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Featured researches published by Yoshio Sumi.


Journal of the Physical Society of Japan | 1977

Experimantal Study of Inclusive Reaction 12C(γ, π-) at 44.2°

Kota Baba; I. Endo; Hirofumi Fujii; Masakazu Fujisaki; S. Kadota; A. Murakami; Yojiro Murata; Shuichi Noguchi; Yoshio Sumi

It is found that, even at a considerably large jab angle 44.2°, momentum spectra of pions in the reaction 12 C(γ, π - ) show a clear singly-peaked structure throughout a photon energy range between 300 and 850 MeV. The peak momentum is always about 40 MeV/c less than that determined by free nucleon kinematics. The width increses almost inearly with photon energy. Differential cross section does not exhibit a marked variation with energy. These data are quite well explained by an impulse-approximation calculation.


Journal of the Physical Society of Japan | 1974

Recoil Proton Polarization and Differential Cross Section in Eta-Meson Photoproduction at 890 MeV

K. Ukai; I. Endo; Katsuhide Yoshida; Masamichi Hongoh; Ken Kikuchi; H. Kobayakawa; K. Mori; Hirobumi Senjyu; Koji Ueno; Tetsuji Yamaki; Haruo Obayashi; Yoshio Sumi

The differential cross section and recoil proton polarization for the process γ+ p →η°+ p were measured by detecting photons from η-decay and recoil protons. The differential cross sections are 0.75±0.03 and 1.04±0.07 µb/sr at the CM angles θ η * =82.3° and 108.3°, respectively, at the incident photon energy k =890 MeV, † and 0.20±0.05 µb/sr at θ η * =83.1° and k =1050 MeV. Thus the differential cross sections at k =890 MeV seem to show a backward peaking. The value of recoil proton polarization is -0.15±0.30 at θ η * =82.3°, whereas it is 0.27±0.25 at θ η * =108.3°, both at k =890 MeV, thus suggesting a sign change around θ η * =90°. In addition to the S 11 (1535), a comparably large contribution of the D 13 (1520) is needed to explain the experimental results.


Lawrence Berkeley National Laboratory | 1972

N overbar N and N overbar D Interactions -- A compilation

James E. Enstrom; T. Ferbel; Paul Francis Slattery; Barry L. Werner; Zaven G.T. Guiragossian; Yoshio Sumi; Toshihiro Yoshida

Author(s): Enstrom, James E.; Ferbel, Thomas; Slattery, Paul F.; Werner, Barry L.; Guiragossian, Zaven G.T.; Sumi, Yoshio; Yoshida, Toshihiro


Physics Letters B | 1968

Radiative pion capture in 16O

Masaaki Kawaguchi; Hisao Ohtsubo; Yoshio Sumi

Abstract The absolute values of the radiative capture rate in 16 O are predicted to be of order of 10 17 sec −1 by the shell model calculation. The observed peak of the gamma ray spectra is interpreted as the giant resonance similar to that of the photo absorption.


Progress of Theoretical Physics | 1965

Nonmesic Decay of Light Hypernuclei : Structure of the Weak Interaction Λ+N→N+N

Takanori Tamiya; Masaaki Kawaguchi; Yoshio Sumi


Progress of Theoretical Physics Supplement | 1968

Radiative Pion Capture in Complex Nuclei

Masaaki Kawaguchi; Hisao Ohtsubo; Yoshio Sumi


Progress of Theoretical Physics | 1964

Feasible Complete Experiments of Pion Photoproduction

Masaaki Kawaguchi; Hiroo Shimoida; Yoshio Sumi; Tamotsu Ueda


Progress of Theoretical Physics | 1969

Effect of Pion-Nucleon Final State Interaction in Backward Pion Photoproduction from Deuterium in 1 GeV Region

Yoshio Sumi


Progress of Theoretical Physics | 1967

One-Particle-Exchange Model in Pion Photoproduction. I*)

Hiroo Shimoida; Yoshio Sumi; Hiroyuki Yokomi


Progress of Theoretical Physics Supplement | 2013

Nucleon- and Antinucleon-Nucleon Elastic and Charge Exchange Processes

Yoshio Sumi; Toshihiro Yoshida

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I. Endo

Hiroshima University

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