Fast kicker beam dynamics simulations

Slides:



Advertisements
Similar presentations
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.
Advertisements

Sergey Antipov, University of Chicago Fermilab Mentor: Sergei Nagaitsev Injection to IOTA ring.
STRIPLINE KICKER STATUS. PRESENTATION OUTLINE 1.Design of a stripline kicker for beam injection in DAFNE storage rings. 2.HV tests and RF measurements.
A fast RF kicker for the MEIC electron cooler Andrew Kimber Amy Sy 31 st March 2015 Thomas Jefferson National Accelerator Facility is managed by Jefferson.
22/03/1999A.Blas1 Hollow bunches A. Blas, S. Hancock, S. Koscielniak, M. Lindroos, F. Pedersen, H. Schonauer  Why: to improve space charge related problems.
Generation and Characterization of Magnetized Bunched Electron Beam from DC Photogun for MEIC Cooler Laboratory Directed Research and Development (LDRD)
Simulation of direct space charge in Booster by using MAD program Y.Alexahin, N.Kazarinov.
Particle dynamics in electron FFAG Shinji Machida KEK FFAG04, October 13-16, 2004.
ASTRA Injector Setup 2012 Julian McKenzie 17/02/2012.
AAC February 4-6, 2003 Protons on Target Ioanis Kourbanis MI/Beams.
Bunched-Beam Phase Rotation and FFAG -Factory Injection David Neuffer Fermilab.
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.
X-Band Deflectors Development at SLAC
Muon cooling with Li lenses and high field solenoids V. Balbekov, MAP Winter Meeting 02/28-03/04, 2011 OUTLINE  Introduction: why the combination of Li.
1 Muon acceleration - amplitude effects in non-scaling FFAG - Shinji Machida CCLRC/RAL/ASTeC 26 April, ffag/machida_ ppt.
Harold G. Kirk Brookhaven National Laboratory Progress in Quad Ring Coolers Ring Cooler Workshop UCLA March 7-8, 2002.
1 Simulations of fast-ion instability in ILC damping ring 12 April ECLOUD 07 workshop Eun-San Kim (KNU) Kazuhito Ohmi (KEK)
A U.S. Department of Energy Office of Science Laboratory Operated by The University of Chicago Office of Science U.S. Department of Energy Containing a.
I PhysicsP I llinois George Gollin, Damping ring kickers, SLAC ILC-America, October Damping ring kickers George.
Preliminary results on simulation of fast-ion instability at 3 km LBNL damping ring 21 April 2005 Pohang Accelerator Laboratory Eun-San Kim.
Overview of Booster PIP II upgrades and plans C.Y. Tan for Proton Source group PIP II Collaboration Meeting 03 June 2014.
Beam Dynamics in the ESS Linac Under the Influence of Monopole and Dipole HOMs A.Farricker 1, R.M.Jones 1, R.Ainsworth 2 and S.Molloy 3 1 The University.
Aaron Farricker 107/07/2014Aaron Farricker Beam Dynamics in the ESS Linac Under the Influence of Monopole and Dipole HOMs.
LDRD: Magnetized Source JLEIC Meeting November 20, 2015 Riad Suleiman and Matt Poelker.
Bunch Separation with RF Deflectors D. Rubin,R.Helms Cornell University.
1 Fast kicker study Machine Time 2011/10/18~10/29(2 weeks) TB meeting 2011/01/14 T.Naito.
P I T Z Photo Injector Test Facility Zeuthen Design consideration of the RF deflector to optimize the photo injector at PITZ S.Korepanov.
July LEReC Review July 2014 Low Energy RHIC electron Cooling Jorg Kewisch, Dmitri Kayran Electron Beam Transport and System specifications.
Thomas Jefferson National Accelerator Facility Operated by the Southeastern Universities Research Association for the U.S. Department of Energy Harmonic.
SPring-8 upgrade : a fast kicker system for beam injection Japan Synchrotron Radiation Research Institute (JASRI) SPring-8 T. Nakamura CFA Beam Dynamics.
Robert R. Wilson Prize Talk John Peoples April APS Meeting: February 14,
S. Bettoni, R. Corsini, A. Vivoli (CERN) CLIC drive beam injector design.
1 Experiments with pulse supplies and strip-lines at ATF, Plans for fast extraction kicker for ATF2 1. Fast Kicker R&D at ATF 2. Instrumentation at ATF.
Bunched-Beam Phase Rotation - Ring Coolers? - FFAGs? David Neuffer Fermilab.
Longitudinal aspects on injection and acceleration for HP-PS Antoine LACHAIZE On behalf of the HP-PS design team.
Aaron Farricker 107/07/2014Aaron Farricker Beam Dynamics in the ESS Linac Under the Influence of Monopole and Dipole HOMs.
F Sergei Nagaitsev (FNAL) Webex meeting Oct ICD-2 chopper requirements and proposal #1.
Investigation of Injection Schemes for SLS 2.0
Progress Report on the Ultra-fast Harmonic Kicker Cavity Design and Beam Dynamic Simulation Yulu Huang 1,2 H. Wang 1, R. A. Rimmer 1, S. Wang 1 1.Thomas.
+-- Collider Front end- Balbekov version
S.M. Polozov & Ko., NRNU MEPhI
Sara Thorin, MAX IV Laboratory
Slice Parameter Measurements at the SwissFEL Injector Test Facility
Electron Cooling Simulation For JLEIC
Experimental Overview
Bunch Separation with RF Deflectors
Magnetized Bunched Electron Beam from DC High Voltage Photogun
Overview Multi Bunch Beam Dynamics at XFEL
CLIC DR EXTRACTION KICKER DESIGN, MANUFACTURE AND EXPERIMENTAL PROGRAM
R. Suleiman and M. Poelker September 29, 2016
PIs: Riad Suleiman and Matt Poelker
OSC simulation update Suntao Wang 10/06/2017.
MEBT1&2 design study for C-ADS
Kicker and RF systems for Damping Rings
Kicker specifications for Damping Rings
PIs: Riad Suleiman and Matt Poelker
He Zhang MEIC R&D Meeting, 07/09/2015
Injector for the Electron Cooler
JLEIC ion fullsize booster (2256m) space charge limit (Δν=0
Update on ERL Cooler Design Studies
H. Wang1, R. A. Rimmer1, S. Wang1, J. Guo1
Technical challenges for forming the double intensity section of JLEIC ion beam Jiquan Guo.
Update on Crab Cavity Simulations for JLEIC
Electron Cooling Work Plan for New Strong Cooling Baseline
JLEIC Main Parameters with Strong Electron Cooling
JLEIC CCR Path Length and Gap Formation
Evaluation of 1GHz vs 2GHz RF frequency in the damping rings
Cooler Ring Design Status - July 2017
Presentation transcript:

