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McCormick, D.J.

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TH6PFP024 Beam Waist Manipulations at the ATF2 Interaction Point 3747
 
  • S. Bai, J. Gao, X.W. Zhu
    IHEP Beijing, Beijing
  • A.S. Aryshev
    JAI, Egham, Surrey
  • P. Bambade, T. Okugi
    KEK, Ibaraki
  • Y. Kamiya
    ICEPP, Tokyo
  • D.J. McCormick, M. Woodley
    SLAC, Menlo Park, California
  • M. Oroku, T. Yamanaka
    University of Tokyo, Tokyo
 
 

Funding: NSFC 10525525 and 10775154. CNRS-IN2P3 and ANR.


The ATF2 project is the final focus system prototype for ILC and CLIC linear collider projects, with a purpose to reach a 37nm vertical beam size at the interaction point. We report on techniques developed based on simulation studies to adjust the horizontal and vertical beam waists independently in the presence of errors, at two different IP locations where the beam size can be measured with different accuracies. During initial commissioning, we will start with larger than nominal β-functions at the IP, to reduce the effects from higher-order optical aberrations and thereby simplify the optical corrections needed. The first measurements in such intermediate β-configurations are reported.

 
FR5REP033 Next Generation Fast RF Interlock Module and VME-ATCA Adapter for ILC High Availability RF Test Station Demonstration 4841
 
  • R.S. Larsen, C. Adolphsen, D.J. McCormick, W.C. Ross, Z.M. Szalata
    SLAC, Menlo Park, California
  • R.W. Downing
    R.W. Downing Inc., Tucson
 
 

Funding: US Department of Energy Contract DE AC03 76SF00515.


The ILC R&D electronics program at SLAC includes development of key technologies aimed at improving reliability and availability and reducing cost. This paper discusses the development of high availability interlocks and controls for the L-Band high power RF stations. A new Fast Fault Finder (F3) VME module has been developed to process both slow interlocks using FPGA logic to detect the interlock trip excursions. This combination eliminates the need for separate PLC control of slow interlocks with modules chained together to accommodate as many inputs as needed. Next a high availability platform demonstration will port the F3’s via a specially designed VME adapter module into the new industry standard ATCA[1] crate (shelf). This high-availability platform features an Intelligent Platform Management (IPMI) system to control and monitor the health of the entire system, provide redundancy as needed for the application, and demonstrate auto-failover and hot-swap to minimize MTTR. The goal is to demonstrate “five nines” (0.99999) system availability at the shelf level. A new international initiative, the xTCA for Physics Standards Working Group, will be briefly mentioned.


[1] Advanced Telecom Computing Architecture

 
TH5RFP070 Nanometer Resolution Beam Position Monitor for the ATF2 Interaction Point Region 3603
 
  • A. Heo, E.-S. Kim, H.-S. Kim
    Kyungpook National University, Daegu
  • R. Ainsworth, S.T. Boogert, G.E. Boorman
    Royal Holloway, University of London, Surrey
  • Y. Honda, T. Tauchi, N. Terunuma
    KEK, Ibaraki
  • S.H. Kim, Y.J. Park
    PAL, Pohang, Kyungbuk
  • A. Lyapin, B. Maiheu, M. Wing
    UCL, London
  • J. May, D.J. McCormick, S. Molloy, J. Nelson, T.J. Smith, G.R. White
    SLAC, Menlo Park, California
  • S. Shin
    Fermilab, Batavia
  • D. Son
    CHEP, Daegu
  • D.R. Ward
    University of Cambridge, Cambridge
 
 

The ATF2 international collaboration is intending to demonstrate nanometer beam sizes required for the future Linear Colliders. The position of the electron beam focused down at the end of the ATF2 extraction line to a size as small as 35 nm has to be measured with nanometer resolution. For that purpose a special Interaction Point(IP) beam position monitor (BPM) was designed. In this paper we report on the features of the BPM and electronics design providing the required resolution. We also consider the results obtained with BPM triplet which was installed in the ATF beamline and the first data from ATF2 commissioning runs.

 
TH6REP025 Development of the S-Band BPM System for ATF2 4003
 
  • A. Lyapin, B. Maiheu, M. Wing
    UCL, London
  • R. Ainsworth, A.S. Aryshev, S.T. Boogert, G.E. Boorman, S. Molloy
    Royal Holloway, University of London, Surrey
  • A. Heo, E.-S. Kim, H.-S. Kim
    Kyungpook National University, Daegu
  • Y. Honda, T. Tauchi, N. Terunuma
    KEK, Ibaraki
  • D.J. McCormick, J. Nelson, G.R. White
    SLAC, Menlo Park, California
  • S. Shin
    Fermilab, Batavia
  • D.R. Ward
    University of Cambridge, Cambridge
 
 

The ATF2 international collaboration is intending to demonstrate nanometre beam sizes required for the future Linear Colliders. An essential part of the beam diagnostics needed to achieve this goal is the high resolution cavity beam position monitors (BPMs). In this paper we report on the S-band system installed in the final focus region of the new ATF2 extraction beamline. It only includes 4 BPMs, but they are mounted on the most critical final focus magnets squeezing the beam down to 35 nm. We discuss both the design and the first operational experience with the system.

