2006
DOI: 10.1103/physrevd.74.064019
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Explicit Fermi coordinates and tidal dynamics in de Sitter and Gödel spacetimes

Abstract: Fermi coordinates are directly constructed in de Sitter and Gödel spacetimes and the corresponding exact coordinate transformations are given explicitly. The quasi-inertial Fermi coordinates are then employed to discuss the dynamics of a free test particle in these spacetimes and the results are compared to the corresponding generalized Jacobi equations that contain only the lowest-order tidal terms. The domain of validity of the generalized Jacobi equation is thus examined in these cases. Furthermore, the dif… Show more

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Cited by 74 publications
(125 citation statements)
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“…In previous work on tidal dynamics [3][4][5][6][7][8][9], the relative behavior of a congruence of geodesics has been studied. Moreover, tidal gravitational acceleration of ultrarelativistic particles has been considered in a general context but via geodesic deviation within the small-deviation approximation [4][5][6][7][8][9].…”
Section: Introductionmentioning
confidence: 99%
“…In previous work on tidal dynamics [3][4][5][6][7][8][9], the relative behavior of a congruence of geodesics has been studied. Moreover, tidal gravitational acceleration of ultrarelativistic particles has been considered in a general context but via geodesic deviation within the small-deviation approximation [4][5][6][7][8][9].…”
Section: Introductionmentioning
confidence: 99%
“…To express this trajectory in terms of the original background coordinate system, it is in general necessary to have the explicit coordinate transformation between the two systems of coordinates. This turns out to be possible only in very special situations [38,39]. However, our first-order approximation scheme makes it possible to proceed as follows.…”
Section: Appendix A: Mpd Equations In Fermi Normal Coordinatesmentioning
confidence: 99%
“…Taking the variational derivatives with respect toḡ µν from the expressions (137) and (138), and applying thermodynamic equations (18), allows us to write down the right sides of equations (134b), (134c) as follows,…”
Section: The Gravitational Field Perturbationsmentioning
confidence: 99%
“…Transformation from the preferred cosmological frame to the local chart must include the Lorentz boost and a geometric part due to the expansion and curvature of cosmological spacetime. It can take on multiple forms which originate from certain geometric and/or experimental requirements [16,18,48,54].We do not impose specific limitations on the choice of coordinates on the background manifold and keep the overall formalism of the post-Newtonian approximations, covariant. The arbitrary coordinates are denoted as x α = (x 0 , x i ) and they are related to the preferred isotropic coordinates X α = (η, X i ) by the coordinate transformation x α = x α X β .…”
mentioning
confidence: 99%
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