Issues in ILC Main Linac and Bunch Compressor from Beam dynamics N. Solyak, A. Latina, K.Kubo.

Slides:



Advertisements
Similar presentations
Update of RTML, Status of FNAL L-band and CLIC X-band BPM, Split SC Quadrupole Nikolay Solyak Fermilab (On behalf of RTML team) LCWS2010 / ILC 10, March.
Advertisements

Emittance dilution due to misalignment of quads and cavities of ILC main linac revised K.Kubo For beam energy 250 GeV,
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.
On Cavity Tilt + Gradient Change (Beam Dynamics) K. Kubo K. Kubo.
Main Linac Simulation - Main Linac Alignment Tolerances - From single bunch effect ILC-MDIR Workshop Kiyoshi KUBO References: TESLA TDR ILC-TRC-2.
ATF2 FB/FF layout Javier Resta Lopez (JAI, Oxford University) for the FONT project group FONT meeting January 11, 2007.
Cryomodule requirements Hitoshi Hayano, KEK for CFS consideration Asian Single Tunnel Design June 1-2,2010.
Feed forward orbit corrections for the CLIC RTML R. Apsimon, A. Latina.
Analysis of ATF EXT/FF Orbit Jitter and extrapolation to IP (Data of ) ATF2 Project Meeting K. Kubo.
Ground Motion + Vibration Transfer Function for Final QD0/SD0 Cryomodule System at ILC Glen White, SLAC ALCPG11, Eugene March 21, 2011.
Summary of AWG4: Beam Dynamics A. Latina (CERN), N. Solyak (FNAL) LCWS13 – Nov 11-15, 2013 – The University of Tokyo, Japan.
ML / RTML WG Summary N.Solyak, K.Kubo, A.Latina AWLC 2014 – Fermilab – May 16, 2014.
For Draft List of Standard Errors Beam Dynamics, Simulations Group (Summarized by Kiyoshi Kubo)
Y. Ohnishi / KEK KEKB-LER for ILC Damping Ring Study Simulation of low emittance lattice includes machine errors and optics corrections. Y. Ohnishi / KEK.
ILC Start-End Simulations Glen White, SLAC May 13, 2014 AWLC14, Fermilab.
Feed forward orbit corrections for the CLIC RTML R. Apsimon, A. Latina.
ILC Feedback System Studies Nikolay Solyak Fermilab 1IWLC2010, Geneva, Oct.18-22, 2010 N.Solyak.
Summary of WG1 K. Kubo, D. Schulte, P. Tenenbaum.
DESY GDE Meeting Global Design Effort 1 / 12 Status of RTML Design and Tuning Studies PT SLAC.
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.
Alignment (Survey) Tolerances in Main Linac from Beam Dynamics Simulations Kiyoshi Kubo.
Simulations Group Summary K. Kubo, D. Schulte, N. Solyak for the beam dynamics working group.
Report of 2 nd ILC Workshop (Snowmass) Working Group Kiyoshi KUBO references: Slides of the plenary talks in the workshop by P.Tenembaum and.
16 August 2005PT for US BC Task Force1 Two Stage Bunch Compressor Proposal Snowmass WG1 “It’s the latest wave That you’ve been craving for The old ideal.
SINGLE-STAGE BUNCH COMPRESSOR FOR ILC-SB2009 Nikolay Solyak Fermilab GDE Baseline Assessment Workshop (BAW-2) SLAC, Jan , 2011 N.Solyak, Single-stage.
July 19-22, 2006, Vancouver KIRTI RANJAN1 ILC Curved Linac Simulation Kirti Ranjan, Francois Ostiguy, Nikolay Solyak Fermilab + Peter Tenenbaum (PT) SLAC.
Simulations (LET beam dynamics ) Group report Kiyoshi Kubo.
Low emittance tuning in ATF Damping Ring - Experience and plan Sendai GDE Meeting Kiyoshi Kubo.
Introduction: Tasks of “Information for simulations”, hardware specs K.Kubo
1 Alternative ILC Bunch Compressor 7 th Nov KNU (Kyungpook National Univ.) Eun-San Kim.
