Abstract

Recently, various authors have proposed that the first ultraviolet effect on the gravitational collapse of massive stars to black holes is the transition between a black-hole geometry and a white-hole geometry, though their proposals are radically different in terms of their physical interpretation and characteristic time scales [1,2]. Several decades ago, it was shown by Eardley that white holes are highly unstable to the accretion of small amounts of matter, being rapidly turned into black holes [3]. Studying the crossing of null shells on geometries describing the black-hole to white-hole transition, we obtain the conditions for the instability to develop in terms of the parameters of these geometries. We conclude that transitions with long characteristic time scales are pathologically unstable: occasional perturbations away from the perfect vacuum around these compact objects, even if being imperceptibly small, suffocate the white hole explosion. On the other hand, geometries with short characteristic time scales are shown to be robust against perturbations, so that the corresponding processes could take place in real astrophysical scenarios. This motivates a conjecture about the transition amplitudes of different decay channels for black holes in a suitable ultraviolet completion of general relativity.

Highlights

  • JHEP01(2016)157 matter content was constructed, in the short essay [1] and its companion article [10]

  • Recently, various authors have proposed that the dominant ultraviolet effect in the gravitational collapse of massive stars to black holes is the transition between a black-hole geometry and a white-hole geometry, though their proposals are radically different in terms of their physical interpretation and characteristic time scales [1, 2]

  • These geometries can be understood as the bounce of the matter distribution when Planckian curvatures are reached, and the corresponding propagation of a non-perturbative shock wave that goes along the distribution of matter and modifies the near-horizon Schwarzschild geometry, turning the black-hole horizon into a white-hole horizon [4]

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Summary

Eardley’s instability

One may argue that the reason for the instability of white holes to the accretion of matter is the following. This very phenomenon does not really require of a white hole, as it only depends on the local properties of spacetime around the crossing point of the ingoing and outgoing null shells. These additional sources of instabilities pile up, making even stronger the case for the unstable character of white holes

The geometric setting
Accretion and instabilities
Extending the analysis to the non-standard transition region
Decay channels for black holes
Conclusions
Full Text
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