Department of Physics, Tohoku University
KEK, National Laboratory for High Energy Physics
KEK, National Laboratory for High Energy Physics
Institute of Applied Physics, University of Tsukuba
KEK, National Laboratory for High Energy Physics
Department of Physics, Tokyo Metropolitan University
Department of Physics, Hiroshima University
Wakayama Medical College
Faculty of Engineering, Tokyo University of Agriculture and Technology
Department of Physics, Hiroshima University
KEK, National Laboratory for High Energy Physics
Department of Physics, Tokyo Metropolitan University
KEK, National Laboratory for High Energy Physics
Department of Physics, Osaka University
Department of Physics, Hiroshima University
Department of Physics, Kyoto University
Department of Applied Physics, Tohoku-Gakuin University
Department of Physics, Tokyo Metropolitan University
Department of Physics, Kyoto University
School of Allied Medical Science, Kobe University
Department of Applied Physics, Tohoku-Gakuin University
Institute of Physics, University of Tsukuba
KEK, National Laboratory for High Energy Physics
Department of Physics, Osaka University
Department of Physics, Osaka University
KEK, National Laboratory for High Energy Physics
Department of Physics, Kyoto University
KEK, National Laboratory for High Energy Physics
Institute of Applied Physics, University of Tsukuba
Department of Physics, Kyoto University
Department of Physics, Kyoto University
KEK, National Laboratory for High Energy Physics
KEK, National Laboratory for High Energy Physics
Department of Physics, Tokyo Metropolitan University
Department of Physics, Kyoto University
Institute of Applied Physics, University of Tsukuba
Department of Physics, Osaka University
Department of Physics, Tohoku University
Department of Physics, Kyoto University
Institute of Physics, University of Tsukuba
Graduate School of Science and Technology, Kobe University
KEK, National Laboratory for High Energy Physics
KEK, National Laboratory for High Energy Physics
KEK, National Laboratory for High Energy Physics
Department of Physics, Hiroshima University
College of Liberal Arts, Kobe University
Department of Physics, Osaka University
Department of Physics, Tokyo Metropolitan University
Graduate School of Science and Technology, Kobe University
KEK, National Laboratory for High Energy Physics
Department of Physics, Osaka University
Institute of Applied Physics, University of Tsukuba
KEK, National Laboratory for High Energy Physics
Department of Physics, Kyoto University
Department of Applied Physics, Tohoku-Gakuin University
Institute of Applied Physics, University of Tsukuba
KEK, National Laboratory for High Energy Physics
KEK, National Laboratory for High Energy Physics
Department of Physics, Osaka University
KEK, National Laboratory for High Energy Physics
Department of Physics, Kyoto University
Institute of Applied Physics, University of Tsukuba
KEK, National Laboratory for High Energy Physics
Department of Physics, Hiroshima University
Department of Physics, Kyoto University
Department of Physics, Hiroshima University
KEK, National Laboratory for High Energy Physics
Faculty of General Education, Meiji-Gakuin University
KEK, National Laboratory for High Energy Physics
Department of Physics, Osaka University
KEK, National Laboratory for High Energy Physics
KEK, National Laboratory for High Energy Physics
Department of Physics, Tokyo Metropolitan University
KEK, National Laboratory for High Energy Physics
Department of Physics, Tokyo Metropolitan University
KEK, National Laboratory for High Energy Physics
KEK, National Laboratory for High Energy Physics
Department of Physics, Tokyo Metropolitan University
Department of Physics, Osaka University
Faculty of Engineering, Fukui University
1987 Volume 56 Issue 11 Pages 3767-3770
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The differential cross sections for e+e−→e+e− and e+e−→γγ have been measured at the highest energy of \sqrts=52 GeV in e+e− collisions.The process e+e−→e+e− is well understood within the framework of the standard model of electroweak interactions. The reaction e+e−→γγ is found to be in good agreement with QED. The 95% confidence limits obtained for the QED cut-off parameters are Λ+>61 GeV and Λ−>72 GeV for e+e−→γγ.
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Proceedings of the Physico-Mathematical Society of Japan. 3rd Series
Proceedings of the Tokyo Mathematico-Physical Society. 2nd Series
Tokyo Sugaku-Butsurigakukwai Kiji-Gaiyo
Tokyo Sugaku-Butsurigakkwai Hokoku
Tokyo Sugaku-Butsurigaku Kwai Kiji