2019
DOI: 10.1088/1475-7516/2019/02/042
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Black-bounce to traversable wormhole

Abstract: So-called "regular black holes" are a topic currently of considerable interest in the general relativity and astrophysics communities. Herein we investigate a particularly interesting regular black hole spacetime described by the line elementThis spacetime neatly interpolates between the standard Schwarzschild black hole and the Morris-Thorne traversable wormhole; at intermediate stages passing through a black-bounce (into a future incarnation of the universe), an extremal null-bounce (into a future incarnatio… Show more

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Cited by 261 publications
(327 citation statements)
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References 98 publications
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“…Let us mention that this kind of geometric structure has been described in situations in which it leads to a bounce into another universe (see [26,27] and [28,29]). However, the spacetimes discussed in these papers are not globally hyperbolic, but display partial Cauchy surfaces [8] with topology R × S 2 .…”
Section: Arxiv:190803261v1 [Gr-qc] 8 Aug 2019mentioning
confidence: 99%
“…Let us mention that this kind of geometric structure has been described in situations in which it leads to a bounce into another universe (see [26,27] and [28,29]). However, the spacetimes discussed in these papers are not globally hyperbolic, but display partial Cauchy surfaces [8] with topology R × S 2 .…”
Section: Arxiv:190803261v1 [Gr-qc] 8 Aug 2019mentioning
confidence: 99%
“…As for the static case analyzed in reference [14], we can define a (radial) "coordinate speed of light":…”
Section: -4 -mentioning
confidence: 99%
“…The existence of a future/past event horizon depends on the presence or absence of an apparent horizon in the limit t → ±∞, that is, event horizon existence depends on whether the limit 2m(±∞)/a exceeds, equals, or is less than unity. We already know from the static case [14], that there is a throat/bounce hypersurface at r = 0. At this hypersurface the induced 3-metric is…”
Section: -4 -mentioning
confidence: 99%
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“…Let us stress that we refer to global hyperbolicity in the "strict" sense of existence of a Cauchy hypersurface which is intersected by every inextensible causal curve exactly once. The weaker condition of partial global hyperbolicity[26], in which there is a partial Cauchy hypersurface which is intersected by every inextensible, causal curve at most once, has also been used in explorations of black hole spacetimes[40,41] 4. Even though this result is certainly not new, there is no proof of this proposition in the literature that we are aware of; we have included a proof for completeness.…”
mentioning
confidence: 99%