Distorted vacuum black holes in the canonical ensemble
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We consider a vacuum static spacetime in a finite size cavity. On the boundary, we specify a metric and a finite constant local temperature [Formula: see text]. No spherical or any other spatial symmetry is assumed. We show that (i) inside a cavity, only a black hole or flat spacetime are possible, whereas a curved horizonless regular spacetime is excluded, (ii) in the limit when the horizon area shrinks, the Hawking temperature diverges, (iii) for the existence of a black hole, [Formula: see text] should be high enough. When [Formula: see text], a black hole phase is favorable thermodynamically. Our consideration essentially uses the coordinate system introduced by Israel in his famous proof of the uniqueness theorem.
2005 ◽
Vol 14
(12)
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pp. 2219-2225
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1995 ◽
Vol 12
(8)
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pp. 2021-2035
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1991 ◽
Vol 8
(4)
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pp. 779-785
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2015 ◽
Vol 12
(07)
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pp. 1550070
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2018 ◽
Vol 33
(33)
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pp. 1850190
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