HOM-BPM study in STF for cavity miss-alignment detection

Slides:



Advertisements
Similar presentations
Beam-based Measurements of HOMs in the HTC Adam Bartnik for ERL Team, Daniel Hall, John Dobbins, Mike Billing, Matthias Liepe, Ivan Bazarov.
Advertisements

Shuichi Noguchi, KEK6-th ILC School, November Beam-Operation Cavity Voltage Control by Feedback & Tuner Dumping of HOM’ s by HOM Dumper  Bunch Induced.
S. N. “ Cavities for Super B-Factory” 1 of 38 Sasha Novokhatski SLAC, Stanford University Accelerator Session April 20, 2005 Low R/Q Cavities for Super.
Main Linac Simulation - Main Linac Alignment Tolerances - From single bunch effect ILC-MDIR Workshop Kiyoshi KUBO References: TESLA TDR ILC-TRC-2.
OPTIMISATION OF BEAM INJECTION INTO THE FIRST ACCELERATING MODULE AT TTF2 WITH CAVITY DIPOLE MODE SIGNALS N. Baboi, H. Schlarb, M. Wendt, G. Kreps, DESY,
Test infrastructure and test programs at KEK-STF Kirk 2013/3/26TTC meeting
Accelerator R&D on LC - Activities of ATF & STF - 1. Introduction 2. ATF 3. STF 4. Summary Seiya Yamaguchi, KEK The US/Japan Collaboration in High Energy.
Zenghai Li SLAC National Accelerator Laboratory LHC-CC13 CERN, December 9-11, 2013 HOM Coupler Optimization & RF Modeling.
BPMs and HOM-BPMs for the XFEL Linac N. Baboi for the BPM and the HOM teams (DESY, CEA-Saclay, SLAC, FNAL, Cockroft/Daresbury) XFEL Linac Review Meeting,
Status of crab crossing studies Presented by NAKANISHI Kota (KEK) 2008/1/25.
E. KAKO (KEK) 2009' Dec. 22 S1-G Webex meeting Global Design Effort 1 Final Results of KEK Cavities for S1-Global Eiji Kako (KEK, Japan)
Preliminary design of SPPC RF system Jianping DAI 2015/09/11 The CEPC-SppC Study Group Meeting, Sept. 11~12, IHEP.
Photocathode 1.5 (1, 3.5) cell superconducting RF gun with electric and magnetic RF focusing Transversal normalized rms emittance (no thermal emittance)
STF Status and Future plan H. Hayano, KEK, LCWS12 Arlington System Test session 1.
High Current Electron Source for Cooling Jefferson Lab Internal MEIC Accelerator Design Review January 17, 2014 Riad Suleiman.
1 C. Simon CLIC Instrumentation workshop BPM C. Simon on behalf of the Saclay’s group CLIC Instrumentation workshop 2 nd - 3 rd June.
The Cavity Beam Position Monitor (BPM) Massimo Dal Forno Paolo Craievich, Raffaele De Monte, Thomas Borden, Andrea Borga, Mauro Predonzani, Mario Ferianis,
704MHz Warm RF Cavity for LEReC Binping Xiao Collider-Accelerator Department, BNL July 8, 2015 LEReC Warm Cavity Review Meeting  July 8, 2015.
Electron Source Configuration Axel Brachmann - SLAC - Jan , KEK GDE meeting International Linear Collider at Stanford Linear Accelerator Center.
2.1 GHz Warm RF Cavity for LEReC Binping Xiao Collider-Accelerator Department, BNL June 15, 2015 LEReC Warm Cavity Review Meeting  June 15, 2015.
Production and Installation Policy of IP-BPM ATF2 Project Meeting, 2006/12/18 Y. Honda, Y. Inoue, T. Hino, T. Nakamura.
Beam Loading experiment at KEK ATF ( Multi-train acceleration at KEK-ATF Injector ) KEK Masafumi Fukuda and Junji Urakawa LCWS /10/052 train acceleration.
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.
Beam Test status and Plans of the ILC Main LINAC BPM
Cavity Alignment Using Beam Induced Higher Order Mode Signals in the TTF LINAC Olivier Napoly, Rita Paparella CEA/DSM/DAPNIA, Gif-sur-Yvette Marc Ross,
E. KAKO (KEK) 2009' Oct. 26 ILC KEK Global Design Effort 1 Cavity Preparation for S1-Global Eiji Kako (KEK, Japan)
The Introduction to CSNS Accelerators Oct. 5, 2010 Sheng Wang AP group, Accelerator Centre,IHEP, CAS.
FLS2010 Workshop, Stanford, March 1-5, 2010 Florian Loehl (Cornell University) Commissioning of the High Current ERL Injector at Cornell Florian Loehl.
Debuncher Stochastic Cooling Paul Derwent March 3, 2016.
Cold BPM development in KEK H. Hayano, March 2011 Jung Keun Ahn (PNU), Sun young Ryu (PNU), Eun San Kim (KNU), Young Im Kim (KNU), Jin yeong Ryu (KNU),
2 nd Workshop of the IHEP 1.3 GHz SRF R&D Project and 2nd IHEP-KEK 1.3 GHz SRF Meeting Opening Remark J. Gao December 2-3, 2009, IHEP, Beijing, China.
First Electrons at the Fermilab superconducting test accelerator Elvin Harms Asian Linear Collider Workshop 2015, Tsukuba 24 April 2015.
Estimates of required MPS reaction time In the merger (at the centers of respective 20deg dipoles and in between 2 lenses) rms R=250 um In the
Beam plan at STF phase1 12/6/2005 TTC-WG3 H. Hayano STF phase1 1st step : DC-gun + photo-cathode (2006) quick beam source( DC gun exist), no pre-acceleration,
Aaron Farricker 107/07/2014Aaron Farricker Beam Dynamics in the ESS Linac Under the Influence of Monopole and Dipole HOMs.
HOMs in the TESLA 9-cell cavity HOMs in the XFEL and ILC Rainer Wanzenberg SPL HOM workshop CERN, June 25 – 26, 2009.
Shuichi NoguchiTTC Meeting at Milano, Injector Cryomodule for cERL at KEK Cavity 2 Prototypes were tested. Input Coupler 2 Couplers were tested.
Sub-Task HOM-BPM HOM based Beam Position Monitors – Planned and Extant Measurements N. Baboi, DESY, Hamburg EuCARD WP 10: SRF, Annual Review Meeting.
HWR, SSR1 and SSR2 transverse kick summary Paolo Berrutti, Vyacheslav Yakovlev.
HOMs in high-energy part of the Project-X linac. V. Yakovlev, N. Solyak, J.-F. Ostiguy Friday 26 June 2009.
RF Dipole HOM Electromagnetic Design
Re-entrant BPM R&D for ILC Main Linac
XFEL beamline loads and HOM coupler for CW
LLRF Research and Development at STF-KEK
An X-band system for phase space linearisation on CLARA
Andrei Shishlo ORNL SNS Project Florence, Italy November 2015
Higher Order Modes and Beam Dynamics at ESS
12.4: SRF HOM Diagnostics: Experimental Results and Future Plans
FPC Coupler RF Dipole Kick
CEPC injector high field S-band accelerating structure design and R&D
Update of CLIC accelerating structure design
KEK injector cryomodule
ERL Main-Linac Cryomodule
Overview Multi Bunch Beam Dynamics at XFEL
RF modes for plasma processing
Bunch Tiltmeter Steve Smith SLAC Snowmass July 16, 2001 Update date
Electron Source Configuration
CEPC Main Ring Cavity Design with HOM Couplers
Fabrication of KEK-ATF2 Q-BPM
2012/10/31 10am version… Abstract #: Conference: NSS (Oral)
Beam Position Measurements in TTF Cavities
HOM Based Beam Diagnostics in TESLA Superconducting Cavities at FLASH
High Precision SC Cavity Alignment Diagnostics with HOM Measurements
Accelerator Physics Particle Acceleration
High Charge Low Emittance RF Gun for SuperKEKB
Operational Experience with LCLS RF systems
Evgenij Kot XFEL beam dynamics meeting,
小型X線源の性能確認実験計画 高輝度・RF電子銃研究会 広島大学 高エネルギー加速器研究機構 浦川順治
Andrew Hutton Concept suggested independently by Haipeng Wang
Presentation transcript:

