TY - JOUR
T1 - “K−pp”, a K-Meson nuclear bound state, observed in 3He(K−, Λp)n Reactions
AU - J-PARC E15 Collaboration
AU - Ajimura, S.
AU - Asano, H.
AU - Beer, G.
AU - Berucci, C.
AU - Bhang, H.
AU - Bragadireanu, M.
AU - Buehler, P.
AU - Busso, L.
AU - Cargnelli, M.
AU - Choi, S.
AU - Curceanu, C.
AU - Enomoto, S.
AU - Fujioka, H.
AU - Fujiwara, Y.
AU - Fukuda, T.
AU - Guaraldo, C.
AU - Hashimoto, T.
AU - Hayano, R. S.
AU - Hiraiwa, T.
AU - Iio, M.
AU - Iliescu, M.
AU - Inoue, K.
AU - Ishiguro, Y.
AU - Ishikawa, T.
AU - Ishimoto, S.
AU - Itahashi, K.
AU - Iwasaki, M.
AU - Kanno, K.
AU - Kato, K.
AU - Kato, Y.
AU - Kawasaki, S.
AU - Kienle, P.
AU - Kou, H.
AU - Ma, Y.
AU - Marton, J.
AU - Matsuda, Y.
AU - Mizoi, Y.
AU - Morra, O.
AU - Nagae, T.
AU - Noumi, H.
AU - Ohnishi, H.
AU - Okada, S.
AU - Outa, H.
AU - Piscicchia, K.
AU - Sada, Y.
AU - Sakaguchi, A.
AU - Sakuma, F.
AU - Sato, M.
AU - Scordo, A.
AU - Tsukada, K.
N1 - Publisher Copyright:
Copyright © 2018, The Authors. All rights reserved.
Copyright:
Copyright 2020 Elsevier B.V., All rights reserved.
PY - 2018/5/30
Y1 - 2018/5/30
N2 - We observed a distinct peak in the Λp invariant mass spectrum of 3He(K−, Λp)n, well below the mass threshold of mK + 2mp. By selecting a relatively large momentum-transfer region q = 350 ∼ 650 MeV/c, one can kinematically separate the peak from the quasi-free process, KN → KN followed by the non-resonant absorption by the two spectator-nucleons KNN → ΛN. We found that the simplest fit to the observed peak gives us a Breit-Wigner pole position at BKpp = 47 ± 3 (stat.) −+36 (sys.) MeV having a width ΓKpp = 115 ± 7 (stat.) −+1020 (sys.) MeV, and the S-wave Gaussian reaction form-factor parameter QKpp = 381 ± 14 (stat.) −+570 (sys.) MeV/c, as a new form of the nuclear bound system with strangeness - “K−pp”.
AB - We observed a distinct peak in the Λp invariant mass spectrum of 3He(K−, Λp)n, well below the mass threshold of mK + 2mp. By selecting a relatively large momentum-transfer region q = 350 ∼ 650 MeV/c, one can kinematically separate the peak from the quasi-free process, KN → KN followed by the non-resonant absorption by the two spectator-nucleons KNN → ΛN. We found that the simplest fit to the observed peak gives us a Breit-Wigner pole position at BKpp = 47 ± 3 (stat.) −+36 (sys.) MeV having a width ΓKpp = 115 ± 7 (stat.) −+1020 (sys.) MeV, and the S-wave Gaussian reaction form-factor parameter QKpp = 381 ± 14 (stat.) −+570 (sys.) MeV/c, as a new form of the nuclear bound system with strangeness - “K−pp”.
KW - Kaon
KW - Mesonic nuclear bound state
KW - Strangeness
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M3 - Article
AN - SCOPUS:85094437343
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