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Lagrange, J.-B.

Paper Title Page
MOPEA039 Beam Study for FFAG Accelerator at KURRI 157
 
  • Y. Kuriyama, Y. Ishi, J.-B. Lagrange, Y. Mori, T. Planche, M. Takashima, T. Uesugi, E. Yamakawa
    KURRI, Osaka
  • H. Imazu, K. Okabe, I. Sakai, Y. Takahoko
    University of Fukui, Faculty of Engineering, Fukui
 
 

In Kyoto University Research Reactor Institute (KURRI), The FFAG accelerator complex for accelerator driven sub-critical reactor (ADSR) project has been already constructed and world first ADSR experiment has been done at May, 2009. In the main ring, proton beams of 11.5 MeV are injected and accelerated up to 100 MeV. During the acceleration, two different types of beam loss have been observed. To investigate these beam loss, betatron and synchrotron motion have been measured experimentally. The details of measurements will be described in this presentation.

 
TUOCRA03 Present Status and Future of FFAGs at KURRI and the First ADSR Experiment 1327
 
  • Y. Ishi, M. Inoue, Y. Kuriyama, J.-B. Lagrange, Y. Mori, T. Planche, M. Takashima, T. Uesugi, E. Yamakawa
    KURRI, Osaka
  • H. Imazu, K. Okabe, I. Sakai, Y. Takahoko
    University of Fukui, Faculty of Engineering, Fukui
 
 

World's first ADSR experiments which use spallation neutrons produced by high energy proton beams accelerated by the FFAG synchrotron has started since March 2009 at KURRI. In these experiments, the prompt and delayed neutrons which indicate neutron multiplication caused by external source have been detected. The accelerator complex for ADSR study in KURRI consists of three FFAG proton rings. It delivers the 100MeV proton beam to the W target located in front of the subcritical nuclear fuel system constructed in the reactor core of KUCA (Kyoto University Critical Assembly) at 30Hz repetition rate. Current status of the facility and the future plans of ADSR system and high intensity pulsed spallation neutron source which employ a newly added 700MeV FFAG synchrotron to the existing FFAG complex in KURRI will be presented.

 

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Slides

 
WEPE056 Accelerator and Particle Physics Research for the Next Generation Muon to Electron Conversion Experiment - the PRISM Task Force 3473
 
  • J. Pasternak, L.J. Jenner, Y. Uchida
    Imperial College of Science and Technology, Department of Physics, London
  • R.J. Barlow
    UMAN, Manchester
  • K.M. Hock, B.D. Muratori
    Cockcroft Institute, Warrington, Cheshire
  • D.J. Kelliher, S. Machida, C.R. Prior
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
  • Y. Kuno, A. Sato
    Osaka University, Osaka
  • A. Kurup
    Fermilab, Batavia
  • J.-B. Lagrange, Y. Mori
    KURRI, Osaka
  • M. Lancaster
    UCL, London
  • S.A. Martin
    FZJ, Jülich
  • C. Ohmori
    KEK/JAEA, Ibaraki-Ken
  • J. Pasternak
    STFC/RAL, Chilton, Didcot, Oxon
  • S.L. Smith
    STFC/DL/ASTeC, Daresbury, Warrington, Cheshire
  • H. Witte, T. Yokoi
    JAI, Oxford
 
 

The next generation of lepton flavour violation experiments will use high intensity and high quality muon beams. Such beams can be produced by sending a short proton pulse to the pion production target, capturing pions and performing RF phase rotation on the resulting muon beam in an FFAG ring, which was proposed for the PRISM project. A PRISM task force was created to address the accelerator and detector issues that need to be solved in order to realise the PRISM experiment. The parameters of the initial proton beam required and the PRISM experiment are reviewed. Alternative designs of the PRISM FFAG ring are presented and compared with the reference design. The ring injection/extraction system, matching with the solenoid channel and progress on the ring's main hardware systems like RF and kicker magnet are discussed. The activity on the simulation of a high sensitivity experiment and the impact on physics reach is described. The progress and future directions of the study are presented in this paper.

 
THPEB009 Development of H- Injection of Proton-FFAG at KURRI 3897
 
  • K. Okabe, R. Nakano, Y. Niwa, I. Sakai
    University of Fukui, Faculty of Engineering, Fukui
  • Y. Arakida
    KEK, Ibaraki
  • M. Inoue, Y. Ishi, Y. Kuriyama, J.-B. Lagrange, Y. Mori, T. Planche, T. Uesugi, E. Yamakawa
    KURRI, Osaka
 
 

In Kyoto University Research Reactor Institute (KURRI), the FFAG accelerator for accelerator driven sub-critical reactor (ADSR) system has been constructed and world's first ADSR experiments have started in March 2009. In order to upgrade beam intensity, multiturn charge exchange injection system for scaling FFAG accelerator is being studied. The 11MeV H- beam is injected from linac and is accelerated up to 100MeV in FFAG main ring. In this presentation, the detail of injection system is described and feasibility of such a low energy H- injection system is discussed.

 
THPD092 Applications of Advanced scaling FFAG Accelerator 4503
 
  • J.-B. Lagrange, Y. Ishi, Y. Kuriyama, Y. Mori, K. Okabe, T. Planche, T. Uesugi, E. Yamakawa
    KURRI, Osaka
 
 

Until today, scaling FFAG accelerator were only designed in a ring shape. But a new criteria of the magnetic field configuration satisfying the scaling condition even for straight FFAG beam line has been recently found. Moreover, combining different types of cells can be used to imagine new lattices. Various applications using these recent developments are here examined: inprovements of the PRISM project and the ERIT project, and a zero-chromatic carbon gantry concept are presented.

 
THPD093 New Approaches to Muon Acceleration with Zero-chromatic FFAGS 4506
 
  • T. Planche, Y. Ishi, Y. Kuriyama, J.-B. Lagrange, Y. Mori, K. Okabe, T. Uesugi, E. Yamakawa
    KURRI, Osaka
 
 

The acceleration of intense muon beams up to 25 GeV is the challenge of the international design work for a future neutrino factory. The present baseline scenario for muon acceleration is based on linacs, recirculating linear accelerators (RLAs) and non-scaling fixed field alternating gradient (FFAG) rings. However RLAs are one of the most cost driving part. Two new approaches to use zero-chromatic FFAG instead of RLA have been proposed. Detailed lattices parameters and 6D tracking results are presented.