Gravitation Physics
スポンサーリンク
概要
- 論文の詳細を見る
Gravitational interactions are generally investigated under the assumptions: (i) the Lorentz invariance (special relativity), (ii) (CPT) invariance, (iii) gauge invariance and (iv) the weak (gravitation) field approximation. Discussions are given for possible effects of P and T violating gravitational interactions as well as empirical upper limits on the degrees of such violations.
- 理論物理学刊行会の論文
著者
-
YAMAGUCHI Yoshio
Institute for Clinical Research, Tochigi National Hospital
-
Hiida Kichiro
Institute For Nuclear Study University Of Tokyo
-
Hiida Kichiro
Institute For Nuclear Study Tokyo University
-
Yamaguchi Yoshio
Institute For Nuclear Study University Of Tokyo
関連論文
- Trends of β-lactam antibiotic susceptibility in blood-borne methicillin-resistant Staphylococcus aureus (MRSA) and their linkage to the staphylococcal cassette chromosome mec (SCCmec) type
- Trends in the gentamicin and arbekacin susceptibility of methicillin-resistant Staphylococcus aureus and the genes encoding aminoglycoside-modifying enzymes
- 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
- Transverse Nucleon Polarization in Elastic Lepton Production by High Energy Neutrino
- Muon Capture in He^3
- Screening Effect in Relativistic QED Plasma
- 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
- Trio-Spinor Formalism and Baryon-Lepton Symmetry
- Electric Charges of Strongly Interacting Particles : Is the K^0-meson electrically neutral?
- Gauge Transformation and Gravitational Potentials
- Perturbation Calculation of Gravitational Potentials
- Chiral Symmetry in the Unified Fermion Theory. I : SU(2)×SU(2)