The LEP Superconducting RF system has reached its maximum configuration of 288 four-cell cavities powered by 36 klystrons in 1999. In 2000, this system,

Slides:



Advertisements
Similar presentations
Status and Future of BESSY RF BESSY II operating since 1999 Willy Wien Laboratory groundbreaking 9/2004 HoBiCaT Testfacility for sc cavities Commissioning.
Advertisements

Thomas Jefferson National Accelerator Facility CWL/Kovar/March 1, 2007 Page 1 Determining Loaded-Q for SRF Cavities Used In ERLs (What do you mean it is.
Tom Powers Practical Aspects of SRF Cavity Testing and Operations SRF Workshop 2011 Tutorial Session.
11/27/2007ILC Power and Cooling VM Workshop Mike Neubauer 1 RF Power and Cooling Requirements Overview from “Main Linac Power and Cooling Information”
Final Design of a CW Radio-Frequency Quadrupole (RFQ) for the Project X Injector Experiment (PXIE)* Abstract: The Project X Injector Experiment (PXIE)
Advanced accelerator research with focus on plasma wakefield acceleration, University of Oslo, Erik Adli, University of Oslo, August 2014,
ESS End-to-End Optics and Layout Integration Håkan Danared European Spallation Source Catania, 6 July 2011.
KAGEYAMA, T. Open Meeting for Proto-Collaboration March 19, 2008.
Thomas Roser Snowmass 2001 June 30 - July 21, MW AGS proton driver (M.J. Brennan, I. Marneris, T. Roser, A.G. Ruggiero, D. Trbojevic, N. Tsoupas,
Beam Dynamics Tutorial, L. Rivkin, EPFL & PSI, Prague, September 2014 Synchrotron radiation in LHC: spectrum and dynamics The Large Hadron Collider (LHC)
Options for a 50Hz, 10 MW, Short Pulse Spallation Neutron Source G H Rees, ASTeC, CCLRC, RAL, UK.
(ISS) Topics Studied at RAL G H Rees, RAL, UK. ISS Work Areas 1. Bunch train patterns for the acceleration and storage of μ ± beams. 2. A 50Hz, 1.2 MW,
LEP3 RF System: gradient and power considerations Andy Butterworth BE/RF Thanks to R. Calaga, E. Ciapala.
Progress of SRF and ERL at Peking University Lu Xiangyang Institute of Heavy Ion Physics Peking University.
Dark Current Measurements and Simulations Chris Adolphsen 2/4/15.
Preliminary design of SPPC RF system Jianping DAI 2015/09/11 The CEPC-SppC Study Group Meeting, Sept. 11~12, IHEP.
Accelerator Physics with Relativity By Mark, Jack and Frances (Designing the LHC in an hour and a half)
High Power RF Systems, Control and Distribution in the HINS Alfred Moretti, Brian Chase, Chris Jensen and Peter Prieto Fermilab Accelerator Advisory Committee.
Christopher Nantista ARD R&D Status Meeting SLAC February 3, …… …… …… … ….
EDM2001 Workshop May 14-15, 2001 AGS Intensity Upgrade (J.M. Brennan, I. Marneris, T. Roser, A.G. Ruggiero, D. Trbojevic, N. Tsoupas, S.Y. Zhang) Proton.
February 17-18, 2010 R&D ERL Alex Zaltsman R&D ERL High Power RF Systems Alex Zaltsman February 17-18, 2010 High Power RF Systems.
RF Development for ESS Roger Ruber and Volker Ziemann Uppsala Universitet 4 Dec Dec-20091RR+VZ: ESS RF Development.
Design of an Isochronous FFAG Ring for Acceleration of Muons G.H. Rees RAL, UK.
Accelerator Laboratory 1 CFS Review of Asian Region (S. Fukuda) June 1/ Hz Operation in DRFS HLRF System KEK S. Fukuda.
Cavities Auto Recovery with Beam RF&Linac Section - ALBA Accelerators Division Francis Perez Angela Salom.
Accelerator Group for LHeC LHeC Meeting at CERN; October Questions raised by Max  does the e-ring fit into the tunnel?  can one bypass ATLAS and.
Proton Driver Main Linac Parameter Optimization G. W. Foster Proton Driver General Meeting Jan 19, 2005.
Machine Protection at the 1MW CEBAF Electron Accelerator and Free Electron Laser Facility Kelly Mahoney Presented at the Workshop for.
PROTON LINAC FOR INDIAN SNS Vinod Bharadwaj, SLAC (reporting for the Indian SNS Design Team)
Linac RF Source Recommendations for Items 22,23,24,46,47 Chris Adolphsen.
RF Tutorial G Burt. TM 010 Monopole Mode E H Beam Z 0 =377 Ohms.
Status of the International Linear Collider and Importance of Industrialization B Barish Fermilab 21-Sept-05.
