Pith. sign in

(36) and (39)] for which the a(t)r→ 0 limit corresponds toR→∞ , whileR = 0 cor- responds to a(t)r = (−m±|q|)/2, where the isotropic coordinater is allowed to assume negative values

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gr-qc 1

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2019 1

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CONDITIONAL 1

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Charged cosmological black holes: a thorough study of a family of solutions

gr-qc · 2019-08-14 · conditional · novelty 6.0

The Shah-Vaidya charged cosmological black hole metric is shown to be an exact solution of Einstein-Maxwell equations with a cuscuton field, and its causal structure is classified into four parameter regions with different horizon counts and naked singularities.

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  • Charged cosmological black holes: a thorough study of a family of solutions gr-qc · 2019-08-14 · conditional · none · ref 5

    The Shah-Vaidya charged cosmological black hole metric is shown to be an exact solution of Einstein-Maxwell equations with a cuscuton field, and its causal structure is classified into four parameter regions with different horizon counts and naked singularities.