Abstract
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.
| Original language | English |
|---|---|
| Article number | P05009 |
| Number of pages | 37 |
| Journal | Journal of Instrumentation |
| Volume | 7 |
| Issue number | 5 |
| DOIs | |
| Publication status | Published - 23 May 2012 |
| Externally published | Yes |
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The MICE Muon Beam on ISIS and the beam-line instrumentation of the Muon Ionization Cooling Experiment. / Bogomilov, M.; Karadzhov, Y.; Kolev, D.; Russinov, I.; Tsenov, R.; Vankova-Kirilova, G.; Wang, L.; Xu, F. Y.; Zheng, S. X.; Bertoni, R.; Bonesini, M.; Ferri, F.; Lucchini, G.; Mazza, R.; Paleari, F.; Strati, F.; Palladino, V.; Cecchet, G.; De Bari, A.; Capponi, M.; Cirillo, A.; Iaciofano, A.; Manfredini, A.; Parisi, M.; Orestano, D.; Pastore, F.; Tonazzo, A.; Tortora, L.; Mori, Y.; Kuno, Y.; Sakamoto, H.; Sato, A.; Yano, T.; Yoshida, M.; Ishimoto, S.; Suzuki, S.; Yoshimura, K.; Filthaut, F.; Garoby, R.; Gilardoni, S.; Gruber, P.; Hanke, K.; Haseroth, H.; Janot, P.; Lombardi, A.; Ramberger, S.; Vretenar, M.; Bene, P.; Blondel, A.; Cadoux, F.; Graulich, J. S.; Grichine, V.; Gschwendtner, E.; Masciocchi, F.; Sandstrom, R.; Verguilov, V.; Wisting, H.; Petitjean, C.; Seviour, R.; Alexander, J.; Charnley, G.; Collomb, N.; Griffiths, S.; Martlew, B.; Moss, A.; Mullacrane, I.; Oates, A.; Owens, P.; White, C.; York, S.; Adams, D.; Apsimon, R.; Barclay, P.; Baynham, D. E.; Bradshaw, T. W.; Courthold, M.; Drumm, P.; Edgecock, R.; Hayler, T.; Hills, M.; Ivaniouchenkov, Y.; Jones, A.; Lintern, A.; MacWaters, C.; Nelson, C.; Nichols, A.; Preece, R.; Ricciardi, S.; Rochford, J. H.; Rogers, C.; Spensley, W.; Tarrant, J.; Tilley, K.; Watson, S.; Wilson, A.; Forrest, D.; Soler, F. J.P.; Walaron, K.; Cooke, P.; Gamet, R.; Alekou, A.; Apollonio, M.; Barber, G.; Beuselinck, R.; Clark, D.; Clark, I.; Colling, D.; Dobbs, A.; Dornan, P.; Fayer, S.; Fish, A.; Hare, R.; Greenwood, S.; Jamdagni, A.; Kasey, V.; Khaleeq, M.; Leaver, J.; Long, K.; McKigney, E.; Matsushita, T.; Pasternak, J.; Sashalmi, T.; Savidge, T.; Takahashi, M.; Blackmore, V.; Carlisle, T.; Cobb, J. H.; Lau, W.; Rayner, M.; Tunnell, C. D.; Witte, H.; Yang, S.; Booth, C. N.; Hodgson, P.; Howlett, L.; Nicholson, R.; Overton, E.; Robinson, M.; Smith, P.; Adey, D.; Back, J.; Boyd, S.; Harrison, P.; Ellis, M.; Kyberd, P.; Littlefield, M.; Nebrensky, J. J.; Bross, A. D.; Geer, S.; Neuffer, D.; Moretti, A.; Popovic, M.; Cummings, M. A.C.; Roberts, T. J.; Demello, A.; Green, M. A.; Li, D.; Virostek, S.; Zisman, M. S.; Freemire, B.; Hanlet, P.; Huang, D.; Kafka, G.; Kaplan, D. M.; Snopok, P.; Torun, Y.; Blot, S.; Kim, Y. K.; Bravar, U.; Onel, Y.; Cline, D.; Fukui, Y.; Lee, K.; Yang, X.; Rimmer, R. A.; Cremaldi, L. M.; Gregoire, G.; Hart, T. L.; Sanders, D. A.; Summers, D. J.; Coney, L.; Fletcher, R.; Hanson, G. G.; Heidt, C.; Gallardo, J.; Kahn, S.; Kirk, H.; Palmer, R. B.
In: Journal of Instrumentation, Vol. 7, No. 5, P05009, 23.05.2012.Research output: Contribution to journal › Article
TY - JOUR
T1 - The MICE Muon Beam on ISIS and the beam-line instrumentation of the Muon Ionization Cooling Experiment
AU - Bogomilov, M.
AU - Karadzhov, Y.
AU - Kolev, D.
AU - Russinov, I.
AU - Tsenov, R.
AU - Vankova-Kirilova, G.
AU - Wang, L.
AU - Xu, F. Y.
AU - Zheng, S. X.
AU - Bertoni, R.
AU - Bonesini, M.
AU - Ferri, F.
AU - Lucchini, G.
AU - Mazza, R.
AU - Paleari, F.
AU - Strati, F.
AU - Palladino, V.
AU - Cecchet, G.
AU - De Bari, A.
AU - Capponi, M.
AU - Cirillo, A.
AU - Iaciofano, A.
AU - Manfredini, A.
AU - Parisi, M.
AU - Orestano, D.
