"Gauge" in General Relativity: Second-order general relativistic gauge-invariant perturbation theory

Simple item page
dc.creatorNakamura, Kouji
dc.date2007-11-07
dc.date.accessioned2026-07-07T08:41:17Z
dc.date.available2026-07-07T08:41:17Z
dc.descriptionAs in the case of the other gauge field theories, there is so called ``gauge'' also in general relativity. This ``gauge'' is unphysical degree of freedom. There are two kinds of ``gauges'' in general relativity. These are called the first- and the second-kind of gauges, respectively. The gauge of the first kind is just coordinate system on a single manifold. On the other hand, the gauge of the second kind arises in the general relativistic perturbations. Through the precise distinction of these two concepts of ``gauges'', we develop second-order gauge-invariant general relativistic perturbation theory.
dc.description4 pages, lt7-proc.cls, Prepared for the proceeding of the 7th internaltional conference on "Lie Theory and Its Application in Physics" 18-24 June 2007, Varna, Bulgaria
dc.identifierhttps://arxiv.org/abs/0711.0996
dc.identifierhttp://arxiv.org/abs/0711.0996
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/141632
dc.subjectGeneral Relativity and Quantum Cosmology
dc.subjectAstrophysics
dc.subjectHigh Energy Physics - Theory
dc.subjectMathematical Physics
dc.title"Gauge" in General Relativity: Second-order general relativistic gauge-invariant perturbation theory
dc.typetext

Files

Collections

arXiv