+

    Photoproduction of Λ and Σ0 hyperons off protons with linearly polarized photons at Eγ=1.53.0 GeV

    S. H. Shiu1,2, H. Kohri3,1, W. C. Chang1, D. S. Ahn4, J. K. Ahn5, J. Y. Chen6, S. Daté7, H. Ejiri3, H. Fujimura8 et al. (LEPS Collaboration)

    H. Fujimura8, M. Fujiwara3,9, S. Fukui3, W. Gohn10, K. Hicks11, T. Hotta3, S. H. Hwang12, K. Imai13, T. Ishikawa14, K. Joo10, Y. Kato15, Y. Kon3, H. S. Lee16, Y. Maeda17, T. Mibe18, M. Miyabe14, K. Mizutani19, Y. Morino18, N. Muramatsu14, T. Nakano3, Y. Nakatsugawa20, M. Niiyama19, H. Noumi3, Y. Ohashi7, T. Ohta21, M. Oka3, J. D. Parker22, C. Rangacharyulu23, S. Y. Ryu3, T. Sawada24, H. Shimizu14, Y. Sugaya3, M. Sumihama25, T. Tsunemi26, M. Uchida27, M. Ungaro10, and M. Yosoi3 (LEPS Collaboration)

    • 1Institute of Physics, Academia Sinica, Taipei 11529, Taiwan
    • 2Department of Physics, National Central University, Taoyuan City 32001, Taiwan
    • 3Research Center for Nuclear Physics, Osaka University, Ibaraki, Osaka 567-0047, Japan
    • 4RIKEN Nishina Center, 2-1 Hirosawa, Wako, Saitama 351-0198, Japan
    • 5Department of Physics, Korea University, Seoul 02841, Republic of Korea
    • 6Light Source Division, National Synchrotron Radiation Research Center, Hsinchu, 30076, Taiwan
    • 7Japan Synchrotron Radiation Research Institute, Sayo, Hyogo 679-5143, Japan
    • 8Wakayama Medical College, Wakayama, 641-8509, Japan
    • 9National Institutes for Quantum and Radiological Science and Technology, Tokai, Ibaraki 319-1195, Japan
    • 10Department of Physics, University of Connecticut, Storrs, Connecticut 06269-3046, USA
    • 11Department of Physics and Astronomy, Ohio University, Athens, Ohio 45701, USA
    • 12Korea Research Institute of Standards and Science (KRISS), Daejeon 34113, Republic of Korea
    • 13Advanced Science Research Center, Japan Atomic Energy Agency, Tokai, Ibaraki 319-1195, Japan
    • 14Research Center for Electron Photon Science, Tohoku University, Sendai, Miyagi 982-0826, Japan
    • 15Kobayashi-Maskawa Institute, Nagoya University, Nagoya, Aichi 464-8602, Japan
    • 16Rare Isotope Science Project, Institute for Basic Science, Daejeon 34047, Korea
    • 17Proton Therapy Center, Fukui Prefectural Hospital, Fukui 910-8526, Japan
    • 18High Energy Accelerator Organization (KEK), Tsukuba, Ibaraki 305-0801, Japan
    • 19Department of Physics, Kyoto University, Kyoto 606-8502, Japan
    • 20Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, China
    • 21Department of Radiology, The University of Tokyo Hospital, Tokyo 113-8655, Japan
    • 22Neutron Science and Technology Center, Comprehensive Research Organization for Science and Society (CROSS), Tokai, Ibaraki 319-1106, Japan
    • 23Department of Physics and Engineering Physics, University of Saskatchewan, Saskatoon, SK S7N 5E2, Canada
    • 24Physics Department, University of Michigan, Michigan 48109-1040, USA
    • 25Department of Education, Gifu University, Gifu 501-1193, Japan
    • 26Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan
    • 27Department of Physics, Tokyo Institute of Technology, Tokyo 152-8551, Japan

    Phys. Rev. C 97, 015208 – Published 31 January, 2018

    DOI: https://doi.org/10.1103/PhysRevC.97.015208

    Abstract

    We report the measurement of the γpK+Λ and γpK+Σ0 reactions at SPring-8. The differential cross sections and photon-beam asymmetries are measured at forward K+ production angles using linearly polarized tagged-photon beams in the range of Eγ=1.53.0 GeV. With increasing photon energy, the cross sections for both γpK+Λ and γpK+Σ0 reactions decrease slowly. Distinct narrow structures in the production cross section have not been found at Eγ=1.53.0 GeV. The forward peaking in the angular distributions of cross sections, a characteristic feature of t-channel exchange, is observed for the production of Λ in the whole observed energy range. A lack of similar feature for Σ0 production reflects a less dominant role of t-channel contribution in this channel. The photon-beam asymmetries remain positive for both reactions, suggesting the dominance of K* exchange in the t channel. These asymmetries increase gradually with the photon energy, and have a maximum value of +0.6 for both reactions. Comparison with theoretical predictions based on the Regge trajectory in the t channel and the contributions of nucleon resonances indicates the major role of t-channel contributions as well as non-negligible effects of nucleon resonances in accounting for the reaction mechanism of hyperon photoproduction in this photon energy regime.

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