Author: Velianoff, G.J.
Paper Title Page
MOPO009 Design Status of the SRF Linac Systems for the Facility for Rare Isotope Beams 56
 
  • M. Leitner, J. Bierwagen, J. Binkowski, S. Bricker, C. Compton, J.L. Crisp, L.J. Dubbs, K. Elliott, A. Facco, A. Fila, R. Fontus, A.D. Fox, P.E. Gibson, P. Guetschow, L.L. Harle, M. Hodek, J.P. Holzbauer, M.J. Johnson, S. Jones, T. Kole, B.R. Lang, D. Leitner, I.M. Malloch, F. Marti, D. R. Miller, S.J. Miller, T. Nellis, D. Norton, R. Oweiss, J. Popielarski, L. Popielarski, X. Rao, G.J. Velianoff, N. Verhanovitz, J. Wei, J. Weisend, M. Williams, K. Witgen, J. Wlodarczak, Y. Xu, Y. Zhang
    FRIB, East Lansing, Michigan, USA
 
  Funding: This material is based upon work supported by the U.S. Department of Energy Office of Science under Cooperative Agreement DE-SC0000661
The Facility for Rare Isotope Beams (FRIB) will utilize a powerful, superconducting heavy-ion driver linac to provide stable ion beams from protons to uranium, at energies of > 200 MeV/u at a beam power of up to 400 kW. ECR ion sources installed above ground will be used to provide highly charged ions, that will be transported into the linac tunnel approx. 10 m below ground. For the heaviest ions, two charge states will be accelerated to about 0.5 MeV/u using a room-temperature 80.5 MHz RFQ and injected into a superconducting cw linac, consisting of 112 quarter-wave (80.5 MHz) and 229 half-wavelength (322 MHz) cavities, installed inside 52 cryomodules operating at 2K. A single stripper section will be located at about 17 MeV/u (for uranium). Transverse focusing along the linac will be achieved by 9 T superconducting solenoids within the same cryostat as the superconducting rf accelerating structures. This paper describes the matured linac design, as the project is progressing towards a Department of Energy performance baseline definition in 2012. Development status of the linac subcomponents are presented with emphasis on the superconducting RF components.
 
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