Proposal Vol.2, KEK Report ホームページ:
ATF2 optics … 1 3 rd Mini-Workshop on Nano Project at ATF ATF2 optics, tuning method and tolerances of initial alignment, magnets, power supplies etc.
March 7, 2007 LET Issues (Cai/Kubo/Zisman) Global Design Effort 1 Low-Emittance Tuning Issues and Plans Yunhai Cai, Kiyoshi Kubo and Michael S. Zisman.
For Draft List of Standard Errors Beam Dynamics, Simulations Group (Summarized by Kiyoshi Kubo)
1 Status of EMMA Shinji Machida CCLRC/RAL/ASTeC 23 April, ffag/machida_ ppt & pdf.
ATF2 Magnets ATF2 Magnets 11Mar '08, Weekly MtgCherrill Spencer Status Report ATF2 FD quads 1 Status Report on the ATF2 “Final Doublet” quads being made.
European Organization for Nuclear Research International Linear Collider INTERNATIONAL WORKSHOP ON FUTURE LINEAR COLLIDERS ЛЦВС14 Vinča Institute of Nuclear.
Matching recipe and tracking for the final focus T. Asaka †, J. Resta López ‡ and F. Zimmermann † CERN, Geneve / SPring-8, Japan ‡ CERN, Geneve / University.
ILC BDS Static Beam-Based Alignment and Tuning Glen White SLAC 1.Aims. 2.Error parameters and other assumptions. 3.Overview of alignment and tuning procedure.
Mark Woodley, SLACATF2 Project March 20-21, Summary of Tuning, Corrections, and Commissioning.
1 BROOKHAVEN SCIENCE ASSOCIATES Issues on Closed Orbit Feedback for NSLSII NSLS-II Stability Workshop April 18-20, 2007 Li-Hua Yu.
Optimization of Field Error Tolerances for Triplet Quadrupoles of the HL-LHC Lattice V3.01 Option 4444 Yuri Nosochkov Y. Cai, M-H. Wang (SLAC) S. Fartoukh,
Analysis of Multipole and Position Tolerances for the ATF2 Final Focus Line James Jones ASTeC, Daresbury Laboratory.
ATF2 Magnets etc. 1. Magnets 2. Power supplies 3. Magnetic field measurement 4. Movers and supports R. Sugahara May 30, 2005.
Initial beam size commissioning for ATF2 T.Okugi 3rd ATF2 Project Meeting, KEK 12/ 19/ 2006.
IP instrumentation configuration for Autumn 2010 ATF2 runs Toshiyuki OKUGI, KEK 2010 / 7/ 1 10 th ATF2 project meeting.
Beam Dynamics IR Stability Issues Glen White / SLAC September IRENG07 Vibration tolerances for final doublet cryomodules Settlement of detector.
Summary of Tuning, Corrections, and Commissioning ( Short summary of ATF2 meeting at SLAC in March 2007 ) and Hardware Issues for beam Tuning Toshiyuki.
COMPENSATION OF DETECTOR SOLENOID FIELD WITH L*=4.1M Glen White, SLAC April 20, 2015 ALCW2015, KEK, Japan.
ERHIC Orbit Correction Studies (Minor Update) Using Oct’14 lattice and dispersion diagnostic January 5, 2015Stephen Brooks, eRHIC FFAG meeting1.
Simulation of the α, dispersion, coupling and β multiknobs in large β optics Sha Bai, Philip Bambade, Benoit Bolzon, Javier Resta Lopez
Warm linac simulations (DTL) and errors analysis M. Comunian F. Grespan.
Status and plan of Beta-matching in Extraction line Kiyoshi Kubo.
Wakefield effect in ATF2 Kiyoshi Kubo
2nd ATF2 Project Meeting (May 30, 2006)M. Woodley [SLAC]1 ATF2 Layout/Optics (v3.3) nBPM (SLAC) nBPM (KEK) FONT Compton / laserwire ODR Existing ATF Extraction.
8 th February 2006 Freddy Poirier ILC-LET workshop 1 Freddy Poirier DESY ILC-LET Workshop Dispersion Free Steering in the ILC using MERLIN.
PS2 Orbit Correction - Update Wolfgang Bartmann PS2 Meeting, 26 th March Mar-091PS2 Orbit Correction - Update.
4 th ATF2 Project Meeting, 31 May 2007 A. Seryi 1 Summary of SLAC simulation study of emittance growth in the ATF extraction line SLAC team: J. Amann,
Integrated ATF2 Dynamic Tuning Simulations Glen White, LAL/SLAC ATF2 Software Workshop June 2008 Simulation overview. Tuning for 37nm IP vertical beam.
IP Tuning Task Updates Glen White, SLAC January
ILC BDS LATTICE DESIGN WITH TDR PARAMETERS
Alignment and stability session
From Beam Dynamics K. Kubo
Cherrill Spencer, SLAC Member of ATF2 Magnet Team
Summary FD Support System
ILC DR Lower Horizontal Emittance, preliminary study
ILC BDS Alignment, Tuning and Feedback Studies
Correlated Misalignments Studies for LCLS-II SC Linac
Tolerances & Tuning of the ATF2 Final Focus Line
For Discussion Possible Beam Dynamics Issues in ILC downstream of Damping Ring LCWS2015 K. Kubo.
Adaptive Alignment & Ground Motion
Alignment Results of Magnets in the ATF2 Beam Line
Non-linear Beam Dynamics Studies for JLEIC Electron Collider Ring
ATF2 IP Tuning Task Simulation Updates
Field quality to achieve the required lifetime goals (single beam)
Updates on IR and FF for super-B factory
Chromatic Corrections in LCLS-II P. Emma, Y. Nosochkov, M. Woodley Mar
Final Focus Optics Test at ATF
Motivation Technique Simulations LCLS LCLS DOE Review, April 24, 2002
DTL M. Comunian M. Eshraqi.
Triplet corrector layout and strength specifications
Yuri Nosochkov Yunhai Cai, Fanglei Lin, Vasiliy Morozov
Crab crossing plan Optimize the crabbing system for best beam stability and minimum emittance impact Study and specify tolerances on cavity multipole components.
DYNAMIC APERTURE OF JLEIC ELECTRON COLLIDER
Presentation transcript:

