Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D, Particles, fields, gravitation, and cosmology · 2009 · 14 citations · 9 references
Natural SciencesPhysicsGravitationRelativityTheoretical PhysicsCurved SpacetimeEinstein Field EquationsExperimental Tests Of RelativityGeneral RelativitySpacetime GeometrySpecial RelativityCurvaturePound-rebka ExperimentSignalsSpace-time Curvature In CosmologyTorsion
We develop some ideas discussed by E. Schucking [arXiv:0803.4128] concerning the geometry of the gravitational field. First, we address the concept according to which the gravitational acceleration is a manifestation of the space-time torsion, not of the curvature tensor. It is possible to show that there are situations in which the geodesic acceleration of a particle may acquire arbitrary values, whereas the curvature tensor approaches zero. We conclude that the space-time curvature does not affect the geodesic acceleration. Then we consider the Pound-Rebka experiment, which relates the time interval $\ensuremath{\Delta}{\ensuremath{\tau}}_{1}$ of two light signals emitted at a position ${r}_{1}$, to the time interval $\ensuremath{\Delta}{\ensuremath{\tau}}_{2}$ of the signals received at a position ${r}_{2}$, in a Schwarzschild type gravitational field. The experiment is determined by four space-time events. The infinitesimal vectors formed by these events do not form a parallelogram in the $(t,r)$ plane. The failure in the closure of the parallelogram implies that the space-time has torsion. We find the explicit form of the torsion tensor that explains the nonclosure of the parallelogram.
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Sir Herman Bondi · Journal of the Franklin Institute · 1974 · 2.8K citations
R. V. Pound, G. A. Rebka · Physical Review Letters · 1960 · 802 citations · Full text
<i>Introducing Einstein's Relativity</i>
Ray d’Inverno, Alex Harvey · Physics Today · 1993 · 240 citations
Natural Sciences, Physics, Cosmology +16