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6 results on '"Capponi, M"'

1. Pion contamination in the MICE muon beam

Author

Adams, D, Alekou, A, Apollonio, M, Asfandiyarov, R, Barber, G, Barclay, P, de Bari, A, Bayes, R, Bayliss, V, Bertoni, R, Blackmore, VJ, Blondel, A, Blot, S, Bogomilov, M, Bonesini, M, Booth, CN, Bowring, D, Boyd, S, Brashaw, TW, Bravar, U, Bross, AD, Capponi, M, Carlisle, T, Cecchet, G, Charnley, C, Chignoli, F, Cline, D, Cobb, JH, Colling, G, Collomb, N, Coney, L, Cooke, P, Courthold, M, Cremaldi, LM, DeMello, A, Dick, A, Dobbs, A, Dornan, P, Drews, M, Drielsma, F, Filthaut, F, Fitzpatrick, T, Franchini, P, Francis, V, Fry, L, Gallagher, A, Gamet, R, Gardener, R, Gourlay, S, Grant, A, Greis, JR, Griffiths, S, Hanlet, P, Hansen, OM, Hanson, GG, Hart, TL, Hartnett, T, Hayler, T, Heidt, C, Hills, M, Hodgson, P, Hunt, C, Iaciofano, A, Ishimoto, S, Kafka, G, Kaplan, DM, Karadzhov, Y, Kim, YK, Kuno, Y, Kyberd, P, Lagrange, J-B, Langlands, J, Lau, W, Leonova, M, Li, D, Lintern, A, Littlefield, M, Long, K, Luo, T, Macwaters, C, Martlew, B, Martyniak, J, Mazza, R, Middleton, S, Moretti, A, Moss, A, Muir, A, Mullacrane, I, Nebrensky, JJ, Neuffer, D, Nichols, A, Nicholson, R, Nugent, JC, Oates, A, Onel, Y, Orestano, D, Overton, E, Owens, P, Palladino, V, and Pasternak, J

Subjects
Nuclear and Plasma Physics, Particle and High Energy Physics, Synchrotrons and Accelerators, Physical Sciences, Instrumentation for particle accelerators and storage rings - low energy, Beam-line instrumentation (beam position and profile, monitors, beam-intensity monitors, bunch length monitors), physics.ins-det, hep-ex, Engineering, Nuclear & Particles Physics, Physical sciences
Abstract

The international Muon Ionization Cooling Experiment (MICE) will perform a systematic investigation of ionization cooling with muon beams of momentum between 140 and 240 MeV/c at the Rutherford Appleton Laboratory ISIS facility. The measurement of ionization cooling in MICE relies on the selection of a pure sample of muons that traverse the experiment. To make this selection, the MICE Muon Beam is designed to deliver a beam of muons with less than ∼1% contamination. To make the final muon selection, MICE employs a particle-identification (PID) system upstream and downstream of the cooling cell. The PID system includes time-of-flight hodoscopes, threshold-Cherenkov counters and calorimetry. The upper limit for the pion contamination measured in this paper is fπ < 1.4% at 90% C.L., including systematic uncertainties. Therefore, the MICE Muon Beam is able to meet the stringent pion-contamination requirements of the study of ionization cooling.

Published
2016

2. Pion contamination in the MICE muon beam

Author

Adams, D, Alekou, A, Apollonio, M, Asfandiyarov, R, Barber, G, Barclay, P, De Bari, A, Bayes, R, Bayliss, V, Bertoni, R, Blackmore, VJ, Blondel, A, Blot, S, Bogomilov, M, Bonesini, M, Booth, CN, Bowring, D, Boyd, S, Brashaw, TW, Bravar, U, Bross, AD, Capponi, M, Carlisle, T, Cecchet, G, Charnley, C, Chignoli, F, Cline, D, Cobb, JH, Colling, G, Collomb, N, Coney, L, Cooke, P, Courthold, M, Cremaldi, LM, Demello, A, Dick, A, Dobbs, A, Dornan, P, Drews, M, Drielsma, F, Filthaut, F, Fitzpatrick, T, Franchini, P, Francis, V, Fry, L, Gallagher, A, Gamet, R, Gardener, R, Gourlay, S, Grant, A, Greis, JR, Griffiths, S, Hanlet, P, Hansen, OM, Hanson, GG, Hart, TL, Hartnett, T, Hayler, T, Heidt, C, Hills, M, Hodgson, P, Hunt, C, Iaciofano, A, Ishimoto, S, Kafka, G, Kaplan, DM, Karadzhov, Y, Kim, YK, Kuno, Y, Kyberd, P, Lagrange, JB, Langlands, J, Lau, W, Leonova, M, Li, D, Lintern, A, Littlefield, M, Long, K, Luo, T, Macwaters, C, Martlew, B, Martyniak, J, Mazza, R, Middleton, S, Moretti, A, Moss, A, Muir, A, Mullacrane, I, Nebrensky, JJ, Neuffer, D, Nichols, A, Nicholson, R, Nugent, JC, Oates, A, Onel, Y, Orestano, D, Overton, E, Owens, P, Palladino, V, and Pasternak, J

