Massless Lorentz Gauge Field Consistent with Einstein's Gravitation Theory : The Case α+2a/3=β-2a/3=γ+3a/2=0 : Astrophysics and Relativity

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概要

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• We study the possible existence of the massless Lorentz gauge field in the linear approximation under the conditions α+2a/3=β-2a/3=γ+3a/2=0. It is found that there are two massless modes of the Lorentz gauge field propagating with positive energy in vacuum. These two massless modes have helicity-parity 1^+ and 1^-, respectively, and cannot coexist. The massless mode with helicity-parity 1^+ is the most interesting, because the axial-vector component of the Lorentz gauge field interacts with Dirac fields directly.

• 理論物理学刊行会の論文
• 1985-04-25

著者

• Nakano T

  Department Of Physics Kyushu University:(present Address)sasaguri Town Office

• Tamura Yoshinobu

  Theory And Computer Simulation Center National Institute For Fusion Science

• FUKUMA Kazumi

  Department of Physics, Osaka City University

• MIYAMOTO Shikao

  Nara Technical College

• NAKANO Tadao

  Department of Physics, Osaka City University

• OHTANI Teruya

  Kansai University of foreign Studies

• TAMURA Yoshinobu

  Department of Physics, Osaka City University

• TAMURA Yoshinobu

  Taisho High School

• Nakano Tadao

  Department Of Physics Osaka City University

• Fukuma K

  Takuma National Coll. Technol. Kagawa Jpn

• Fukuma Kazumi

  Department Of Control Engineering Takuma National College Of Technology

• Ohtani T

  Kansai Univ. Foreign Studies Hirakata Jpn

• Tamura Yoshinobu

  Department Of Electronic Engineering Graduate School Of Engineering Osaka University

• FUKUMA Kazumi

  Department of Control Engineering, Takuma National College of Technology

• FUKUMA Kazumi

  Mukogawa Women's University

• TAMURA Yuichi

  Theory and Computer Simulation Center, National Institute for Fusion Science

• NAKANO Takuya

  Department of Physics, Kyushu University:(Present Address)Sasaguri Town Office

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