BEPCII Transverse Feedback System Yue Junhui Beam Instrumentation Group IHEP , Beijing.

Slides:



Advertisements
Similar presentations
Beam Dynamics in MeRHIC Yue Hao On behalf of MeRHIC/eRHIC working group.
Advertisements

CEPC BoosterDesign CEPC Booster Design FCC Week 2015, March, 2015 Marriot Georgetown Hotel Huiping Geng Presented for Chuang Zhang.
SNS Accumulator Ring Instability Damper and Beam Transfer Function Studies Robert Hardin.
Damping ring K. Ohmi LC Layout Single tunnel Circumference 6.7 km Energy 5 GeV 2 km 35 km.
SuperB and the ILC Damping Rings Andy Wolski University of Liverpool/Cockcroft Institute 27 April, 2006.
DESIGN OF A 7-CELLS, HOM DAMPED, SUPERCONDUCTING CAVITY FOR THE STRONG RF FOCUSING EXPERIMENT AT DANE David Alesini, Caterina Biscari, Roberto Boni, Alessandro.
ALPHA Storage Ring Indiana University Xiaoying Pang.
Impedance measurements at SLS E. Koukovini-Platia CERN, EPFL TIARA mid-term meeting, Madrid, 13 th June 2012 Many thanks to M. Dehler, N. Milas, A. Streun.
A.Blas AB/RF/FB APC meeting 20/4/ Status of the PS TFB Upgrade launched in July 2005 L. Arnaudon, A. Blas, F. Caspers, D. Glenat, R. Louwerse, V.
STRIPLINE KICKER STATUS. PRESENTATION OUTLINE 1.Design of a stripline kicker for beam injection in DAFNE storage rings. 2.HV tests and RF measurements.
March 2, 2007ELC Experience with clearing voltages and solenoids at SPS damper pick-ups W. Hofle Acknowledgements PS-OP, SL-OP, SL-BI LHC-VAC, SL-HRF.
Few slides from J. Fox’ talk in last November’s LARP meeting LARP CM
BEPCII Transverse Feedback System Yue Junhui IHEP , Beijing Sep 17 th, 08IMAC.
Impedance and Collective Effects in BAPS Na Wang Institute of High Energy Physics USR workshop, Huairou, China, Oct. 30, 2012.
Preliminary design of SPPC RF system Jianping DAI 2015/09/11 The CEPC-SppC Study Group Meeting, Sept. 11~12, IHEP.
Feedback for CESR TA Michael Billing May 17, 2007.
1 Status of EMMA Shinji Machida CCLRC/RAL/ASTeC 23 April, ffag/machida_ ppt & pdf.
AAC February 4-6, 2003 Protons on Target Ioanis Kourbanis MI/Beams.
CAN WE BUILD A SINGLE BUNCH FEEDBACK Eric Plouviez ESRF Diagnostic group.
Beam dynamics on damping rings and beam-beam interaction Dec 포항 가속기 연구소 김 은 산.
Beam observation and Introduction to Collective Beam Instabilities Observation of collective beam instability Collective modes Wake fields and coupling.
Simulation of Beam Instabilities in SPring-8 T. Nakamura JASRI / SPring-8
January 19, 2006PEP TFB R.Akre PEP II Transverse Feedback System Ron Akre William Colocho Anatoly Krasnykh Vojtech Pacak Dmitry Teytelman Uli Wienands.
Managed by UT-Battelle for the Department of Energy Analysis of 2008 Beam Instability Data S. Cousineau, V. Danilov, M. Plum HB2008.
Summary of Booster Dampers Systems Dave McGinnis December 7, 2010.
Lecture 25 - E. Wilson - 12/15/ Slide 1 Lecture 6 ACCELERATOR PHYSICS HT E. J. N. Wilson
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.
High Bandwidth damper Input from W.Hölfe Acknowledgement to all collaborators at SLAC, INFN, LBNL and CERNL Presentation of recent MD results (J.Cesaratto):
BEPC II TIMING SYSTEM EPICS Seminar Presented by Ma zhenhan IHEP 20.August 2002.
Bunch by bunch feedback systems for KEKB Makoto Tobiyama KEK Accelerator Laboratory.
The SPS as a Damping Ring Test Facility for CLIC March 6 th, 2013 Yannis PAPAPHILIPPOU CERN CLIC Collaboration Working meeting.
R.SREEDHARAN  SOLEIL main parameters  Booster and storage ring low level RF system  New digital Booster LLRF system under development  Digital LLRF.
RF 1/33 ALBA RF system why, how and other questions Francis Perez.
The Introduction to CSNS Accelerators Oct. 5, 2010 Sheng Wang AP group, Accelerator Centre,IHEP, CAS.
Beam Physics Issue in BEPCII Commisionning Xu Gang Accelerator physics group.
2 February 8th - 10th, 2016 TWIICE 2 Workshop Instability studies in the CLIC Damping Rings including radiation damping A.Passarelli, H.Bartosik, O.Boine-Fankenheim,
 NICA is being constructed  For heavy ions we need very highluminosity level – 10 cm s  For keeping up such level we inevitably need cooling  Stochastic.
Characterization of the Fast Ion Instability at CesrTA David Rubin Cornell University.
LFB, LLRF, TFB Alessandro Drago Annecy, March 2010.
RF Commissioning D. Jacquet and M. Gruwé. November 8 th 2007D. Jacquet and M. Gruwé2 RF systems in a few words (I) A transverse dampers system ACCELERATING.
Beam Instrumentation of CEPC Yue Junhui (岳军会) for the BI Group Accelerator Center, IHEP HF2014.
Bunch by bunch feedback systems for KEKB Makoto Tobiyama KEK Accelerator Laboratory.
Coupled bunch Instabilities at ILC Damping Rings L. Wang SLAC ILC Damping Rings R&D Workshop - ILCDR06 September 26-28, 2006 Cornell University Refer to.
RF acceleration and transverse damper systems
PEP II Transverse Feedback System
PETRA III at DESY Hamburg/Germany
HOM coupler design and collective instability study
Working groups status report on Feedbacks
Failure analysis at BEPCII
LEIR IMPEDANCE AND INSTABILITY MEASUREMENTS
Cavity-beam interaction and Longitudinal beam dynamics for CEPC DR&APDR 宫殿君
Study on Beam Instability
Status of CEPC lattice design
Collective effects in CEPC
Limits on damping times
The LHC25ns cycle in the PS Triple splitting after 2nd injection
CEPC Injector Damping Ring
Design Study of the CEPC Booster
LHC (SSC) Byung Yunn CASA.
Instability measurement plans at ATF
PETRA IV System design concept Old and new machine
Lecture 6 ACCELERATOR PHYSICS HT E. J. N. Wilson
Institute of High Energy Physics Chinese Academy of Sciences
Injection design of CEPC
CEPC SRF Parameters (100 km Main Ring)
Damping Ring parameters with reduced bunch charge
Parameters Changed in New MEIC Design
RF Parameters for New 2.2 km MEIC Design
RF Parameters for New 2.2 km MEIC Design
Presentation transcript:

