T. Kinoshita
Tohoku University
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Featured researches published by T. Kinoshita.
Progress of Theoretical Physics Supplement | 2007
F. Miyahara; Jirohta Kasagi; T. Nakabayashi; H. Fukasawa; R. Hashimoto; T. Ishikawa; T. Iwata; H. Kanda; T. Kinoshita; Kazushige Maeda; K. Nawa; T. Nomura; H. Shimizu; T. Shishido; K. Suzuki; Y. Tajima; Tadayuki Takahashi; H. Ueno; H. Yamazaki; H. Y. Yoshida
Differential and total cross sections of the D(γ, η)pn reaction have been measured for photon energies between 600 and 1150 MeV. The data provide the information of the γn → ηn reaction above Eγ ≥ 800 MeV. The total cross section shows a narrow resonance structure peaked at Eγ = 1020 MeV. The angular distribution coefficients together with the total cross section are compared with the calculation of the isobar model by using the impulse approximation. Although the spin and parity of the resonance cannot be determined unambiguously, a negative parity assignment gives better fit to the data.
Archive | 2008
H. Shimizu; F. Miyahara; T. Nakabayashi; H. Fukasawa; R. Hashimoto; T. Ishikawa; T. Iwata; H. Kanda; Jirohta Kasagi; T. Kinoshita; K. Maeda; K. Nawa; T. Nomura; T. Shishido; K. Suzuki; Y. Tajima; Tadayuki Takahashi; H. Ueno; H. Yamazaki; H. Y. Yoshida
A resonance-like structure has been observed in the total cross section for the γd → ηnp reaction at E γ ∼ 1.02 GeV. The experiment was conducted at Laboratory of Nuclear Science, Tohoku University, by utilizing a tagged photon beam provided with an internal radiator in a 1.2 GeV electron synchrotron. A solid deuterium target was employed as well as a solid hydrogen target to extract information on the process γn → ηn. A clear bump has been observed in the total cross section for the γn’ → ηn reactio where n’ means a neutron in Fermi motion. A simple analysis gives the position of about 1670 MeV and the width of less than 40 MeV for the bump, respectively, taking into account the Fermi motion. There is no bump structure observed, in contrast, in the γp→ ηp process at the same energy region. The U-spin conservation may naturally account for this phenomenon, if the bump is an indication of a hidden-strangeness pentaquark baryon N 5(1670) in the anti-decuplet state.
Progress of Theoretical Physics Supplement | 2007
F. Miyahara; H. Y. Yoshida; T. Nakabayashi; H. Shimizu; H. Ueno; R. Hashimoto; T. Kinoshita; T. Nomura; H. Yamazaki; K. Suzuki; Y. Tajima; H. Kanda; Kazushige Maeda; Kanabu Nawa; Tetsuya Ishikawa; H. Fukasawa; Jirohta Kasagi; Tadayuki Takahashi; T. Shishido; T. Iwata
Differential and total cross sections of the D(γ, η)pn reaction have been measured for photon energies between 600 and 1150 MeV. The data provide the information of the γn → ηn reaction above Eγ ≥ 800 MeV. The total cross section shows a narrow resonance structure peaked at Eγ = 1020 MeV. The angular distribution coefficients together with the total cross section are compared with the calculation of the isobar model by using the impulse approximation. Although the spin and parity of the resonance cannot be determined unambiguously, a negative parity assignment gives better fit to the data.
Progress of Theoretical Physics Supplement | 2007
F. Miyahara; Jirohta Kasagi; Tokuhiro Nakabayashi; H. Fukasawa; R. Hashimoto; Tetsuya Ishikawa; T. Iwata; H. Kanda; T. Kinoshita; Kunihiko Maeda; Kanabu Nawa; T. Nomura; H. Shimizu; T. Shishido; K. Suzuki; Y. Tajima; Tadayuki Takahashi; H. Ueno; H. Yamazaki; H. Y. Yoshida
Differential and total cross sections of the D(γ, η)pn reaction have been measured for photon energies between 600 and 1150 MeV. The data provide the information of the γn → ηn reaction above Eγ ≥ 800 MeV. The total cross section shows a narrow resonance structure peaked at Eγ = 1020 MeV. The angular distribution coefficients together with the total cross section are compared with the calculation of the isobar model by using the impulse approximation. Although the spin and parity of the resonance cannot be determined unambiguously, a negative parity assignment gives better fit to the data.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2005
H. Yamazaki; T. Kinoshita; K. Hirota; T. Katsuyama; T. Itoh; A. Katoh; T. Nakabayashi; O. Konno; T. Takahashi; K. Maeda; J. Kasagi
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2010
T. Ishikawa; H. Fujimura; R. Hashimoto; T. Ishida; Jirohta Kasagi; T. Kinoshita; S. Kuwasaki; Fusashi Miyahara; A. Miyamoto; K. Mochizuki; T. Nakabayashi; M. Nanao; K. Nawa; Y. Okada; K. Okamura; Y. Onodera; Y. Saito; K. Satou; M. Sengoku; H. Shimizu; K. Suzuki; S. Suzuki; Y. Tajima; T. Takahashi; H. Yamazaki; H. Yonemura; H. Y. Yoshida
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2005
H. Shimizu; F. Miyahara; H. Hariu; T. Hayakawa; T. Ishikawa; M. Itaya; T. Iwata; T. Kinoshita; M. Moriya; T. Nakabayashi; T. Sasaki; Y. Tajima; S. Takita; M. Yamamoto; H. Yamazaki; H. Y. Yoshida; Y. Yoshida
Progress of Theoretical Physics Supplement | 2007
F. Miyahara; Jirohta Kasagi; T. Nakabayashi; H. Fukasawa; R. Hashimoto; Tetsuya Ishikawa; T. Iwata; H. Kanda; T. Kinoshita; Kazushige Maeda; Kanabu Nawa; T. Nomura; H. Shimizu; T. Shishido; K. Suzuki; Y. Tajima; Tadayuki Takahashi; H. Ueno; H. Yamazaki; H. Y. Yoshida
Progress of Theoretical Physics Supplement | 2007
F. Miyahara; Jirohta Kasagi; Tokuhiro Nakabayashi; H. Fukasawa; Ronaldo Fumio Hashimoto; Tetsuya Ishikawa; Tadahisa Iwata; Hiroyuki Kanda; T. Kinoshita; Kunihiko Maeda; Kanabu Nawa; Tetsuro Nomura; Hirohiko M. Shimizu; T. Shishido; Kinuko Suzuki; Y. Tajima; Tsutomu Takahashi; H. Ueno; Hiroshi Yamazaki; H. Y. Yoshida
Archive | 2002
Hiroshi Yamazaki; T. Kinoshita; Kaoru Hirota; K. Kino; Tokuhiro Nakabayashi; Tsutomu Katsuyama; A. Katoh; T. Terasawa; Hirohiko M. Shimizu; J. Kasagi; Tsuyoshi Takahashi; Hiroyuki Kanda; Kei-ichi Maeda; Y. Tajima; H. Y. Yoshida; Takeshi Noma; Yasuhiro Aruga; A. Iijima; Y. Ito; T. Fujinoya; T. Yorita; O. Konno