1 Virtual Accelerator plan and status at RCS Hiroshima University, Graduate School of Science Experimental Quark Physics Lab ( & JAEA Accelerator Development.

Slides:



Advertisements
Similar presentations
Current Status of Virtual Accelerator at J-PARC 3 GeV Rapid Cycling Synchrotron H. Harada*, K. Shigaki (Hiroshima University in Japan), H. Hotchi, F. Noda,
Advertisements

Masahito TOMIZAWA and Satoshi MIHARA Accelerator and proton beam.
Current Status of MATLAB-based Accelerator Physics Application Programs for the TPS Commissioning and Operation at NSRRC Fan-Hsin Tseng ( 曾繁信 ) Beam Dynamics.
XAL at J-PARC Hiroyuki Sako, G. Shen, JAEA C. K. Allen, ORNL Contents Why did we introduce XAL? Installing XAL Developing XAL Achievements with XAL Summary.
“AC” Dispersion Measurement David Rubin Cornell Laboratory for Accelerator-Based Sciences and Education.
Searching for CesrTA guide field nonlinearities in beam position spectra Laurel Hales Mike Billing Mark Palmer.
Resonance crossing and error tolerances Shinji Machida KEK FFAG05 at Fermilab, April 3-7, 2005.
Diane Fairley High Level October 24-28, 2005 High Level Physics Applications LCLS Week / FAC October 24-28, 2005.
Introduction Status of SC simulations at CERN
JCE A Java-based Commissioning Environment tool Hiroyuki Sako, JAEA Hiroshi Ikeda, Visible Information Center Inc. SAD Workshop.
Sep 29 – Oct 3, 2009 LCWA 09 Linear Collider Workshop of the Americas Sept 29 – Oct 4, 2009 Damping Ring R&D updates SLAC Mauro Pivi SLAC Allison Fero.
25-26 June, 2009 CesrTA Workshop CTA09 Electron Cloud Single-Bunch Instability Modeling using CMAD M. Pivi CesrTA CTA09 Workshop June 2009.
Simulation of direct space charge in Booster by using MAD program Y.Alexahin, N.Kazarinov.
A Brief Introduction of SAD for ATF2 Flight Simulator S.Kuroda(KEK) mini work shop for flight simulator(LAL)2008.
BROOKHAVEN SCIENCE ASSOCIATES High level applications and EPICS control GUOBAO SHEN NSLS-II, Control Group May 4 th, 2009.
Virtual Accelerator at J-PARC 3 GeV Rapid Cycling Synchrotron H. Harada*, K. Shigaki (Hiroshima University in Japan), H. Hotchi, F. Noda, H. Sako, H. Suzuki,
Particle dynamics in electron FFAG Shinji Machida KEK FFAG04, October 13-16, 2004.
1 Status of EMMA Shinji Machida CCLRC/RAL/ASTeC 23 April, ffag/machida_ ppt & pdf.
The CSS Scan System Kay-Uwe Kasemir SNS/ORNL Dec
Development of Simulation Environment UAL for Spin Studies in EDM Fanglei Lin December
Basic BPM Hardware Theory Jim Steimel. Wall Current Charge in a cylindrical perfectly conducting pipe produces an equal and opposite image charge at the.
Details of space charge calculations for J-PARC rings.
Mathilde FAVIER Fellow in BE/BI/QP Mathilde FAVIER BE/BI-QPSCHOTTKY STATUS - BI DAY - December 6th
Kazuro Furukawa, KEK, Jul KEK Linac Operation and Stability Linac Mini-Workshop 2006, IHEP, Beijing 1 KEK Linac Operation (Some Experiences) Kazuro.
ATF2 beam commissioning status and beam time request Toshiyuki Okugi 2008 / 11 / 12 ATF2 Commissioning Meeting.
Simulation of direct space charge in Booster by using MAD program Y.Alexahin, A.Drozhdin, N.Kazarinov.
Beam observation and Introduction to Collective Beam Instabilities Observation of collective beam instability Collective modes Wake fields and coupling.
Storage ring optics characterization – the basics
1 BROOKHAVEN SCIENCE ASSOCIATES Storage Ring Commissioning Samuel Krinsky-Accelerator Physics Group Leader NSLS-II ASAC Meeting October 14-15, 2010.
1 FFAG Role as Muon Accelerators Shinji Machida ASTeC/STFC/RAL 15 November, /machida/doc/othertalks/machida_ pdf/machida/doc/othertalks/machida_ pdf.
Part III Commissioning. Proof of Principle FFAG (POP) study The world first proton FFAG –Commissioned in March –From 50 keV to 500 keV in 1ms. –Proof.
