COMET Phase-I technical design report

Abstract The Technical Design for the COMET Phase-I experiment is presented in this paper. COMET is an experiment at J-PARC, Japan, which will search for neutrinoless conversion of muons into electrons in the field of an aluminum nucleus ($\mu$–$e$ conversion, $\mu^{-}N \rightarrow e^{-}N$); a lepto...

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Veröffentlicht in:PTEP 2020-03, Vol.2020 (3), p.1
Hauptverfasser: Abramishvili, R, Adamov, G, Allin, A, Angélique, J C, Anishchik, V, Aznabayev, D, Ban, G, Ban, Y, Bondar, A E, Chau, T T, Chen, S J, da Silva, W, Densham, C, Devidze, G, Drutskoy, A, Duginov, V, Eguchi, Y, Epshteyn, L B, Finger Jr, M, Finger, M, Fukao, Y, Gabriel, J L, Grigoriev, D N, Hai, V H, Hamada, E, Hashim, I H, Hayashi, O, Hayashi, T, Hiasa, T, Ibrahim, Z A, Igarashi, Y, Ishibashi, K, Jansen, A, Jonsson, P, Kachelhoffer, T, Kawagoe, K, Kawashima, R, Kazak, N, Kazanin, V F, Khvedelidze, A, Koike, M, Kozyrev, A N, Kravchenko, M, Kumsiashvili, G, Kuno, Y, Kurup, A, Lagrange, B, Lee, M J, Li, W G, Loan, T, Lomidze, D, Lomidze, I, Loveridge, P, Makida, Y, Markin, O, Melkadze, A, Melnik, A, Miyazaki, Y, Mohamad Idris, F, Moiseenko, A, Nakai, Y, Nakatsugawa, Y, Nakazawa, Y, Nash, J, Nioradze, M, Nishiguchi, H, Numao, T, Ogitsu, T, Oishi, K, Okamura, T, Omori, C, Ota, T, Pasternak, J, Rusinov, V, Sabirov, B, Sato, A, Sato, J, Takayanagi, T, Tanaka, M, Tao, C V, Tevzadze, Y, Tolmachev, S S, Tomizawa, M, Toriashvili, T, Trekov, I, Tsamalaidze, Z, Tsverava, N, Velicheva, E, Volkov, A, Vrba, V, Abdullah, W A T Wan, Warin-Charpentier, P, Wong, M L, Xing, T Y, Yamaguchi, H, Yamanaka, M, Yoshioka, T, Zhang, J, Zhang, Y, Zuber, K
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Sprache:eng
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Zusammenfassung:Abstract The Technical Design for the COMET Phase-I experiment is presented in this paper. COMET is an experiment at J-PARC, Japan, which will search for neutrinoless conversion of muons into electrons in the field of an aluminum nucleus ($\mu$–$e$ conversion, $\mu^{-}N \rightarrow e^{-}N$); a lepton flavor-violating process. The experimental sensitivity goal for this process in the Phase-I experiment is $3.1\times10^{-15}$, or 90% upper limit of a branching ratio of $7\times 10^{-15}$, which is a factor of 100 improvement over the existing limit. The expected number of background events is 0.032. To achieve the target sensitivity and background level, the 3.2 kW 8 GeV proton beam from J-PARC will be used. Two types of detectors, CyDet and StrECAL, will be used for detecting the $\mu$–$e$ conversion events, and for measuring the beam-related background events in view of the Phase-II experiment, respectively. Results from simulation on signal and background estimations are also described.
ISSN:2050-3911
2050-3911
DOI:10.1093/ptep/ptz125