The MICE Muon Beam on ISIS and the beamline instrumentation of the Muon Ionization Cooling Experiment The MICE Collaboration

M. Bogomilov, Y. Karadzhov,D. Kolev, I. Russinov,R. Tsenov,G. Vankova-Kirilova,L. Wang,F. Y. Xu, S. X. Zheng, R. Bertoni,M. Bonesini,F. Ferri, G. Lucchini, R. Mazza, F. Paleari, F. Strati, V. Palladino, G. Cecchet,A. de Bari, M. Capponi, A. Cirillo, A. Iaciofano, A. Manfredini,M. Parisi, D. Orestano, F. Pastore, A. Tonazzo, L. Tortora,Y. Mori,H. Sakamoto,A. Sato, S. Ishimoto, S. Suzuki,K. Yoshimura,F. Filthaut, R. Garoby, S. Gilardoni,P. Gruber, K. Hanke, H. Haseroth,P. Janot, A. Lombardi, S. Ramberger,M. Vretenar, P. Bene,A. Blondel, F. Cadoux, J.-S. Graulich, V. Grichine, E. Gschwendtner,F. Masciocchi, R. Sandstrom,V. Verguilov, H. Wisting,C. Petitjean,R. Seviour, J. Alexander, G. Charnley,N. Collomb, S. Griffiths, R. Apsimon,P. Barclay,D. E. Baynham, T. W. Bradshaw, M. Courthold, P. Drumm,R. Edgecock, T. Hayler,M. Hills, Y. Ivaniouchenkov, A. Jones, A. Lintern, C. MacWaters, C. Nelson, A. Nichols, R. Preece, S. Ricciardi, J. H. Rochford, C. Rogers, W. Spensley,J. Tarrant, K. Tilley, S. Watson, A. Wilson

semanticscholar(2012)

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摘要
The international Muon Ionization Cooling Experiment (MICE), which is under construction at the Rutherford Appleton Laboratory (RAL), will demonstrate the principle of ionization cooling as a technique for the reduction of the phase-space volume occupied by a muon beam. Ionization cooling channels are required for the Neutrino Factory and the Muon Collider. MICE will evaluate in detail the performance of a single lattice cell of the Feasibility Study 2 cooling channel. The MICE Muon Beam has been constructed at the ISIS synchrotron at RAL, and in MICE Step I, it has been characterized using the MICE beam-instrumentation system. In this paper, the MICE Muon Beam and beam-line instrumentation are described. The muon rate is presented as a function of the beam loss generated by the MICE target dipping into the ISIS proton beam. For a 1 V signal from the ISIS beam-loss monitors downstream of our target we obtain a 30 KHz instantaneous muon rate, with a neglible pion contamination in the beam.
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