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Search for Pentaquark Theta super(+) in Hadronic Reaction at J-PARC

by Joo, G G , Sako, H , Samoilov, V , Masumoto, S , Moritsu, M , Koike, T , Ajimura, S , Sato, M , Ishibashi, N , Ishimoto, S , Itahashi, K , Kim, S J , Ieiri, M , Fujioka, H , Botta, E , Ozawa, K , Saito, N , Evtoukhovitch, P , Kulikov, V V , Komatsu, Y , Matsuoka, K , Hosomi, K , Kanatsuki, S , Miwa, K , Ota, R , Bassalleck, B , Marcello, S , Noumi, H , Imai, K , Naruki, M , Matsumoto, Y , Kiuchi, R , Adachi, S , Sakaguchi, A , Aoki, K , Igarashi, Y , Niiyama, M , et. al , Bufalino, S , Bang, H , Ekawa, H , Iwasaki, R , Nozawa, Y , Nagae, T , Ichikawa, Y , Hiruma, F , Honda, R , Agnello, M , Kim, MJ , Hayakawa, S , Feliciello, A

in Autumn

2013

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Search for Pentaquark Theta super(+) in Hadronic Reaction at J-PARC

in Autumn

2013

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2013

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Journal Article

Search for Pentaquark Theta super(+) in Hadronic Reaction at J-PARC

Joo, G G,

Sako, H,

Samoilov, V,

Masumoto, S,

Moritsu, M,

Koike, T,

Ajimura, S,

Sato, M,

Ishibashi, N,

Ishimoto, S,

Itahashi, K,

Kim, S J,

Ieiri, M,

Fujioka, H,

Botta, E,

Ozawa, K,

Saito, N,

Evtoukhovitch, P,

Kulikov, V V,

Komatsu, Y,

Matsuoka, K,

Hosomi, K,

Kanatsuki, S,

Miwa, K,

Ota, R,

Bassalleck, B,

Marcello, S,

Noumi, H,

Imai, K,

Naruki, M,

Matsumoto, Y,

Kiuchi, R,

Adachi, S,

Sakaguchi, A,

Aoki, K,

Igarashi, Y,

Niiyama, M,

et. al,

Bufalino, S,

Bang, H,

Ekawa, H,

Iwasaki, R,

Nozawa, Y,

Nagae, T,

Ichikawa, Y,

Hiruma, F,

Honda, R,

Agnello, M,

Kim, MJ,

Hayakawa, S,

Feliciello, A

2013

Overview

The first experiment at the J-PARC hadron facility, the J-PARC E19 experiment, aims at searching for the Theta super(+) pentaquark in the hadronic reaction pi super(-) p arrow right K super(-) X using the missing-mass technique. Based on a superconducting magnet excited at 2.5 T, the spectrometer achieved the high mass resolution of 1.4 MeV/c super(2) for the Theta super(+) production process. The first data taking was performed in the autumn of 2010. No significant structure was observed in the missing-mass spectrum. The upper limit obtained for the differential cross section is 0.26 mu b/sr in the laboratory frame at a 90 % CL.

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