1 Alternative Bunch Compressor 30 th Sep KNU Eun-San Kim.
Beam Dynamics WG Summary N.Solyak, K.Kubo, A.Latina LCWS 2014 – Oct 6-10, 2014 – Belgrade, Serbia.
1 DR -> IP Beam Transport Simulations with Intra-Train Feedback Glen White, SLAC Jan 19 th 2006.
Beam Dynamics WG K. Kubo, N. Solyak, D. Schulte. Presentations –N. Solyak Coupler kick simulations update –N. Solyak CLIC BPM –A. Latina: Update on the.
13 September 2006 Global Design Effort 1 ML (x.7) Goals and Scope of Work to end FY09 Nikolay Solyak Fermilab Peter Tenenbaum SLAC.
Placet based DFS simulations in the ILC Main Linac. Some preliminary results of error scans open for discussion Javier Resta Lopez JAI, Oxford University.
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.
Low Emittance Generation and Preservation K. Yokoya, D. Schulte.
GDE Main Linac and RTML Beam Dynamics Conveners: Nikolay Solyak, Cris Adolphsen, Kyioshi Kubo April 20, Room 303, 14:30 – 18:00.
1 DFS Studies on the Main Linac with Rnd-walk-like motion (preliminary) Accelerator Physics Meeting 02 october 2007 Freddy Poirier.
1 DFS Studies on the Main Linac with Rnd-walk-like motion LET Beam Dynamics Workshop 12 th December 2007 Freddy Poirier.
DMS steering with BPM scale error - Trial of a New Optics - Kiyoshi Kubo
Main Linac Tolerances What do they mean? ILC-GDE meeting Beijing Kiyoshi Kubo 1.Introduction, review of old studies 2.Assumed “static” errors.
Emittance preservation in the main linacs of ILC and CLIC Andrea Latina (CERN) Kiyoshi Kubo (KEK) LCWS University of Texas at Arlington - Oct
Simulations - Beam dynamics in low emittance transport (LET: From the exit of Damping Ring) K. Kubo
April Recent work on Low Emittance Transport, Main Linac Paul Lebrun CD/FNAL.
Emittance preservation in the RTML of ILC and CLIC Andrea Latina (CERN) Nikolay Solyak (FNAL) LCWS University of Texas at Arlington - Oct
DRAFT: What have been done and what to do in ILC-LET beam dynamics Beam dynamics/Simulations Group Beijing.
Wakefield effect in ATF2 Kiyoshi Kubo
Freddy Poirier - DESY Preliminary Merlin DFS studies following discussion (Very preliminary) Freddy Poirier DESY.
8 th February 2006 Freddy Poirier ILC-LET workshop 1 Freddy Poirier DESY ILC-LET Workshop Dispersion Free Steering in the ILC using MERLIN.
Progress in CLIC DFS studies Juergen Pfingstner University of Oslo CLIC Workshop January.
Review of Alignment Tolerances for LCLS-II SC Linac Arun Saini, N. Solyak Fermilab 27 th April 2016, LCLS-II Accelerator Physics Meeting.
ILC Main Linac Beam Dynamics Review K. Kubo.
Effects of Accelerating Cavities on On-Line Dispersion Free Steering in the Main Linac of CLIC Effects of Accelerating Cavities on On-Line Dispersion Free.
From Beam Dynamics K. Kubo
Arun Saini, N. Solyak Fermi National Accelerator Laboratory
Correlated Misalignments Studies for LCLS-II SC Linac
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)
ILC Z-pole Calibration Runs Main Linac performance
Summary of Beam Dynamics Working Group
DFS Simulations on ILC bunch compressor
Adaptive Alignment & Ground Motion
Accelerator Physics Technical System Group Review
The Proposed Conversion of CESR to an ILC Damping Ring Test Facility
Feed forward orbit corrections for the CLIC RTML
Start-to-End Simulations for the TESLA LC
Presentation transcript:

Issues in ILC Main Linac and Bunch Compressor from Beam dynamics N. Solyak, A. Latina, K.Kubo

Introduction From results of large amount of past studies in ML beam dynamics, our conclusion was (and is): No serious problem is expected. However – More simulations for emittance preservation in BC is necessary. – BC + ML combined simulation is necessary for completeness. – Experimental test of steering correction is desirable. – How to proceed commissioning has not been studied. – Our requirements may not be really understood or agreed by groups/people who should be responsible for the hardware e.g., alignment, magnet control, cavity control,,,,. Need to modify some of the requirements, for making them more realistic. Coupler kicks in BC

BC emittance growth Emittance budget is barely satisfied in TDR. Need more careful studies E.g. coupler kicks (see later)

BC + ML combined simulations Most simulations assume beam energy is controllable at the entrance of ML for DFS (DMS). – Energy control is actually done in BC and should be included in simulations. – Effects to bunch length? Difficulty is (was?) – Most (?) simulation codes do not include relative longitudinal position change. This can be part of S2E simulations, reported by BDS.

Experimental test of steering correction DFS and WFS (Dispersion free steering and wake free steering) experiment at FACET – Results have not been very satisfactory. – Need more analysis and simulations. Then, probably further experiments. Possibly by a wider collaboration. – Though condition is significantly different from ILC BC+ML, this experiment can tell how out simulations are reliable.

Commissioning studies Strategy? – What is the incoming beam condition when we want to start commissioning of BC and ML? From upstream to down stream step by step, making good condition in each region (DR, RTML, BC, ML, BDS)? Or go through the whole beam line first and gradually improve all? Tactics? – Use single bunch, small number of bunches or long trains? Intra-pulse feedback? No systematic studies so far?

Specifications Revisit + alpha

ErrorRTML and ML Coldwith respect to Quad Offset300 μmcryo-module Quad roll300 μraddesign RF Cavity Offset300 μmcryo-module RF Cavity tilt300 μradcryo-module BPM Offset (initial)300 μmcryo-module Cryomoduloe Offset 200 μmdesign Cryomodule Pitch20 μraddesign Local Alignment Error in ML What is the long range alignment method? Is the “independent random error” assumption good enough? Independent Gaussian Random assumed in evaluation of all errors. Not based on realistic survey/alignment models. Distance range up to betatron period, ~ 400 m, is important.

BPM performance Resolution5 μm* Scale Error<10%* Attention: Resolution: Simulations assumed 1 um resolution  Need averaging 25 Scale Error: < 3% is desirable. For adjusting nonzero vertical dispersion. Possibility of calibration using beam should be considered. Or, consider optics less sensitive to the error. TDR

Cavity Acc. Voltage Flatness Cavity tilt (alignemnt) + voltage change cause transverse orbit change Cavity by cavity Acc. Voltage “Flatness” required – RF control for individual cavity, not only “Vector Sum” Tolerance: – (RMS cavity tilt) x (RMS Flatness) < (300 um) x (1%) Demonstrated at FLASH (TDR Part I 3.2) All RF stations can be controlled with this accuracy? RF control in low energy part of the linac is important.

Main Linac Bunch compressor Dynamic Errors (from TDR)

Transverse Coupler Kicks From slides by V.Yakovlev, in ILC-CLIC Beam Dynamics Workshop, CERN 2009 upstream downstream Vertical total Kicks at Upstream and Downstream mostly cancelled. Careful design needed???

Simulated Emittance growth in Bunch Compressor From slides by V.Yakovlev, in ILC-CLIC Beam Dynamics Workshop, CERN 2009 nm Cryomodule pitch remote control is desirable. TDR mentions as follows (bol. 3 part II, p130.) “In addition to the other BBA algorithms, the simulations applied a “girder optimisaton” (or tilting of cryomodules) algorithm to minimize emittance growth to 1.09 nm rms (1.48 for 90% of seeds)” But this is not explicitly required in TDR.

Proposed (used in a simulation) Cryo-module pitch adjustment (remote movers) Range ~ 0.3 mm Step ~ 10 micron All 3 modules in BC1, 4 modules in BC2 (out of 48) Need response from engineering point of view. Then, detail should be re-studied For better emittance control

Manpower Tasks (guesstimated FET x Year) Beam Dynamics – Lattice design, including flexible BC (0.5) – BC emittance simulations including coupler kicks (1) – BC + ML combined simulations, part of S2E whole machine simulations (1-2) Beam dynamics + Engineering – BC cryo-module pitch control engineering (0.5) – Alignment studies and modeling, probably for whole machine (?) Experiment – Beam Based Steering Correction at FACET. (?) Present manpower is not enough. (for Beam Dynamics) May be ~1 FTE in 2014 from America ? ~0.1 FTE from Europe ? ~0.2 from Asia ?