Author: Kim, S.H.
Paper Title Page
WE2A04
Integration of Superconducting Solenoids in Long Cryomodules  
 
  • S.H. Kim, Z.A. Conway, M. Kedzie, M.P. Kelly, P.N. Ostroumov, T. Reid
    ANL, Argonne, Illinois, USA
  • W. McGhee
    Cryomagnetics, Inc., Tennessee, USA
 
  Superconducting (SC) solenoids provide efficient focusing of ion beams in SC linacs. This talk will discuss design, installation and operational experience of long cryomodules containing multiple SC solenoids. The techniques for the alignment of cavity-solenoid string will be presented. The solenoid assemblies include X-, Y-steering coils and does not require any iron shielding. The studies of SRF cavity properties after the quenching next to the solenoid will be presented.  
slides icon Slides WE2A04 [2.191 MB]  
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THPLR027 Progress Towards a 2.0 K Half-Wave Resonator Cryomodule for Fermilab's PIP-II Project 906
 
  • Z.A. Conway, A. Barcikowski, G.L. Cherry, R.L. Fischer, B.M. Guilfoyle, C.S. Hopper, M. Kedzie, M.P. Kelly, S.H. Kim, S.W.T. MacDonald, P.N. Ostroumov, T. Reid
    ANL, Argonne, Illinois, USA
  • V.A. Lebedev, A. Lunin
    Fermilab, Batavia, Illinois, USA
 
  Funding: This material is supported by the U.S. Department of Energy, Office of Science, Office of Nuclear Physics and Office of High-Energy Physics, Contracts No. DE-AC02-76-CH03000 and DE-AC02-06CH11357.
In support of Fermilab's Proton Improvement Plan-II project Argonne National Laboratory is constructing a superconducting half-wave resonator cryomodule. This cryomodule is designed to operate at 2.0 K, a first for low-velocity ion accelerators, and will accelerate ≥1 mA proton/H beams from 2.1 to 10.3 MeV. Since 2014 the construction of 9 162.5 MHz b = 0.112 superconducting half-wave resonators, the vacuum vessel and the majority of the cryomodule subsystems have been finished. Here we will update on the status of this work and report on preliminary cavity test results. This will include cavity performance measurements where we found residual resistances of < 3 nanoOhms at low fields and peak voltage gains of 5.9 MV, which corresponds to peak surface fields of 134 MV/m and 144 mT electric and magnetic respectively.
 
DOI • reference for this paper ※ https://doi.org/10.18429/JACoW-LINAC2016-THPLR027  
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