BEPCII Transverse Feedback System Yue Junhui Beam Instrumentation Group IHEP , Beijing

Outline Including three parts: The main parameters of BEPCII The coupled bunch instability The bunch by bunch feedback system

I : Some Parameters of BEPCII Beam Energy, E GeV 1.89 Circumference, C m Total beam current, A 0.91 Bunch current, mA 9.8 Revolution frequency, MHz RF frequency, MHz Harmonic Number, h 396 Tunes, 6.57/7.61/0.034 Radiation damping times, ms 25/25/12.5 Number of Bunches, B 93 Bunch spacing, m 2.4 Bunch frequency, MHz 125

The high beam current (0.9 A) and the large number of bunches (93 bunches) may cause the coupled bunch instabilities (CBI) in BEPCII Two source  The higher order modes (HOMs) of RF cavities  The resistive wall impedance Active feedback systems are required to suppress CBI II :The Coupled Bunch Instability

Bunch by bunch feedback system will be used on BEPCII The electronics bandwidth should be at least half of the bunch frequency  colliding mode 62.5MHz  synchronous radiation mode 250MHz The damping time of transverse feedback system is 0.5ms III: Bunch by bunch Transverse Feedback System

The Transverse Feedback System Schematic diagram Front-end electronics Signal processing system Kicker and power amplifier Parameters of Transverse Feedback System The experiments of BEPCII TFB

The Schematic Diagram of TFB System

The local station of the Transverse Feedback System

Transfer the signal whose bandwidth is 500MHz at the center frequency of 1.5GHz to base band. Detection frequency is 1.5GHz , triple of RF. Front-end electronics

Signal processing system Full analog system simply using the cable line Three functions  Making the 90 phase shift  Rejection the closed orbit signal  One turn delay Realization  Two manual attenuators for 90 phase shift control  Notch filter rejection the revolution frequency  The time delay by cable

Signal processing system - Phase shift and Notch Filter

Kicker and Power Amplifier Four strip line electrode as kicker (considering it is easy to realize, so the kicker length is 600mm just for every other bunches) One kicker per ring because the limited space Model 75A250A power amplifier is selected. Two 75A250A are connected in the differential style

Kicker and Power Amplifier

Specifications of the TFB system RF frequency MHz Bunch spacing ns 8 Feedback damping time ms 0.5 Detection frequency GHz 1.5 Number of kickers per plane per ring 1 Kicker shunt impedance (at 125MHz) k  3.0 Total damping voltage per turn V 800 Kicker power for 800 V w 106 Number of power amplifiers per plane per ring 2 Bandwidth of power amplifier MHz 250

The experiments of BEPCII TFB(1) With TFB system off, we can observe the vertical and the horizontal sidebands.

Only turn on the y direction TFB , the vertical sidebands disappear and the horizontal sidebands become strong. The experiments of BEPCII TFB(2)

Turn on x direction TFB, the horizontal sidebands also disappear, the beam size become smaller. The experiments of BEPCII TFB(3)

Conclusion In a word , This system can restrain coupled bunch instabilities. But stable and continued run need more efforts and more experiences 。 Other parameters need to measure in the future study 。

Thank you very much!