Abstract
Black holes encountered in general relativity are characterized by spacetime singularities hidden within an event horizon. These singularities provide a key motivation to go beyond general relativity and look for regular black holes where the spacetime curvature remains bounded everywhere. A prominent mechanism achieving this replaces the singularity by a regular patch of de Sitter space. The resulting regular geometries exhibit two horizons: the outer event horizon is supplemented by an inner Cauchy horizon. The latter could render the geometry unstable against perturbations through the so-called mass-inflation effect, i.e., an exponential growth of the mass function. This chapter reviews the mass-inflation effect for spherically symmetric black hole spacetimes contrasting the dynamics of the mass function for Reissner–Nordstöm and regular black holes. We also cover recent developments related to the late-time attractors induced by Hawking radiation which exorcise the exponential growth of the spacetime curvature encountered in the standard mass-inflation scenario. In order to make the exposition self-contained, we also briefly discuss basic properties of regular black holes including their thermodynamics.
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Notes
- 1.
- 2.
For more details on the infinitely thin-shell formalism, see [57].
- 3.
This makes the crucial assumption that the Cauchy horizon actually exists. While there is good evidence for forming such a horizon for the black holes encountered in general relativity, the question whether such a horizon actually forms in the collapse to a regular black hole is a largely open question, see [63, 64] for some recent work in this direction. For a first self-consistent dynamical calculation of mass-inflation without assuming the existence of a Cauchy horizon we refer to [65].
- 4.
According to Tipler, a null singularity is called “strong” if there exists at least one component of the Riemann tensor (in a parallelly propagated frame) which does not converge when integrated with respect to the affine parameter \(\tau \) twice. The physical meaning of this requirement is that the tidal distortion is not finite as an observer crosses the singularity.
- 5.
This conclusion has been challenged in [69, 70] (also see [60] for an earlier analysis based on the DTR-relations), claiming that the onset of the attractor behavior is preceded by a “fatal” phase of exponential growth. This conclusion is flawed for three reasons though. Firstly, it builds on an analysis of the system at “early times” outside the region of validity of the underlying assumptions: Price’s law holds at asymptotically late times only where the optical geometric limit is valid and one is allowed to neglect the “finite size” effects of the inner potential barrier. In a realistic collapse the early-time dynamics is significantly more complicated because of the presence of the flux from the collapsing star. Secondly, closing eyes to this difficulty and extrapolating the model to early times, Fig. 10.7 establishes that the analysis of [69, 70] is incomplete. There are initial conditions which actually reach the salient late-time attractor also from early times. Determining the precise initial data requires the analysis of the full dynamical process and is beyond the scope of a simplified model whose fundamental limitation is the assumption that the Cauchy Horizon always exist at \(v=\infty \). Thirdly, a divergence in the asymptotic mass \(m_+\) may just not be fatal for the geometry as the Misner-Sharp mass controlling the curvature of spacetime may remain finite. This is clear from Eq. (10.65) which shows that the limit \(m\rightarrow \infty \) has different physical implications for the Reissner–Nordström and Hayward geometry. Most remarkably, very similar conclusions have already been reached when analyzing the mass-inflation effect for loop black holes [59]. For a recent discussion of this viewpoint by the authors of [69, 70] also see [71].
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Acknowledgements
We thank our collaborators N. Alkhofer, J. Daas, M. Galis, G. d’Odorico, I. van der Pas, A. Platania, A. Khosravi, B. Koch,, S. Silveravalle, F. Vidotto, M. Wondrak, and, foremost, M. Reuter for many inspiring discussions developing our understanding of spacetime singularities, regular black holes, and the stability properties of Cauchy horizons. The work of F.S. is supported by the Dutch Black Hole Consortium.
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Bonanno, A., Saueressig, F. (2023). Stability Properties of Regular Black Holes. In: Bambi, C. (eds) Regular Black Holes. Springer Series in Astrophysics and Cosmology. Springer, Singapore. https://doi.org/10.1007/978-981-99-1596-5_10
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