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Fraction of electrons in the T9 pion beams
In the T9 beam line, the beam instrumentation does not permit the separation of electrons from pions, except for the 1:5, 3 and 5 GeV/c beam momenta. For beam momenta of 8 GeV/c or higher, the flux of beam electrons must be subtracted from the flux of pion-like particles incident on the target in or...
Autores principales: | , , , , , , , , , , , , , , |
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Lenguaje: | eng |
Publicado: |
2008
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Materias: | |
Acceso en línea: | http://cds.cern.ch/record/1142663 |
Sumario: | In the T9 beam line, the beam instrumentation does not permit the separation of electrons from pions, except for the 1:5, 3 and 5 GeV/c beam momenta. For beam momenta of 8 GeV/c or higher, the flux of beam electrons must be subtracted from the flux of pion-like particles incident on the target in order to obtain correct pion interaction cross-sections. In this memo, data from the beam instrumentation and the electron-identifier in `empty-target' runs are analysed in order to determine the fraction of electrons incident on the target, in the pion beams from 1.5 to 15 GeV/c. |
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