2018
DOI: 10.1088/1361-6382/aabd97
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Imaging a non-singular rotating black hole at the center of the Galaxy

Abstract: We show that the rotating generalization of Hayward's non-singular black hole previously studied in the literature is geodesically incomplete, and that its straightforward extension leads to a singular spacetime. We present another extension, which is devoid of any curvature singularity. The obtained metric depends on three parameters and, depending on their values, yields an event horizon or not. These two regimes, named respectively regular rotating Hayward black hole and naked rotating wormhole, are studied… Show more

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Cited by 70 publications
(61 citation statements)
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“…In this section we consider the rotating wormhole solution first described in Lamy et al (2018), which we hereafter refer to as Lamy wormhole. This solution was found by generalizing the spherically symmetric regular (i.e., singularity-free) black hole solution of Hayward (2006) to the rotating case.…”
Section: Lamy Spinning Wormholementioning
confidence: 99%
“…In this section we consider the rotating wormhole solution first described in Lamy et al (2018), which we hereafter refer to as Lamy wormhole. This solution was found by generalizing the spherically symmetric regular (i.e., singularity-free) black hole solution of Hayward (2006) to the rotating case.…”
Section: Lamy Spinning Wormholementioning
confidence: 99%
“…Generic regular NED black holes were introduced in [25,61]. Along with the static and spherically symmetric non-rotating solutions, generalizations to the rotating spacetimes were derived and studied extensively [34,59]. It is thus of crucial importance to look for clear observational signatures of the regular black holes.…”
Section: Introductionmentioning
confidence: 99%
“…Then the image of a wormhole, that is, the shape and brightness of the wormhole accretion disk, is determined by the behaviour of null geodesics of both these kinds, together with the inclination of the disk plane with respect to the line of sight of an observer. In general, an analytical computation of this image for scalar field wormholes seems to be impossible, therefore we will briefly discuss these issues qualitatively in the same standard manner as for black holes [4,7,14,17,26,27].…”
Section: Trajectories Of Null Geodesicsmentioning
confidence: 99%
“…This approach allows us to explore some unevident features of the trajectories of massive and massless test particles in such spacetimes; these features are usually hidden in qualitative models based on computer simulations. Other useful fully analytical models are based on the Kerr-like configurations, which, however, do not take account of dark matter [4,26,27]. We will consider the simplest case of a spherically symmetric, static, traversable wormhole supported by a nonlinear self-gravitating minimally coupled phantom (in another terminology, ghost) scalar field with an arbitrary self-interaction potential.…”
Section: Introductionmentioning
confidence: 99%