Vaidya black hole in non-stationary de Sitter space: Hawking’s temperature
In this paper we present a class of non-stationary solutions of Einstein’s field equations describing embedded Vaidya-de Sitter black holes with a cosmological variable function Λ ( u ). The Vaidya-de Sitter black hole is interpreted as the radiating Vaidya black hole is embedded into the non-statio...
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Veröffentlicht in: | Astrophysics and space science 2014-03, Vol.350 (1), p.285-292 |
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Sprache: | eng |
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Zusammenfassung: | In this paper we present a class of non-stationary solutions of Einstein’s field equations describing embedded Vaidya-de Sitter black holes with a cosmological variable function
Λ
(
u
). The Vaidya-de Sitter black hole is interpreted as the radiating Vaidya black hole is embedded into the non-stationary de Sitter space with variable
Λ
(
u
). The energy-momentum tensor of the Vaidya-de Sitter black hole is expressed as the sum of the energy-momentum tensors of the Vaidya null fluid and that of the non-stationary de Sitter field, and satisfies the energy conservation law. We study the energy conditions (like weak, strong and dominant conditions) for the energy-momentum tensor. We find the violation of the strong energy condition due to the negative pressure and leading to a repulsive gravitational force of the matter field associated with
Λ
(
u
) in the space-time. We also find that the time-like vector field for an observer in the Vaidya-de Sitter space is expanding, accelerating, shearing and non-rotating. It is also found that the space-time geometry of non-stationary Vaidya-de Sitter solution with variable
Λ
(
u
) is Petrov type D in the classification of space-times. We also find the Vaidya-de Sitter black hole radiating with a thermal temperature proportional to the surface gravity and entropy also proportional to the area of the cosmological black hole horizon. |
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ISSN: | 0004-640X 1572-946X |
DOI: | 10.1007/s10509-013-1712-y |