ATF2:Summary of Tolerance S.Kuroda( KEK ) 1. Summary of ATF2 proposal vol.1 2. Tolerance for Q Power Supply 3. Tolerance of SX component of Q with Correction 4. Tolerance of Q Misalignment with Linear Knob Correction ( Studies 2,3 and 4 are preliminary should be sophisticated. ) 2nd ATF2project meeting 30MAY2006

1. Summary of ATF2 proposal vol.1 Tolerable field ratio at r=10mm for 2% beam size growth [J.Jones]

Summary of ATF2 proposal vol.1(cont.) Vibration tolerance for 2% beam size growth [A.Seryi]

2. Tolerance for Q Power Supply Qs are classified into 5 groups( cf. Kumada case1 ) QD0, QF1, QD4&10, QM, others In this simulation, for each Q, K1 error is dK1/K1=s maxK1/K1 Here maxK1 is maximum Abs[K1] of the group and s =10ppm(QD0) 30ppm(QF1, QD4&10) sx(QM, others) Sim. Cond. ex=2e-9,gey=3e-8, d=8e-4 ideal sy=34.8nm sx =100ppm Gaussian error dist. sy(95%CL)=48nm sx =100ppm Uniform error dist. sy(95%CL)=38.5nm  sx =250ppm Uniform error dist. sy(95%CL)=52nm 

3. Tolerance of SX component of Q with Correction sigx sigy Gaussian error dB2/B1@r=10mm =1e-4 for FD =1e-3 for 20cm Q Correction Knob: SX Trial and error looking at sy step: dK2=1e-2 Perfect BSM resolution is assumed After Correction

Tolerance of SX component of Q with Correction( cont. ) =1e-3(for 20cm Q) variable(for FD) dK2=2 sgn K1 /r (r=10mm, sgn=1: random for each Q) dK2=+2 K1 /r (r=10mm) dK2=-2 K1 /r (r=10mm) Example:dFD=5e-4 Corr  It seems OK for dFD=5e-4.

Tolerance of SX component of Q with Correction(cont.2) dK2=2 sgn K1 /r Sin[q], dSK2=2 sgn K1 /r Cos[q] (r=10mm, sgn=1: random for each Q,0<q<2p:uniformly random) Correction: roll(1mrad step) of SX+K2(1% step) of SX dFD=1e-4 After cor., sy(95%CL)=44nm Iteration of correction x2  sy(95%CL)=47nm Iteration of cor. is not effective Cor.  dFD=5e-4, d20cmQ=5e-4 After cor., sy(95%CL)=225nm SK2 of FD affects significantly to sy. Tolerance of SK2 should be much less than 1e-4. Cor. 

4. Tolerance of Q Misalignment with Linear Knob Correction Mover of SX DXWaistX, WaistY, PEX DYPEY, Coupling(R1,R2) Each knobs are orthogonalized by linear combination Correction Order: R2,R1,WY,PEY Correction step: WaistY:1mm(sy>1mm) 100mm(sy>100nm) 20mm(sy<100nm) R1:1e-2 (sy>1mm) 1e-3(sy>100nm) 1e-4(sy<100nm) R2:1e-3 (sy>1mm) 1e-4(sy>100nm) 2e-5(sy<100nm) PEY: 10mm because of the resolution of the sy calculation by tracking(NP=1000) Performance for Single Type of Error of Q Gaussian error is assumed. Iterative correction was done for errors DY and Roll. dX dY d dK1  4e-5  2e-5  1e-6  5e-4 95% CL values are plotted.

Tolerance of Q Misalignment with Linear Knob Correction( cont. ) All types of errors (dK1/K1, dx, dy, roll)=a(5e-4, 40mm, 20mm,100mrad) Correction # of iteration ≤ 5 Iteration stops if sy≤ 35nm For a<0.7, sy<40nm after correction Mover Spec. Requirement Minimum step min. coeff. knob min.step WY:2e-5 SF1_DX=-0.0121574 wy 2.4e-7 PEY:1e-5 SD4_DY= -0.186651 py 1.9e-6 R1:1e-4 SD0_DY= -0.220771 r1 2.2e-5 R2:2e-5 SD0_DY= -0.127017 r1 2.5e-6 Dynamic range For a=0.6 max. coeff. knob max.step maxWY:1.98e-3 SD4_DX= 0.0721866 wy 1.4e-4 maxPEY:3e-4 SD0_DY= 0.429982 py 1.3e-4 maxR1:1.3e-3 SF6_DY= 0.526463 r1 6.5e-4 maxR2:3.8e-3 SF6_DY= 0.387005 r1 1.5e-3

Summary & Discussion Tolerances for multipole component of Q & vibration are reviewed( proposal vol.1 ). Some results of study for tolerance with correction are reported. But these are not completed and to be done more; 1. Higher order parameters should be included in the knobs. Then SX strength will be used as a part, so the correction for the SX component of Q should be done again. 2. Optics for the study should be updated. 3. Tolerance for FD is defined separately with the other Q( ? )