We searched for the Φ−−(1860) pentaquark in the photoproduction process off the deuteron in the Ξ−π−-decay channel using CLAS. The invariant-mass spectrum of the Ξ−π− system does not indicate any statistically significant enhancement near the reported mass M=1.860 GeV. The statistical analysis of the sideband-subtracted mass spectrum yields a 90%-confidence-level upper limit of 0.7 nb for the photoproduction cross section of Φ−−(1860) with a consecutive decay into Ξ−π− in the photon-energy range 4.5 GeV<Eγ<5.5 GeV.

Egiyan, H., Langheinrich, J., Gothe, R., Graham, L., Holtrop, M., Lu, H., et al. (2012). Upper limits for the photoproduction cross section for the phi(--)(1860) pentaquark state off the deuteron. PHYSICAL REVIEW. C, NUCLEAR PHYSICS, 85(14), 015205-1-015205-9 [10.1103/PhysRevC.85.015205].

Upper limits for the photoproduction cross section for the phi(--)(1860) pentaquark state off the deuteron

D'ANGELO, ANNALISA;
2012-01-30

Abstract

We searched for the Φ−−(1860) pentaquark in the photoproduction process off the deuteron in the Ξ−π−-decay channel using CLAS. The invariant-mass spectrum of the Ξ−π− system does not indicate any statistically significant enhancement near the reported mass M=1.860 GeV. The statistical analysis of the sideband-subtracted mass spectrum yields a 90%-confidence-level upper limit of 0.7 nb for the photoproduction cross section of Φ−−(1860) with a consecutive decay into Ξ−π− in the photon-energy range 4.5 GeV
30-gen-2012
Pubblicato
Rilevanza internazionale
Articolo
Esperti anonimi
Settore FIS/04 - FISICA NUCLEARE E SUBNUCLEARE
English
Con Impact Factor ISI
DEEP-INELASTIC SCATTERING; XI-PI; SEARCH; CLAS; DETECTOR; HERA; BARYONS; DECAYS; SYSTEM; LEP
Clas collaboration
http://prc.aps.org/abstract/PRC/v85/i1/e015205
Egiyan, H., Langheinrich, J., Gothe, R., Graham, L., Holtrop, M., Lu, H., et al. (2012). Upper limits for the photoproduction cross section for the phi(--)(1860) pentaquark state off the deuteron. PHYSICAL REVIEW. C, NUCLEAR PHYSICS, 85(14), 015205-1-015205-9 [10.1103/PhysRevC.85.015205].
Egiyan, H; Langheinrich, J; Gothe, R; Graham, L; Holtrop, M; Lu, H; Mattione, P; Mutchler, G; Park, K; Smith, E; Stepanyan, S; Zhao, Z; Adhikari, K; Aghasyan, M; Anghinolfi, M; Baghdasaryan, H; Ball, J; Baltzell, N; Battaglieri, M; Bedlinskiy, I; Bennett, R; Biselli, A; Bookwalter, C; Branford, D; Briscoe, W; Brooks, W; Burkert, V; Carman, D; Celentano, A; Chandavar, S; Contalbrigo, M; D'Angelo, A; Daniel, A; Dashyan, N; De Vita, R; De Sanctis, E; Deur, A; Dey, B; Dickson, R; Djalali, C; Doughty, D; Dupre, R; El Alaoui, A; El Fassi, L; Eugenio, P; Fedotov, G; Fegan, S; Fradi, A; Gabrielyan, M; Gevorgyan, N; Gilfoyle, G; Giovanetti, K; Girod, F; Goetz, J; Gohn, W; Golovatch, E; Griffioen, K; Guidal, M; Guler, N; Guo, L; Gyurjyan, V; Hafidi, K; Hakobyan, H; Hanretty, C; Heddle, D; Hicks, K; Ilieva, Y; Ireland, D; Ishkhanov, B; Jo, H; Joo, K; Khetarpal, P; Kim, A; Kim, W; Klein, A; Klein, F; Kubarovsky, V; Kuleshov, S; Livingston, K; Macgregor, I; Mao, Y; Mayer, M; Mckinnon, B; Mokeev, V; Munevar, E; Nadel Turonski, P; Ni, A; Niculescu, G; Ostrovidov, A; Paolone, M; Pappalardo, L; Paremuzyan, R; Park, S; Pasyuk, E; Pereira, S; Phelps, E; Pogorelko, O; Pozdniakov, S; Price, J; Procureur, S; Protopopescu, D; Raue, B; Ricco, G; Rimal, D; Ripani, M; Ritchie, B; Rosner, G; Rossi, P; Sabatie, F; Saini, M; Salgado, C; Schott, D; Schumacher, R; Seder, E; Seraydaryan, H; Sharabian, Y; Smith, G; Sober, D; Stepanyan, S; Strauch, S; Taiuti, M; Tang, W; Taylor, C; Tedeschi, D; Ungaro, M; Voutier, E; Watts, D; Weinstein, L; Weygand, D; Wood, M; Zachariou, N; Zana, L; Zhao, B
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/2108/69373
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