Sigma p scattering experiment at J-PARC - results of commissioning run -

K. Miwa,J. K. Ahn,Y. Akazawa, T. Aramaki, S. Ashikaga,S. Callier,N. Chiga,S. W. Choi, H. Ekawa,P. Evtoukhovitch, N. Fujioka,M. Fujita, S. Hasegawa, S. Hayakawa,R. Honda, S. Hoshino,K. Hosomi,M. Ichikawa,Y. Ichikawa,M. Ieiri,M. Ikeda,K. Imai, Y. Ishikawa,S. Ishimoto, W. S. Jung, H. Kanauchi, H. Kanda, B. M. Kang, H. Kawai,S. H. Kim,K. Kobayashi,T. Koike,K. Matsuda, Y. Matsumoto,R. Nagatomi, Y. Nakada,M. Nakagawa,I. Nakamura, T. Nanamura,M. Naruki,S. Ozawa,L. Raux,A. Sakaguchi,H. Sako,S. Sato,T. Shiozaki,K. Shirotori,K. Suzuki,S. Suzuki,M. Tabata, C. d. L. Taille, H. Takahashi, T. Takahashi, T. N. Takahashi,H. Tamura,Z. Tsamalaidze, H. Umetsu, M. Ukai, T. O. Yamamoto,K. Yoshimura

AIP Conference Proceedings(2019)

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摘要
The Sigma p scattering experiment has just been started at J-PARC this year (2018). We made "Sigma beam factory" a reality where a beam with an intensity of more than 5x10(5) Sigma(-) beam per day could be produced by using 20 M/spill pi(-) beam. The CATCH system, which is a dedicated system to detect recoil proton from the Sigma p scattering, operated stably under the high counting rate, and its successful operation was confirmed by identifying the pp scattering events in J-PARC. In the June beam time, the production run of the Sigma(-)p scattering was carried out for 2 days, which was just 10% of the requested beam time. The remaining beam time of the Sigma(-)p channel and the Sigma(+)p channel will take place in the spring of 2019.
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