Implementation of Dipole Type Bosonic BRST Symmetry in QED(Reconstruction of Gaugeon Theory of QED)

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概要

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• It is shown in QED that we can incorporate dipole type bosonic BRST symmetry with gauge function (∧) satisfying □^2(∧)=0 in quite the same way as bosonic BRST symmetry is implemented. Lagrangian so defined turns out to be that of Yokoyama's gaugeon formalism. However difference in formulating the theory yields remarkable differences in its properties. Gaugeon and its conjugate fields come to transform differently in order for the gauge transformations to be residual ones with infinitesimal generator. We need not classify the gaugeon theory into types I and II because constituent operators of genuine QED transform such that values of the gauge parameter of Nakanishi-Lautrup formalism are freely altered. It follows that equivalence evidently holds among the one parameter covariant gauges and hence the difficulty inherent in Nakanishi-Lautrup formalism is resolved.

• 理論物理学刊行会の論文
• 1995-01-25

著者

• Ozaki K

  Faculty Of General Education Osaka Institute Of Technology

• Tanaka Atushi

  Department Of Physics Tokyo Metropolitan University

• NAKAWAKI Yuji

  Division of Physics and Mathematics, Faculty of Engineering Setsunan University

• TANAKA Azuma

  Junior college of Osaka Institute of Technology

• OZAKI Kazuhiko

  Faculty of General Education, Osaka Institute of Technology

• Nakawaki Y

  Setsunan Univ. Osaka Jpn

• Nakawaki Yuji

  Division Of Mathematics And Physics Department Of Engineering Setsunan University

• TANAKA Akiko

  Department of Physics, Kyoto Sangyo University

• OZAKI Kazuhiro

  Department of Physics, Faculty of General Education, Osaka Institute of Technology

• OZAKI Kazuhiko

  Department of Physics, Faculty of General Education The Osaka Institute of Technology

• Tanaka Azuma

  Research Center for Nuclear Physics (RCNP), Osaka University

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