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Brooks, S.J.

Paper Title Page
WEPE098 Optimising Pion Production Target Shapes for the Neutrino Factory 3581
 
  • S.J. Brooks
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
 
 

The neu­tri­no fac­to­ry re­quires a source of pions with­in a mo­men­tum win­dow de­ter­mined by the ‘muon front end' ac­cel­er­a­tor struc­ture down­stream. The tech­nique of find­ing which parts of a large tar­get block are net ab­sorbers or emit­ters of par­ti­cles may be adapt­ed with this mo­men­tum win­dow in mind. There­fore, anal­y­sis of a hadron­ic pro­duc­tion sim­u­la­tion run using MARS15 can pro­vide a can­di­date tar­get shape in a sin­gle pass. How­ev­er, chang­ing the shape of the ma­te­ri­al also af­fects the ab­sorp­tion/emis­sion bal­ance, so this paper in­ves­ti­gates it­er­a­tive schemes to find a self-con­sis­tent op­ti­mal, or near-op­ti­mal, tar­get ge­om­e­try.

 
THPEC089 Overview of Solid Target Studies for a Neutrino Factory 4263
 
  • T.R. Edgecock
    STFC/RAL, Chilton, Didcot, Oxon
  • J.J. Back
    University of Warwick, Coventry
  • J.R.J. Bennett
    STFC/RAL/ISIS, Chilton, Didcot, Oxon
  • C.N. Booth, G.P. Skoro
    Sheffield University, Sheffield
  • S.J. Brooks
    STFC/RAL/ASTeC, Chilton, Didcot, Oxon
 
 

The UK pro­gramme of high power tar­get de­vel­op­ments for a Neu­tri­no Fac­to­ry is cen­tred on the study of high-Z ma­te­ri­als (tung­sten, tan­ta­lum). A de­scrip­tion of life­time shock tests on can­di­date ma­te­ri­als is given as part of the re­search into a solid tar­get so­lu­tion. A fast high cur­rent pulse is ap­plied to a thin wire of the sam­ple ma­te­ri­al and the life­time mea­sured from the num­ber of puls­es be­fore fail­ure. These mea­sure­ments are made at tem­per­a­tures up to ~2000 K. The stress on the wire is cal­cu­lat­ed using the LS-DY­NA code and com­pared to the stress ex­pect­ed in the real Neu­tri­no Fac­to­ry tar­get. It has been found that tan­ta­lum is too weak to sus­tain pro­longed stress at these tem­per­a­tures but a tung­sten wire has reached over 26 mil­lion puls­es (equiv­a­lent to more than ten years of op­er­a­tion at the Neu­tri­no Fac­to­ry). An ac­count is given of the op­ti­mi­sa­tion of sec­ondary pion pro­duc­tion from the tar­get and the is­sues re­lat­ed to mount­ing the tar­get in the muon cap­ture solenoid and tar­get sta­tion are dis­cussed.