Aug 23, 2006 Half Current Option: Impact on Linac Cost Chris Adolphsen With input from Mike Neubauer, Chris Nantista and Tom Peterson.
Design Optimization of MEIC Ion Linac & Pre-Booster B. Mustapha, Z. Conway, B. Erdelyi and P. Ostroumov ANL & NIU MEIC Collaboration Meeting JLab, October.
Cold versus Warm, parameters impacting LC reliability and efficiency contribution to the discussion on risk factors Giorgio Bellettini, Seul ITRP meeting,
ParameterL-bandS-bandX-band Length (m) Aperture 2a (mm) Gradient (Unloaded/Loaded) (MV/m)17/1328/2250/40 Power/structure (MW) Beam.
RF 1/33 ALBA RF system why, how and other questions Francis Perez.
Comparison of Fermilab Proton Driver to Suggested Energy Amplifier Linac Bob Webber April 13, 2007.
THE DESIGN OF THE AGS-BASED PROTON DRIVER FOR NEUTRINO FACTORY W.T. WENG, BNL FFAG WORKSHOP JULY 7-11, 2003 KEK, JAPAN.
Progress and Plans for R&D and the Conceptual Design of the ILC Main Linacs H. Hayano, KEK PAC2005 5/18/2005.
Operational experience of high-power RF at Diamond Light Source
Jan Low Energy 10 Hz Operation in DRFS (Fukuda) (Fukuda) 1 Low Energy 10Hz Operation in DRFS S. Fukuda KEK.
1 Consequences of RF system failures during LHC beam commissioning T.Linnecar AB-RF.
CW and High Average Power Workshop BNL The Diamond Storage Ring IOT based High Power Amplifier Morten Jensen on behalf of the SR RF Group.
Stefan Wilke, DESY MHF-e 1 12th ESLS RF Meeting 1 st October, 2008 at DIAMOND Overview and Status of Assembling and Commissioning the RF-System at PETRA.
ALBA RF Systems Francis Perez.
HISTORY OF SNS DESIGN AND TECHNOLOGY CHOICES PROJECT X WORKSHOP NOVEMBER 12-13, 2007 R. KUSTOM.
Presenter : Yang Wu McMaster University Work conducted at IHEP.
PSI, Zurich February 29 – March Session classification : Accelerator Concepts Tuesday, March 1, 2016 Summary Vyacheslav Yakovlev Fermilab, USA.
Shuichi NoguchiTTC Meeting at Milano, Injector Cryomodule for cERL at KEK Cavity 2 Prototypes were tested. Input Coupler 2 Couplers were tested.
A CW Linac scheme for CLIC drive beam acceleration. Hao Zha, Alexej Grudiev 07/06/2016.
Operation Status of the RF Systems and Taiwan Photon Source
ILC Power and Cooling VM Workshop
Syratchev(CERN) on behalf of
SOLEIL EXPERIENCE WITH HIGH POWER SOLID STATE AMPLIFIERS
CLIC Civil Engineering & Infrastructure Working Group Meeting
CEPC APDR Study Zhenchao LIU
Q &A for the questions from CFS of April 29,2011
DRFS and Low Energy 10 Hz Option
BEPCII RF POWER SOURCE AND INPUT COUPLER
Accelerator Layout and Parameters
CEPC RF Power Sources System
A Superconducting Proton/Electron Linac
Status and New Developments of ALBA RF Systems
CEPC APDR SRF considerations(4) -LEP Cavity Voltage &BBU
Operational Experience with LCLS RF systems
Status and New Developments of ALBA RF Systems
Used PEP-II 476 MHz Cavities for MEIC Collider Rings
Summary of the maximum SCRF voltage in XFEL
RF Parameters for New 2.2 km MEIC Design
Presentation transcript:

The LEP Superconducting RF system has reached its maximum configuration of 288 four-cell cavities powered by 36 klystrons in 1999. In 2000, this system, together with 56 cavities of the original copper RF system, routinely provided more than 3630 MV, allowing the beam energy to be raised up to 104.5 GeV. This has required not only operating the cavities more than 15% above their design gradient, but has also demanded a very high operational reliability from the entire system. Since 1995 energy upgrade from 45 GeV / beam with Superconducting cavities up to 104.5 GeV From 360 MV --> 3666 MV LEP circumference : 26.7 km, RF system in four straight sections one-cavity segment of module * 18 Power converter 100 kV / 40 A + 22 control racks in klystron tunnel RF Power Plant for SC cavities 8 cavities per klystron two 1.3 MW RF klystrons per 4 MW DC power supply Interlock trips lead to loss of accelerating voltage: RF trip: 8 cavites off, loss of about 100 MV ! High Voltage trip: 16 cavities off, loss of about 200 MV ! 1.3 MW cw klystron main cavity parameters