Geodesic motion in Bogoslovsky-Finsler Spacetimes

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Hauptverfasser: Elbistan, M., Zhang, P. -M., Dimakis, N., Gibbons, G. W., Horvathy, P. A.
Format: Preprint
Veröffentlicht: 2020
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author Elbistan, M.
Zhang, P. -M.
Dimakis, N.
Gibbons, G. W.
Horvathy, P. A.
author_facet Elbistan, M.
Zhang, P. -M.
Dimakis, N.
Gibbons, G. W.
Horvathy, P. A.
contents We study the free motion of a massive particle moving in the background of a Finslerian deformation of a plane gravitational wave in Einstein's General Relativity. The deformation is a curved version of a one-parameter family of Relativistic Finsler structures introduced by Bogoslovsky, which are invariant under a certain deformation of Cohen and Glashow's Very Special Relativity group ISIM(2). The partially broken Carroll Symmetry we derive using Baldwin-Jeffery-Rosen coordinates allows us to integrate the geodesics equations. The transverse coordinates of timelike Finsler-geodesics are identical to those of the underlying plane gravitational wave for any value of the Bogoslovsky-Finsler parameter $b$. We then replace the underlying plane gravitational wave by a homogenous pp-wave solution of the Einstein-Maxwell equations. We conclude by extending the theory to the Finsler-Friedmann-Lemaitre model.
format Preprint
id arxiv_https___arxiv_org_abs_2004_02751
institution arXiv
publishDate 2020
record_format arxiv
spellingShingle Geodesic motion in Bogoslovsky-Finsler Spacetimes
Elbistan, M.
Zhang, P. -M.
Dimakis, N.
Gibbons, G. W.
Horvathy, P. A.
General Relativity and Quantum Cosmology
High Energy Physics - Theory
Mathematical Physics
We study the free motion of a massive particle moving in the background of a Finslerian deformation of a plane gravitational wave in Einstein's General Relativity. The deformation is a curved version of a one-parameter family of Relativistic Finsler structures introduced by Bogoslovsky, which are invariant under a certain deformation of Cohen and Glashow's Very Special Relativity group ISIM(2). The partially broken Carroll Symmetry we derive using Baldwin-Jeffery-Rosen coordinates allows us to integrate the geodesics equations. The transverse coordinates of timelike Finsler-geodesics are identical to those of the underlying plane gravitational wave for any value of the Bogoslovsky-Finsler parameter $b$. We then replace the underlying plane gravitational wave by a homogenous pp-wave solution of the Einstein-Maxwell equations. We conclude by extending the theory to the Finsler-Friedmann-Lemaitre model.
title Geodesic motion in Bogoslovsky-Finsler Spacetimes
topic General Relativity and Quantum Cosmology
High Energy Physics - Theory
Mathematical Physics
url https://arxiv.org/abs/2004.02751