Subjects
Instrumentation for particle accelerators and storage rings - low energy, Beam-line instrumentation (beam position and profile, monitors, beam-intensity monitors, bunch length monitors), physics.ins-det, hep-ex, monitors, beam-intensity monitors, bunch length monitors), Nuclear & Particles Physics, Other Physical Sciences, Physical Sciences, Engineering
Abstract

The international Muon Ionization Cooling Experiment (MICE) will perform a systematic investigation of ionization cooling with muon beams of momentum between 140 and 240 MeV/c at the Rutherford Appleton Laboratory ISIS facility. The measurement of ionization cooling in MICE relies on the selection of a pure sample of muons that traverse the experiment. To make this selection, the MICE Muon Beam is designed to deliver a beam of muons with less than ∼1% contamination. To make the final muon selection, MICE employs a particle-identification (PID) system upstream and downstream of the cooling cell. The PID system includes time-of-flight hodoscopes, threshold-Cherenkov counters and calorimetry. The upper limit for the pion contamination measured in this paper is fπ < 1.4% at 90% C.L., including systematic uncertainties. Therefore, the MICE Muon Beam is able to meet the stringent pion-contamination requirements of the study of ionization cooling.

Published
2016

3. Electron-muon ranger: Performance in the MICE muon beam

Author

Adams, D, Alekou, A, Apollonio, M, Asfandiyarov, R, Barber, G, Barclay, P, De Bari, A, Bayes, R, Bayliss, V, Bene, P, Bertoni, R, Blackmore, VJ, Blondel, A, Blot, S, Bogomilov, M, Bonesini, M, Booth, CN, Bowring, D, Boyd, S, Bradshaw, TW, Bravar, U, Bross, AD, Cadoux, F, Capponi, M, Carlisle, T, Cecchet, G, Charnley, C, Chignoli, F, Cline, D, Cobb, JH, Colling, G, Collomb, N, Coney, L, Cooke, P, Courthold, M, Cremaldi, LM, Debieux, S, Demello, A, Dick, A, Dobbs, A, Dornan, P, Drielsma, F, Filthaut, F, Fitzpatrick, T, Franchini, P, Francis, V, Fry, L, Gallagher, A, Gamet, R, Gardener, R, Gourlay, S, Grant, A, Graulich, JS, Greis, J, Griffiths, S, Hanlet, P, Hansen, OM, Hanson, GG, Hart, TL, Hartnett, T, Hayler, T, Heidt, C, Hills, M, Hodgson, P, Hunt, C, Husi, C, Iaciofano, A, Ishimoto, S, Kafka, G, Kaplan, DM, Karadzhov, Y, Kim, YK, Kuno, Y, Kyberd, P, Lagrange, JB, Langlands, J, Lau, W, Leonova, M, Li, D, Lintern, A, Littlefield, M, Long, K, Luo, T, Macwaters, C, Martlew, B, Martyniak, J, Masciocchi, F, Mazza, R, Middleton, S, Moretti, A, Moss, A, Muir, A, Mullacrane, I, Nebrensky, JJ, Neuffer, D, Nichols, A, Nicholson, R, Nicola, L, Messomo, EN, and Nugent, JC

Subjects
Particle identification methods, Particle tracking detectors, Performance of High Energy Physics Detectors, Calorimeters, physics.ins-det, hep-ex, Nuclear & Particles Physics, Other Physical Sciences, Physical Sciences, Engineering
Abstract

The Muon Ionization Cooling Experiment (MICE) will perform a detailed study of ionization cooling to evaluate the feasibility of the technique. To carry out this program, MICE requires an efficient particle-identification (PID) system to identify muons. The Electron-Muon Ranger (EMR) is a fully-active tracking-calorimeter that forms part of the PID system and tags muons that traverse the cooling channel without decaying. The detector is capable of identifying electrons with an efficiency of 98.6%, providing a purity for the MICE beam that exceeds 99.8%. The EMR also proved to be a powerful tool for the reconstruction of muon momenta in the range 100-280 MeV/c.

