Late time decay of scalar, electromagnetic, and gravitational perturbations outside rotating black holes
Late time decay of scalar, electromagnetic, and gravitational perturbations outside rotating black holes
We study analytically, via the Newman-Penrose formalism, the late time decay of scalar, electromagnetic, and gravitational perturbations outside a realistic rotating (Kerr) black hole. We find a power-law decay at timelike infinity, as well as at null infinity and along the event horizon (EH). For generic initial data we derive the power-law indices for all radiating modes of the various fields. We also give an exact analytic expression (accurate to leading order in 1/t) for the r dependence of the late time tail at any r. Some of our main conclusions are the following. (i) For generic initial data, the late time behavior of the fields is dominated by the mode l=|s| (with s being the spin parameter), which dies off at fixed r as t-2|s|-3 — as in the Schwarzschild background. (ii) However, other modes admit decay rates slower than in the Schwarzschild case. (iii) For s>0 fields, non-axially symmetric modes dominate the late time behavior along the EH. These modes oscillate along the null generators of the EH.
27pp
Barack, Leor
f08e66d4-c2f7-4f2f-91b8-f2c4230d0298
January 2000
Barack, Leor
f08e66d4-c2f7-4f2f-91b8-f2c4230d0298
Barack, Leor
(2000)
Late time decay of scalar, electromagnetic, and gravitational perturbations outside rotating black holes.
Physical Review D, 61 (24026), .
(doi:10.1103/PhysRevD.61.024026).
Abstract
We study analytically, via the Newman-Penrose formalism, the late time decay of scalar, electromagnetic, and gravitational perturbations outside a realistic rotating (Kerr) black hole. We find a power-law decay at timelike infinity, as well as at null infinity and along the event horizon (EH). For generic initial data we derive the power-law indices for all radiating modes of the various fields. We also give an exact analytic expression (accurate to leading order in 1/t) for the r dependence of the late time tail at any r. Some of our main conclusions are the following. (i) For generic initial data, the late time behavior of the fields is dominated by the mode l=|s| (with s being the spin parameter), which dies off at fixed r as t-2|s|-3 — as in the Schwarzschild background. (ii) However, other modes admit decay rates slower than in the Schwarzschild case. (iii) For s>0 fields, non-axially symmetric modes dominate the late time behavior along the EH. These modes oscillate along the null generators of the EH.
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Published date: January 2000
Identifiers
Local EPrints ID: 48006
URI: http://eprints.soton.ac.uk/id/eprint/48006
ISSN: 1550-7998
PURE UUID: 847285e3-36c4-4157-a6c6-c71548867826
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Date deposited: 20 Aug 2007
Last modified: 16 Mar 2024 03:41
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