HOM-BPM study in STF for cavity miss-alignment detection A.Kuramoto Graduate University for Advanced Studies (KEK) TTC meeting at Jefferson Lab 5 November 2012

Purpose of research Find electric center of superconducting cavity by using beam induced HOM (dipole mode). Detect cavity miss-alignment of cavity offset, tilt and bending. Using two dipole modes. π/9 mode of 1st dipole passband Beam pipe mode

Idea Cavity center Find electric center in the middle of cavity by using π/9 mode of 1st dipole passband. Find electric center at beam pipe by using beam pipe mode. Detect cavity tilt and bending from combination of two electric centers. Cavity end Electric fields in a TDR-like TESLA 9-cell cavity calculated with magnetic boundary by R.Wanzenberg

requirement To detect π/9 mode -> use narrow band BPF +high gain RF amp. Big offset of electrical center is expected for beam pipe mode (main coupler, HOM coupler disturbance)-> bead-pull measurement is required.

Bead-pull measurement Example of measurement 2 1 S22 Ceramic bead is used. Electric field is measured in the left side beam pipe. 2.244 GHz 2.245 GHz

STF accelerator Beam energy : 40 MeV (RF Gun out 3 MeV) Bunch charge : 62 pC Number of bunch : 162500 (1 ms, 162.5 MHz) Repetition : 5 Hz SC cavity : 19 MV/m + 21 MV/m Dipole magnet B PM B PM e-

Set up for induced HOM measurement Dipole magnet B PM MHI-13 MHI-12 B PM e- 16 bunch 40pC/bunch HOM1 HOM2 DSO9404A (Agilent Technologies) A AMP A AMP A AMP HPF HPF highpass filter (Mini-Circuits) VHF-1500+ AMP (Mini-Circuits) ZX60-6013E+:gain=15dB BPF bandpass filter (Trilithic) 1.59-1.695 GHz 10.0 GSa/s,524 kpts

π/9 mode of 1st dipole passband Oscilloscope waveform π/9 mode’s spectrum is founded. Signal is small. Plot of amplitude vs. beam position doesn’t show V-shape.

Example of V-shape; 3π/9 mode of 1st dipole passband 3π/9 mode’s amplitude is big. Plot of amplitude vs. beam position for 3π/9 mode describes V-shape.

Beam pipe mode Oscilloscope waveform X position of Electric center for beam pipe mode is bigger than 3000 μm. Due to beam kick effect? Coupler is inserted from +X direction. The detail calculation is on going.

Summary The study of cavity miss-alignment (offset, tilt, bending) detection using beam induced HOM is presented. The beam induced HOM signals were detected by changing beam orbit. Measurement of electrical center to mechanical center is under performing by bead-pull method.

More detailed measurement is on a way in this STF beam run. Beam kick effect by coupler RF field is expected because Beam energy is too low (injection 3 MeV). More detailed measurement is on a way in this STF beam run. More high energy beam experiment and RF off experiment are required (for example at FLASH). end