The CLAS detector was used to obtain the first ever measuremen t of the electromagnetic decay of the Σ∗+(1385) from the reaction γp→K0Σ∗+(1385). A real photon beam with a maximum energy of 3.8 GeV was incident on a liquid-hydrogen target, resulting in the photoproduction ofthe kaon and Σ∗ hyperon. Kinematic fitting was used to separate the reaction channel from the background processes. The fitting algorithm exploited a new method to kinematically fit neutrons in the CLAS detector, leading to the partial width measurement of 250.0±56.9(stat)+34.3−41.2(sys) keV. A U-spin symmetry test using the SU(3) flavor-multiplet representation yields predictions for the Σ∗+(1385)→Σ+γ and Σ∗0(1385)→Λγ partial widths that agree with the experimental measurements.

Branching ratio of the electromagnetic decay of the Sigma(+)(1385)

CONTALBRIGO, Marco;PAPPALARDO, Luciano Libero;
2012

Abstract

The CLAS detector was used to obtain the first ever measuremen t of the electromagnetic decay of the Σ∗+(1385) from the reaction γp→K0Σ∗+(1385). A real photon beam with a maximum energy of 3.8 GeV was incident on a liquid-hydrogen target, resulting in the photoproduction ofthe kaon and Σ∗ hyperon. Kinematic fitting was used to separate the reaction channel from the background processes. The fitting algorithm exploited a new method to kinematically fit neutrons in the CLAS detector, leading to the partial width measurement of 250.0±56.9(stat)+34.3−41.2(sys) keV. A U-spin symmetry test using the SU(3) flavor-multiplet representation yields predictions for the Σ∗+(1385)→Σ+γ and Σ∗0(1385)→Λγ partial widths that agree with the experimental measurements.
2012
D., Keller; K., Hicks; K. P., Adhikari; D., Adikaram; M. J., Amaryan; M., Anghinolfi; H., Baghdasaryan; J., Ball; M., Battaglieri; I., Bedlinskiy; A. S., Biselli; C., Bookwalter; S., Boiarinov; D., Branford; W. J., Briscoe; W. K., Brooks; V. D., Burkert; D. S., Carman; A., Celentano; S., Chandavar; P. L., Cole; Contalbrigo, Marco; V., Crede; A., D'Angelo; A., Daniel; N., Dashyan; R. D., Vita; E. D., Sanctis; C., Djalali; D., Doughty; R., Dupre; A. E., Alaoui; L. E., Fassi; L., Elouadrhiri; P., Eugenio; G., Fedotov; M. Y., Gabrielyan; N., Gevorgyan; G. P., Gilfoyle; K. L., Giovanetti; W., Gohn; E., Golovatch; R. W., Gothe; L., Graham; K. A., Griffioen; M., Guidal; N., Guler; L., Guo; K., Hafidi; H., Hakobyan; M., Holtrop; Y., Ilieva; D. G., Ireland; B. S., Ishkhanov; E. L., Isupov; H. S., Jo; K., Joo; M., Khandaker; P., Khetarpal; A., Kim; W., Kim; F. J., Klein; A., Kubarovsky; V., Kubarovsky; S. V., Kuleshov; H. Y., Lu; I. J., D.; Y., Mao; N., Markov; M., Mayer; B., Mckinnon; C. A., Meyer; T., Mineeva; M., Mirazita; V., Mokeev; H., Moutarde; E., Munevar; P., Nadel Turonski; R., Nasseripour; S., Niccolai; G., Niculescu; I., Niculescu; M., Osipenko; A. I., Ostrovidov; M., Paolone; Pappalardo, Luciano Libero; R., Paremuzyan; K., Park; S., Park; E., Pasyuk; S. A., Pereira; S., Pisano; O., Pogorelko; S., Pozdniakov; S., Procureur; Y., Prok; D., Protopopescu; B. A., Raue; G., Ricco; D., Rimal; M., Ripani; B. G., Ritchie; G., Rosner; P., Rossi; F., Sabatie; M. S., Saini; C., Salgado; D., Schott; R. A., Schumacher; H., Seraydaryan; Y. G., Sharabian; E. S., Smith; G. D., Smith; D. I., Sober; D., Sokhan; S. S., Stepanyan; S., Stepanyan; P., Stoler; S., Strauch; M., Taiuti; W., Tang; C. E., Taylor; S., Tkachenko; B., Vernarsky; M. F., Vineyard; A. V., Vlassov; H., Voskanyan; E., Voutier; D. P., Watts; M. H., Wood; N., Zachariou; L., Zana; B., Zhao; Z. W., Zhao
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11392/1871826
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