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Eshraqi, M.

Paper Title Page
THP004 Layout and Machine Optimisation for the SPL at CERN 761
 
  • F. Gerigk, S. Atieh, S. Calatroni, O. Capatina, E. Ciapala, M. Eshraqi, L.M.A. Ferreira, R. Garoby, M. Hernandez Flano, W. Höfle, E. Lebbos, A.M. Lombardi, E. Montesinos, Th. Otto, V. Parma, P.A. Posocco, T. Renaglia, M. Schuh, V. Vlachoudis, W. Weingarten, S. Weisz
    CERN, Geneva
  • R. Calaga
    BNL, Upton, Long Island, New York
 
 

During the past 2 years the Superconducting Proton Linac (SPL) study has grown into an international collaboration with the goal of optimising the architecture of a pulsed superconducting (SC) high-power proton linac. This effort includes the study and prototyping of major technical components, such as SC high-gradient cavities, power couplers, the RF distribution system, HOM couplers, cryo-modules, focusing elements, etc. Even though the effort is driven by CERN specific needs, the established design principles are valid for a range of superconducting linac projects. In this paper we report on the latests decisions concerning the machine architecture and on the ongoing R&D effort for technical components.

 
THP005 Beam Dynamics Optimisation of Linac4 Structures for Increased Operational Flexibility 764
 
  • G. Bellodi, M. Eshraqi, M.G. Garcia Tudela, L.M. Hein, J.-B. Lallement, A.M. Lombardi, P.A. Posocco, E. Sargsyan
    CERN, Geneva
  • J. Stovall
    TechSource, Santa Fe, New Mexico
 
 

Linac4 is a new 160 MeV, 40 mA average beam current H- accelerator which will be the source of particles for all proton accelerators at CERN as from 2015. Construction started in October 2008, and beam commissioning of the 3MeV frontend is scheduled for early next year. A baseline design of the linac beam dynamics was completed 2 years ago and validated by a systematic campaign of transverse and longitudinal error studies to assess tolerance limits and machine activation levels. Recent studies have been mainly focused on optimising this design to achieve both a smoother performance for nominal beam conditions and to gain operational flexibility for non-nominal scenarios. These include a review of the chopper beam dynamics design, a re-definition of the DTL and CCDTL inter-tank regions and a study of operational schemes for reduced beam currents (either permanent or in pulse-to-pulse mode). These studies have been carried out in parallel to first specifications for a beam commissioning strategy of the linac and its low-energy front-end.

 
TU203 Plans for the ESS Linac 367
 
  • S. Peggs, M. Eshraqi, H. Hahn, A. Jansson, M. Lindroos, A. Ponton, K. Rathsman, C.G. Trahern
    ESS, Lund
  • S. Bousson
    IPN, Orsay
  • R. Calaga
    BNL, Upton, Long Island, New York
  • H. Danared
    MSL, Stockholm
  • G. Devanz, R.D. Duperrier
    CEA, Gif-sur-Yvette
  • J. Eguia
    Fundación TEKNIKER, Eibar (Gipuzkoa)
  • S. Gammino
    INFN/LNS, Catania
  • S.P. Møller
    ISA, Aarhus
  • C. Oyon
    SPRI, Bilbao
  • R.J.M.Y. Ruber
    Uppsala University, Uppsala
  • T. Satogata
    JLAB, Newport News, Virginia
 
 

Following selection of Lund as the site for the long-pulse ESS (European Spallation Source), a team of accelerator and target experts has been working on an update of the 2003 ESS linac design. Improvements to the 2003 design will be summarised, and the latest designs for the linac will be presented.

 

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Slides

 
THP003 Diagnostic Lines for the 160 MeV H- Linac4 at CERN 758
 
  • B. Mikulec, G. Bellodi, K. Hanke, T. Hermanns
    CERN, Geneva
  • M. Eshraqi
    ESS, Lund
 
 

Linac4 will be the new linear accelerator of the CERN accelerator chain delivering H- ions at 160 MeV from 2016. The increased injection energy compared to the 50 MeV of its predecessor Linac2, combined with a H- charge-exchange injection, will pave the way to reach ultimate goals for the LHC luminosity. Extensive commissioning for Linac4 is planned for the coming years. For this purpose, the beam will be studied after the exit of Linac4 in a straight line ending at the Linac4 dump, equipped with various beam instruments. An almost 180 m long transfer line will guide the beam to the charge exchange injection point at the entry of the Proton Synchrotron Booster. About 50 m upstream of this point, two measurement lines will be upgraded to perform transverse emittance measurements as well as energy and energy spread measurements of the Linac4 beam. A detailed description of the beam measurement principles and setups at these three Linac4 diagnostics lines related to distinct Linac4 commissioning phases will be given.