2020
DOI: 10.1103/physrevd.102.045001
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Asymptotic horizon formation, spacetime stretching, and causality

Abstract: In this work we analyze asymptotically flat, spherically symmetric spacetimes in which an event horizon is present without any trapped surfaces. We identify two types of such spacetimes, each related to the asymptotic behavior (in time) of one of the two degrees of freedom of the metric. We study the causal structure of both types, showing that one almost always has a Cauchy horizon beyond which it is extendable, while the other is inextendable but has two separate future null infinity regions on either side o… Show more

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Cited by 4 publications
(2 citation statements)
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“…To see how the surface gravity diverges, first we need to define this quantity more precisely. Following the procedure from our previous work [21], we will use the generalised redshift function F(v, r), which goes on the right-hand side of the equation for outgoing null radial geodesics,…”
Section: Oppenheimer-snyder Collapsementioning
confidence: 99%
“…To see how the surface gravity diverges, first we need to define this quantity more precisely. Following the procedure from our previous work [21], we will use the generalised redshift function F(v, r), which goes on the right-hand side of the equation for outgoing null radial geodesics,…”
Section: Oppenheimer-snyder Collapsementioning
confidence: 99%
“…To see how the surface gravity diverges, first we need to define this quantity more precisely. Following the procedure from our previous work [17], we will use the generalised redshift function F (v, r), which goes on the right-hand side of the equation for outgoing null radial geodesics,…”
Section: Oppenheimer-snyder Collapsementioning
confidence: 99%