Fast kicker beam dynamics simulations A. Sy 05-28-2015

Fast kicker LDRD Fast kicker project aims to drive a transverse kicker with “CW” waveform generated by summing subharmonics of bunch frequency For n bunches in train, summed waveform has effective frequency of f/n Summed waveform applies transverse kick to every nth bunch, leaving other n-1 bunches undisturbed Beam dynamics simulations to investigate effects on both kicked and unkicked bunches 9/18/2019

Waveform generation Subharmonics of bunch frequency with appropriate amplitudes, zero phase offset sum to generate sharp kicking pulse Desired properties: Rise/fall time of kicking pulse == bunch spacing Zero amplitude, zero gradient at arrival times of unkicked bunches in train Applied transverse deflection vs. angular spread of kicked bunch

Waveform generation Initial bunch frequency f=476 MHz f = 0 MHz

Waveform generation f = 43 MHz

Waveform generation f = 87 MHz

Waveform generation f = 130 MHz

Waveform generation f = 173 MHz

Waveform generation f = 216 MHz

Waveform generation f = 260 MHz

Waveform generation f = 303 MHz

Waveform generation f = 346 MHz

Waveform generation f = 389 MHz

Waveform generation Effective bunch frequency f/(# bunches) For unkicked bunches, V=0, dV/dt = 0 f = 433 MHz

Nonuniformity of kicking pulse For full beam size of 2 mm transverse, 600 ps longitudinal (+/- 3σ) At head/tail of bunch, V = 0.85 Vpeak for f=748.5 MHz V = 0.934 Vpeak for f=476 MHz *Plots shown for f=748.5 MHz

Elegant simulations 55 MeV electrons to cool 100 GeV protons Bunch frequencies f=476, 748.5 MHz Kicker waveform generated using series of RF deflectors with appropriate phase and amplitude Kicked bunch circulates n times in cooler ring approximated by one-turn transfer matrix matched to initial bunch

Particle phase space plots x-x’, f=476 MHz, n=31 bunches Unkicked bunch Turn 2 Turn 8 Turn 21 Turn 30 Turn 31 Receives opposite kick

Particle phase space plots t-p, f=476 MHz, n=31 bunches No appreciable change in t-p phase space Unkicked bunch Turn 2 Turn 31

Growth of normalized emittance Red: 476 MHz Blue: 748.5 MHz Less than 2% growth of εnx for bunch length less than 5 cm 3% reduction of εny

Kick voltage amplitude 476 MHz Red: 5 kV Green: 20 kV Orange: 50 kV

Summary Nonuniformity of kicking pulse (up to 85% of peak voltage) does not seriously degrade transverse emittance of kicked bunch for relevant electron bunch lengths Further work to be done: Effects (if any) of residual waveform on unkicked bunches Verification of proper waveform generation in Elegant Replace one-turn matrix for cooler ring with more realistic design