Published
2015

4. Electron-muon ranger: performance in the MICE muon beam

Author

Adams, D, Alekou, A, Apollonio, M, Asfandiyarov, R, Barber, G, Barclay, P, de Bari, A, Bayes, R, Bayliss, V, Bene, P, Bertoni, R, Blackmore, VJ, Blondel, A, Blot, S, Bogomilov, M, Bonesini, M, Booth, CN, Bowring, D, Boyd, S, Bradshaw, TW, Bravar, U, Bross, AD, Cadoux, F, Capponi, M, Carlisle, T, Cecchet, G, Charnley, C, Chignoli, F, Cline, D, Cobb, JH, Colling, G, Collomb, N, Coney, L, Cooke, P, Courthold, M, Cremaldi, LM, Debieux, S, DeMello, A, Dick, A, Dobbs, A, Dornan, P, Drielsma, F, Filthaut, F, Fitzpatrick, T, Franchini, P, Francis, V, Fry, L, Gallagher, A, Gamet, R, Gardener, R, Gourlay, S, Grant, A, Graulich, JS, Greis, J, Griffiths, S, Hanlet, P, Hansen, OM, Hanson, GG, Hart, TL, Hartnett, T, Hayler, T, Heidt, C, Hills, M, Hodgson, P, Hunt, C, Husi, C, Iaciofano, A, Ishimoto, S, Kafka, G, Kaplan, DM, Karadzhov, Y, Kim, YK, Kuno, Y, Kyberd, P, Lagrange, J-B, Langlands, J, Lau, W, Leonova, M, Li, D, Lintern, A, Littlefield, M, Long, K, Luo, T, Macwaters, C, Martlew, B, Martyniak, J, Masciocchi, F, Mazza, R, Middleton, S, Moretti, A, Moss, A, Muir, A, Mullacrane, I, Nebrensky, JJ, Neuffer, D, Nichols, A, Nicholson, R, Nicola, L, Messomo, E Noah, and Nugent, JC

Subjects
Nuclear and Plasma Physics, Synchrotrons and Accelerators, Physical Sciences, Particle identification methods, Particle tracking detectors, Performance of High Energy Physics Detectors, Calorimeters, physics.ins-det, hep-ex, Engineering, Nuclear & Particles Physics, Physical sciences
Abstract

The Muon Ionization Cooling Experiment (MICE) will perform a detailed study of ionization cooling to evaluate the feasibility of the technique. To carry out this program, MICE requires an efficient particle-identification (PID) system to identify muons. The Electron-Muon Ranger (EMR) is a fully-active tracking-calorimeter that forms part of the PID system and tags muons that traverse the cooling channel without decaying. The detector is capable of identifying electrons with an efficiency of 98.6%, providing a purity for the MICE beam that exceeds 99.8%. The EMR also proved to be a powerful tool for the reconstruction of muon momenta in the range 100-280 MeV/c.

Published
2015

5. Characterisation of the muon beams for the Muon Ionisation Cooling Experiment

Author

The MICE Collaboration, Adams, D, Adey, D, Alekou, A, Apollonio, M, Asfandiyarov, R, Back, J, Barber, G, Barclay, P, de Bari, A, Bayes, R, Bayliss, V, Bertoni, R, Blackmore, VJ, Blondel, A, Blot, S, Bogomilov, M, Bonesini, M, Booth, CN, Bowring, D, Boyd, S, Bradshaw, TW, Bravar, U, Bross, AD, Capponi, M, Carlisle, T, Cecchet, G, Charnley, G, Cobb, JH, Colling, D, Collomb, N, Coney, L, Cooke, P, Courthold, M, Cremaldi, LM, DeMello, A, Dick, AJ, Dobbs, A, Dornan, P, Fayer, S, Filthaut, F, Fish, A, Fitzpatrick, T, Fletcher, R, Forrest, D, Francis, V, Freemire, B, Fry, L, Gallagher, A, Gamet, R, Gourlay, S, Grant, A, Graulich, JS, Griffiths, S, Hanlet, P, Hansen, OM, Hanson, GG, Harrison, P, Hart, TL, Hartnett, T, Hayler, T, Heidt, C, Hills, M, Hodgson, P, Hunt, C, Iaciofano, A, Ishimoto, S, Kafka, G, Kaplan, DM, Karadzhov, Y, Kim, YK, Kolev, D, Kuno, Y, Kyberd, P, Lau, W, Leaver, J, Leonova, M, Li, D, Lintern, A, Littlefield, M, Long, K, Lucchini, G, Luo, T, Macwaters, C, Martlew, B, Martyniak, J, Middleton, S, Moretti, A, Moss, A, Muir, A, Mullacrane, I, Nebrensky, JJ, Neuffer, D, Nichols, A, Nicholson, R, Nugent, JC, Onel, Y, Orestano, D, Overton, E, and Owens, P

