Late time tails of wave propagation in higher dimensional space-times
Late time tails of wave propagation in higher dimensional space-times
We study the late-time tails appearing in the propagation of massless fields (scalar, electromagnetic, and gravitational) in the vicinities of a D-dimensional Schwarzschild black hole. We find that at late times the fields always exhibit a power-law falloff, but the power law is highly sensitive to the dimensionality of the spacetime. Accordingly, for odd D>3 we find that the field behaves as t−(2l+D−2) at late times, where l is the angular index determining the angular dependence of the field. This behavior is entirely due to D being odd; it does not depend on the presence of a black hole in the spacetime. Indeed this tail is already present in the flat space Green’s function. On the other hand, for even D>4 the field decays as t−(2l+3D−8), and this time there is no contribution from the flat background. This power law is entirely due to the presence of the black hole. The D=4 case is special and exhibits, as is well known, t−(2l+3) behavior. In the extra dimensional scenario for our Universe, our results are strictly correct if the extra dimensions are infinite, but also give a good description of the late-time behavior of any field if the large extra dimensions are large enough.
Cardoso, Vitor
08c1bdef-b56a-4067-ab37-89a9ece74fb7
Yoshida, Shijun
7671361b-0f79-4404-b1f3-537b855e4f22
Dias, Oscar J.C.
f01a8d9b-9597-4c32-9226-53a6e5500a54
Lemos, Jose P.S.
4e94199c-42b9-4592-9da9-f5035913088c
15 September 2003
Cardoso, Vitor
08c1bdef-b56a-4067-ab37-89a9ece74fb7
Yoshida, Shijun
7671361b-0f79-4404-b1f3-537b855e4f22
Dias, Oscar J.C.
f01a8d9b-9597-4c32-9226-53a6e5500a54
Lemos, Jose P.S.
4e94199c-42b9-4592-9da9-f5035913088c
Cardoso, Vitor, Yoshida, Shijun, Dias, Oscar J.C. and Lemos, Jose P.S.
(2003)
Late time tails of wave propagation in higher dimensional space-times.
Phys.Rev.D, 68 (6), [061503].
(doi:10.1103/PhysRevD.68.061503).
Abstract
We study the late-time tails appearing in the propagation of massless fields (scalar, electromagnetic, and gravitational) in the vicinities of a D-dimensional Schwarzschild black hole. We find that at late times the fields always exhibit a power-law falloff, but the power law is highly sensitive to the dimensionality of the spacetime. Accordingly, for odd D>3 we find that the field behaves as t−(2l+D−2) at late times, where l is the angular index determining the angular dependence of the field. This behavior is entirely due to D being odd; it does not depend on the presence of a black hole in the spacetime. Indeed this tail is already present in the flat space Green’s function. On the other hand, for even D>4 the field decays as t−(2l+3D−8), and this time there is no contribution from the flat background. This power law is entirely due to the presence of the black hole. The D=4 case is special and exhibits, as is well known, t−(2l+3) behavior. In the extra dimensional scenario for our Universe, our results are strictly correct if the extra dimensions are infinite, but also give a good description of the late-time behavior of any field if the large extra dimensions are large enough.
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Published date: 15 September 2003
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©2003 American Physical Society
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Local EPrints ID: 468160
URI: http://eprints.soton.ac.uk/id/eprint/468160
PURE UUID: 03a56612-f3c5-4c13-ba83-5d8cecddff85
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Date deposited: 04 Aug 2022 16:37
Last modified: 17 Mar 2024 03:35
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Author:
Vitor Cardoso
Author:
Shijun Yoshida
Author:
Jose P.S. Lemos
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