 
TH6REP028 Development of the C-Band BPM System for ATF2 4009
 
  • S. Molloy, R. Ainsworth, S.T. Boogert, G.E. Boorman
    Royal Holloway, University of London, Surrey
  • A. Heo, E.-S. Kim, H.-S. Kim
    Kyungpook National University, Daegu
  • Y. Honda, T. Tauchi, N. Terunuma
    KEK, Ibaraki
  • A. Lyapin, B. Maiheu, M. Wing
    UCL, London
  • D.J. McCormick, J. Nelson, G.R. White
    SLAC, Menlo Park, California
  • S. Shin
    Fermilab, Batavia
  • D.R. Ward
    University of Cambridge, Cambridge
 
 

The ATF2 international collaboration is intending to demonstrate nanometre beam sizes required for the future Linear Colliders. An essential part of the beam diagnostics needed to achieve that goal is the high resolution cavity beam position monitors (BPMs). In this paper we report on the C-band system consisting of 32 BPMs spread over the whole length of the new ATF2 extraction beamline. We discuss the design of the BPMs and electronics, main features of the DAQ system, and the first operational experience with these BPMs.

 
FR1RAI03 ATF2 Commissioning 4205
 
  • A. Seryi, J.W. Amann, P. Bellomo, B. Lam, D.J. McCormick, J. Nelson, J.M. Paterson, M.T.F. Pivi, T.O. Raubenheimer, C.M. Spencer, M.-H. Wang, G.R. White, W. Wittmer, M. Woodley, Y.T. Yan, F. Zhou
    SLAC, Menlo Park, California
  • D. Angal-Kalinin, J.K. Jones
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
  • R. Apsimon, B. Constance, C. Perry, J. Resta-López, C. Swinson
    JAI, Oxford
  • S. Araki, A.S. Aryshev, H. Hayano, Y. Honda, K. Kubo, T. Kume, S. Kuroda, M. Masuzawa, T. Naito, T. Okugi, R. Sugahara, T. Tauchi, N. Terunuma, J. Urakawa, K. Yokoya
    KEK, Ibaraki
  • S. Bai, J. Gao
    IHEP Beijing, Beijing
  • P. Bambade, Y. Renier, C. Rimbault
    LAL, Orsay
  • G.A. Blair, S.T. Boogert, V. Karataev, S. Molloy
    Royal Holloway, University of London, Surrey
  • B. Bolzon, N. Geffroy, A. Jeremie
    IN2P3-LAPP, Annecy-le-Vieux
  • P. Burrows
    OXFORDphysics, Oxford, Oxon
  • G.B. Christian
    ATOMKI, Debrecen
  • J.-P. Delahaye, D. Schulte, R. Tomás, F. Zimmermann
    CERN, Geneva
  • E. Elsen
    DESY, Hamburg
  • E. Gianfelice-Wendt, M.C. Ross, M. Wendt
    Fermilab, Batavia
  • A. Heo, E.-S. Kim, H.-S. Kim
    Kyungpook National University, Daegu
  • J.Y. Huang, W.H. Hwang, S.H. Kim, Y.J. Park
    PAL, Pohang, Kyungbuk
  • Y. Iwashita, T. Sugimoto
    Kyoto ICR, Uji, Kyoto
  • Y. Kamiya
    ICEPP, Tokyo
  • S. Komamiya, M. Oroku, T.S. Suehara, T. Yamanaka
    University of Tokyo, Tokyo
  • A. Lyapin
    UCL, London
  • B. Parker
    BNL, Upton, Long Island, New York
  • T. Sanuki
    Tohoku University, Graduate School of Science, Sendai
  • A. Scarfe
    UMAN, Manchester
  • T. Takahashi
    Hiroshima University, Graduate School of Science, Higashi-Hiroshima
  • A. Wolski
    Cockcroft Institute, Warrington, Cheshire
 
 

ATF2 is a final-focus test beam line that attempts to focus the low-emittance beam from the ATF damping ring to a beam size of about 37 nm, and at the same time to demonstrate nm beam stability, using numerous advanced beam diagnostics and feedback tools. The construction is well advanced and beam commissioning of ATF2 has started in the second half of 2008. ATF2 is constructed and commissioned by ATF international collaborations with strong US, Asian and European participation.

 

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