Gauge Transformation and Gravitational Potentials
スポンサーリンク
概要
- 論文の詳細を見る
It is believed in particle physics that the velocity-dependent part of potential is, in general, ambiguous as far as it is derived from S-matrix. We consider the most general form of the graviton. propagator under an arbitrary q-number gauge transformation for the graviton field. The propagator dep,ends on twelve arbitr ary functions of k^2, k being the space part of the momentum of the graviton. The arbitrariness of the gauge functions can be used to remove the ambiguity of one-giaviton exchange potential up to the order of (G/r) (υ/c)^4, G being the gravitational constant. The potential thus obtained depends only on one gauge parameter, say x. The perihelionmotion of two-body system is gauge independent, although the potentials in the order of (G/r) (υ/c)^2 and G^2/r^2 depend on the gauge parameter x. The potentials are derived from those in a fixed gauge parameter x by a coordinate transformation.
- 理論物理学刊行会の論文
- 1972-05-25
著者
-
Okamura Hiroshi
Institute For Nuclear Study University Of Tokyo
-
Okamura Hiroshi
Institute For Nuclear Study And Department Of Physics University Of Tokyo
-
Hiida Kichiro
Institute For Nuclear Study Tokyo University
関連論文
- A Regge Pole Model for Charged Pion Photoproduction
- CP Violation and PT Invariance
- Physically Acceptable Solution of Einstein's Equation for Many-Body System
- Substitution Law and Identity for Long-Range Potentials
- General Theory of Chiral Transformations
- Gravitation Physics
- Einstein's Theory of Relativity and Mach's Principle
- Coordinate Condition and Higher Order Gravitational Potential in Canonical Formalism
- A Theory of Anomalous Gravitational Interaction. I : Case of the Bose Particle
- Quantum Theory of Gravity and the Perihelion Motion of the Mercury
- Gauge Transformation and Gravitational Potentials
- Perturbation Calculation of Gravitational Potentials
- Chiral Symmetry in the Unified Fermion Theory. I : SU(2)×SU(2)