Beam Loss Simulation in the Main Injector at Slip-Stacking Injection A.I. Drozhdin, B.C. Brown, D.E. Johnson, I. Kourbanis, K. Seiya June 30, 2006 A.Drozhdin.
Managed by UT-Battelle for the Department of Energy Using Online Single Particle Model for SNS Accelerator Tuning Andrei Shishlo, Alexander Aleksandrov.
The Quadrupole Pick-up in the CPS -intro and progress report PPC 3 Dec 1999 A. Jansson.
E-cloud studies at LNF T. Demma INFN-LNF. Plan of talk Introduction New feedback system to suppress horizontal coupled-bunch instability. Preliminary.
E Levichev -- Dynamic Aperture of the SRFF Storage Ring Frontiers of Short Bunches in Storage Rings INFN-LNF, Frascati, 7-8 Nov 2005 DYNAMIC APERTURE OF.
J-PARC Accelerator and Beam Simulations Sep. 7th, SAD2006 Masahito Tomizawa J-PARC Main Ring G., KEK Outline of J-PARC Accelerator Characteristics of High.
Andreas Jansson, "Quadrupole Pick-ups", LHC BI-Review, November 19-20, Quadrupole Pick-ups  What is a quadrupole pick-up?  PS pick-ups and experimental.
2/20/2016J-PARC1 Virtual Accelerator An Accelerator Simulator.
… Work in progress at CTF3 … Davide Gamba 01 July 2013 Study and Implementation of L INEAR F EEDBACK T OOLS for machine study and operation.
1 BEAM COMMISSIONING SOFTWARE AND DATABASE FOR J-PARC LINAC Hiroyuki Sako G. Shen, H. Sakaki, H. Takahashi, H. Yoshikawa, JAEA H. Ikeda, VIC C. K. Allen,
Off-momentum DA of RCS 3D_BM & QFF & CC AP meeting / December 8, 2004 Alexander Molodozhentsev Etienne Forest KEK.
Beam-beam Simulation at eRHIC Yue Hao Collider-Accelerator Department Brookhaven National Laboratory July 29, 2010 EIC Meeting at The Catholic University.
Experience with Novosibirsk FEL Getmanov Yaroslav Budker INP, Russia Dec. 2012, Berlin, Germany Unwanted Beam Workshop.
1 Error study of non-scaling FFAG 10 to 20 GeV muon ring Shinji Machida CCLRC/RAL/ASTeC 26 July, ffag/machida_ ppt.
Beam Diagnostics Seminar, Nov.05, 2009 Das Tune-Meßverfahren für das neue POSI am SIS-18 U. Rauch GSI - Strahldiagnose.
Professor Philip Burrows John Adams Institute for Accelerator Science Oxford University ACAS School for Accelerator Physics January 2014 Longitudinal Dynamics.
6 July 2010 | TU Darmstadt | Fachbereich 18 | Institut Theorie Elektromagnetischer Felder | Sabrina Appel | 1 Micro bunch evolution and „turbulent beams“
HEADTAIL simulation during the accelerating ramp in the PS S. Aumon - EPFL & CERN Acknowledgement to B. Salvant, G. Rumolo.
BEAM COMMISSIONING SOFTWARE AND DATABASE FOR J-PARC LINAC Hiroyuki Sako G. Shen, H. Sakaki, H. Takahashi, H. Yoshikawa, JAEA H. Ikeda, VIC C. K. Allen,
LCLS Commissioning & Operations High Level Software
Weiming Guo Accelerator Physics Group / ASD Advanced Photon Source
Vertical emittance measurement and modeling Correction methods
Beam based measurements
402.5 MHz Debunching in the Ring
HIAF Electron Cooling System &
Electron Cooling Simulation For JLEIC
Pretzel scheme of CEPC H. Geng, G. Xu, Y. Zhang, Q. Qin, J. Gao, W. Chou, Y. Guo, N. Wang, Y. Peng, X. Cui, T. Yue, Z. Duan, Y. Wang, D. Wang, S. Bai,
LCLS Commissioning & Operations High Level Software
Multiturn extraction for PS2
Lecture HT14 Beam-Beam II
Lecture 33 ACCELERATOR PHYSICS HT E. J. N. Wilson.
November 14, 2008 The meeting on RIKEN AVF Cyclotron Upgrade Progress report on activity plan Sergey Vorozhtsov.
A Virtual Implementation of VELA (CLARA)
November 7, 2008 The meeting on RIKEN AVF Cyclotron Upgrade Progress report on activity plan Sergey Vorozhtsov.
High Level Physics Applications for LCLS Commissioning
Progress in Code Benchmarking
Physics 417/517 Introduction to Particle Accelerator Physics
Simulation of the bunching effect:
High Level Physics Applications Lehman Review February 7 - 9, 2006
Presentation transcript:

1 Virtual Accelerator plan and status at RCS Hiroshima University, Graduate School of Science Experimental Quark Physics Lab ( & JAEA Accelerator Development Group ) Hiroyuki Harada MR/RCS beam commissioning meeting in KEK Oct. 25th (Tues), 2005 Web page of my work:

2 Plan for virtual accelerator 1. Estimation of the best K value of each magnet from matching by simulation code 2. Estimation of the measurement method of each parameter and the beam & elements condition from the monitor's signal by the tracking. → Reflection to real measurement. 3. Estimation of the beam loss by MARS.

3 SAD SIMPSONS STRUCT/MARS ・・・ Element EPICS Control Model by VA Set Magnets Simulator Simulation Input File PCASIOC Operating Log DB Operating parameter DB1 ( DB for elements ) IOC Interface Power Source Position information of the elements Physics value ⇔ Device value Transformation parameters EPICS Channel name Operation panel with GUI The signal of each monitor Start virtual operation Real AcceleratorVirtual Accelerator the signal of each monitor

4 Plan 1 ~ operation and matching Matching will be carried out by SAD, but maybe switch to JAD in the future. Operation panel with GUI for commissioning will be created by JAD (script by java based SAD) until the comprehensive examination of RCS around Dec The GUI operation panels for each operating mode and scenario will be created. This will carry out COD correction and search of the best K1 tune by tune, etc.

5 Sample GUI by KBFrame

6 Plan 2 ~ examination of measurement method of each parameter by VA The measurement of the tune (now in progress) The measurement of the chromaticity (now in progress) The measurement of the dispersion function The measurement of the Beta function The measurement of all other parameters

7 Plan 3 ~ estimation of beam loss The estimation of the beam loss will be calculated by MARS, using the results from the tracking by Simpsons. The other thing than those above is unknown yet.

8 Status for VA VA system via EPICS PCAS - Preliminary system was created. System to create the input files for simulation code from DB - Trace3D, SAD, MAD and XAL only QM and BM was created by Sako-san. Examination of measurement method for each parameter - Measurement for tune and chromaticity is now in progress. Integration of simulation codes (SAD, Simpsons and MARS) - The communication between EPICS and Simpsons is now in progress.

9 The construction of system ~ The control system of simulation code via EPICS PCAS GUI Operation panel (by KBFrame) EPICS PCAS Simulator K1 value Monitor signal K1 value Figure. A created the sample operation panel with GUI Monitor signal EPICS : Experimental Physics and Industrial Control System PCAS : Portable Channel Access Server

10

11 Fourier transform

12 Measurement of the tune For the beam condition, εx, y : 216 pi mmmrad Number of particles : 4800 Spread of the dp/p : 1% Length of the bunch : about 83 m Non space charge Non fluctuation of the BPMs Side band by Synchrotron Oscillation

13 The location of the exciters at RCS

14 The exciter at RCS RCS L (m) 0.81 p (GeV/c) 0.61 → 3.82 Z (Ω) 100 P (W) 1000 d (m) Table . The parameters of RCS-Exciter θrms is the kick-angle by the exciter, p is the beam momentum, β is Lorenz beta, c is the speed of light, P is the power supplied from the amp, d is the length of electrode plate, Ex is the electric field. The exciter gives the beam the kick with Δx’ at a point in RCS ring turns by turns. The frequency spectrum of the exciter is the band-limited white noise of the frequency width with ΔΩ, Ωj is the frequency, φj is the random initial phase, N is the number of the spectrum that the amplitude is constant. Figure . The white noise of simulated RCS- Exciter

15 Measurements of the Chromaticity RF frequency Δf vs dp/p The right figure shows that a change of the RF frequency makes the dp/p of the beam a fluctuation. The chromaticity is gotten by the measurement of Δν for each dp/p (or the RF frequency). Chromaticity :ξ = Δν/ Δp/p It seems that the RF in SAD is not right when the RF frequency is changed. So, the RF is under examination. If the RF has a buggy behavior, I will simulate the RF by using the other code. task

16 The time schedule of VA at RCS Submission of my thesis now the comprehensive examination at RCS Start of the beam commissioning at RCS the completion of the operation panel with GUI by JAD The communication between EPICS and Simpsons will be done. The main code of the tracking replace SAD to Simpsons. Start to create the operation panel with GUI by JAD Start to create the scenario for the commissioning at RCS The coordination of the connection between EPICS and the operation panel with GUI by JAD

17 Back a slide