Subjects
Nuclear and Plasma Physics, Synchrotrons and Accelerators, Physical Sciences, physics.acc-ph, Atomic, Molecular, Nuclear, Particle and Plasma Physics, Quantum Physics, Nuclear & Particles Physics, Astronomical sciences, Atomic, molecular and optical physics, Particle and high energy physics
Abstract

A novel single-particle technique to measure emittance has been developed and used to characterise seventeen different muon beams for the Muon Ionisation Cooling Experiment (MICE). The muon beams, whose mean momenta vary from 171 to 281 MeV/c, have emittances of approximately 1.2-2.3 π mm-rad horizontally and 0.6-1.0 π mm-rad vertically, a horizontal dispersion of 90-190 mm and momentum spreads of about 25 MeV/c. There is reasonable agreement between the measured parameters of the beams and the results of simulations. The beams are found to meet the requirements of MICE. © 2013 The Author(s).

Published
2013

6. Characterisation of the muon beams for the Muon Ionisation Cooling Experiment

Author

Adams, D, Adey, D, Alekou, A, Apollonio, M, Asfandiyarov, R, Back, J, Barber, G, Barclay, P, de Bari, A, Bayes, R, Bayliss, V, Bertoni, R, Blackmore, VJ, Blondel, A, Blot, S, Bogomilov, M, Bonesini, M, Booth, CN, Bowring, D, Boyd, S, Bradshaw, TW, Bravar, U, Bross, AD, Capponi, M, Carlisle, T, Cecchet, G, Charnley, G, Cobb, JH, Colling, D, Collomb, N, Coney, L, Cooke, P, Courthold, M, Cremaldi, LM, DeMello, A, Dick, AJ, Dobbs, A, Dornan, P, Fayer, S, Filthaut, F, Fish, A, Fitzpatrick, T, Fletcher, R, Forrest, D, Francis, V, Freemire, B, Fry, L, Gallagher, A, Gamet, R, Gourlay, S, Grant, A, Graulich, JS, Griffiths, S, Hanlet, P, Hansen, OM, Hanson, GG, Harrison, P, Hart, TL, Hartnett, T, Hayler, T, Heidt, C, Hills, M, Hodgson, P, Hunt, C, Iaciofano, A, Ishimoto, S, Kafka, G, Kaplan, DM, Karadzhov, Y, Kim, YK, Kolev, D, Kuno, Y, Kyberd, P, Lau, W, Leaver, J, Leonova, M, Li, D, Lintern, A, Littlefield, M, Long, K, Lucchini, G, Luo, T, Macwaters, C, Martlew, B, Martyniak, J, Middleton, S, Moretti, A, Moss, A, Muir, A, Mullacrane, I, Nebrensky, JJ, Neuffer, D, Nichols, A, Nicholson, R, Nugent, JC, Onel, Y, Orestano, D, Overton, E, Owens, P, and Palladino, V

Subjects
physics.acc-ph, Nuclear & Particles Physics, Quantum Physics, Atomic, Molecular, Nuclear, Particle and Plasma Physics, Atomic, Molecular, Nuclear, Particle and Plasma Physics
Abstract

A novel single-particle technique to measure emittance has been developed and used to characterise seventeen different muon beams for the Muon Ionisation Cooling Experiment (MICE). The muon beams, whose mean momenta vary from 171 to 281 MeV/c, have emittances of approximately 1.2-2.3 π mm-rad horizontally and 0.6-1.0 π mm-rad vertically, a horizontal dispersion of 90-190 mm and momentum spreads of about 25 MeV/c. There is reasonable agreement between the measured parameters of the beams and the results of simulations. The beams are found to meet the requirements of MICE. © 2013 The Author(s).

Published
2013

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