AU - Pastore, F.
AU - Tonazzo, A.
AU - Tortora, L.
AU - Mori, Y.
AU - Kuno, Y.
AU - Sakamoto, H.
AU - Sato, A.
AU - Yano, T.
AU - Yoshida, M.
AU - Ishimoto, S.
AU - Suzuki, S.
AU - Yoshimura, K.
AU - Filthaut, F.
AU - Garoby, R.
AU - Gilardoni, S.
AU - Gruber, P.
AU - Hanke, K.
AU - Haseroth, H.
AU - Janot, P.
AU - Lombardi, A.
AU - Ramberger, S.
AU - Vretenar, M.
AU - Bene, P.
AU - Blondel, A.
AU - Cadoux, F.
AU - Graulich, J. S.
AU - Grichine, V.
AU - Gschwendtner, E.
AU - Masciocchi, F.
AU - Sandstrom, R.
AU - Verguilov, V.
AU - Wisting, H.
AU - Petitjean, C.
AU - Seviour, R.
AU - Alexander, J.
AU - Charnley, G.
AU - Collomb, N.
AU - Griffiths, S.
AU - Martlew, B.
AU - Moss, A.
AU - Mullacrane, I.
AU - Oates, A.
AU - Owens, P.
AU - White, C.
AU - York, S.
AU - Adams, D.
AU - Apsimon, R.
AU - Barclay, P.
AU - Baynham, D. E.
AU - Bradshaw, T. W.
AU - Courthold, M.
AU - Drumm, P.
AU - Edgecock, R.
AU - Hayler, T.
AU - Hills, M.
AU - Ivaniouchenkov, Y.
AU - Jones, A.
AU - Lintern, A.
AU - MacWaters, C.
AU - Nelson, C.
AU - Nichols, A.
AU - Preece, R.
AU - Ricciardi, S.
AU - Rochford, J. H.
AU - Rogers, C.
AU - Spensley, W.
AU - Tarrant, J.
AU - Tilley, K.
AU - Watson, S.
AU - Wilson, A.
AU - Forrest, D.
AU - Soler, F. J.P.
AU - Walaron, K.
AU - Cooke, P.
AU - Gamet, R.
AU - Alekou, A.
AU - Apollonio, M.
AU - Barber, G.
AU - Beuselinck, R.
AU - Clark, D.
AU - Clark, I.
AU - Colling, D.
AU - Dobbs, A.
AU - Dornan, P.
AU - Fayer, S.
AU - Fish, A.
AU - Hare, R.
AU - Greenwood, S.
AU - Jamdagni, A.
AU - Kasey, V.
AU - Khaleeq, M.
AU - Leaver, J.
AU - Long, K.
AU - McKigney, E.
AU - Matsushita, T.
AU - Pasternak, J.
AU - Sashalmi, T.
AU - Savidge, T.
AU - Takahashi, M.
AU - Blackmore, V.
AU - Carlisle, T.
AU - Cobb, J. H.
AU - Lau, W.
AU - Rayner, M.
AU - Tunnell, C. D.
AU - Witte, H.
AU - Yang, S.
AU - Booth, C. N.
AU - Hodgson, P.
AU - Howlett, L.
AU - Nicholson, R.
AU - Overton, E.
AU - Robinson, M.
AU - Smith, P.
AU - Adey, D.
AU - Back, J.
AU - Boyd, S.
AU - Harrison, P.
AU - Ellis, M.
AU - Kyberd, P.
AU - Littlefield, M.
AU - Nebrensky, J. J.
AU - Bross, A. D.
AU - Geer, S.
AU - Neuffer, D.
AU - Moretti, A.
AU - Popovic, M.
AU - Cummings, M. A.C.
AU - Roberts, T. J.
AU - Demello, A.
AU - Green, M. A.
AU - Li, D.
AU - Virostek, S.
AU - Zisman, M. S.
AU - Freemire, B.
AU - Hanlet, P.
AU - Huang, D.
AU - Kafka, G.
AU - Kaplan, D. M.
AU - Snopok, P.
AU - Torun, Y.
AU - Blot, S.
AU - Kim, Y. K.
AU - Bravar, U.
AU - Onel, Y.
AU - Cline, D.
AU - Fukui, Y.
AU - Lee, K.
AU - Yang, X.
AU - Rimmer, R. A.
AU - Cremaldi, L. M.
AU - Gregoire, G.
AU - Hart, T. L.
AU - Sanders, D. A.
AU - Summers, D. J.
AU - Coney, L.
AU - Fletcher, R.
AU - Hanson, G. G.
AU - Heidt, C.
AU - Gallardo, J.
AU - Kahn, S.
AU - Kirk, H.
AU - Palmer, R. B.
PY - 2012/5/23
Y1 - 2012/5/23
N2 - 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.
AB - 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.
KW - Accelerator Applications
KW - Calorimeters
KW - Instrumentation and methods for time-of-flight (TOF) spectroscopy
KW - Instrumentation for particle accelerators and storage rings - low energy (linear accelerators, cyclotrons, electrostatic accelerators)
UR - http://www.scopus.com/inward/record.url?scp=84861923188&partnerID=8YFLogxK
U2 - 10.1088/1748-0221/7/05/P05009
DO - 10.1088/1748-0221/7/05/P05009
M3 - Article
AN - SCOPUS:84861923188
VL - 7
JO - Journal of Instrumentation
JF - Journal of Instrumentation
SN - 1748-0221
IS - 5
M1 - P05009
ER -