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Backreaction of Hawking Radiation on a Gravitationally Collapsing Star I: Black Holes? (1406.1525v1)

Published 5 Jun 2014 in hep-th, gr-qc, and hep-ph

Abstract: Particle creation leading to Hawking radiation is produced by the changing gravitational field of the collapsing star. The two main initial conditions in the far past placed on the quantum field from which particles arise, are the Hartle Hawking vacuum and the Unruh vacuum. The former leads to a time symmetric thermal bath of radiation, while the latter to a flux of radiation coming out of the collapsing star. The energy of Hawking radiation in the interior of the collapsing star is negative and equal in magnitude to its value at future infinity. This work investigates the backreaction of Hawking radiation on the interior of a gravitationally collapsing star, in a Hartle-Hawking initial vacuum. It shows that due to the negative energy Hawking radiation in the interior, the collapse of the star stops at a finite radius, before the singularity and the event horizon of a black hole have a chance to form. That is, the star bounces instead of collapsing to a black hole. A trapped surface near the last stage of the star's collapse to its minimum size may still exist temporarily. Its formation depends on the details of collapse. Results for the case of Hawking flux of radiation with the Unruh initial state, will be given in a companion paper II.

Citations (73)
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Summary

Analysis of Hawking Radiation's Backreaction on Gravitational Collapse

The paper by Laura Mersini-Houghton investigates the significant question of whether black holes form during the gravitational collapse of stars, taking into account the backreaction effects of Hawking radiation on the stars' interior dynamics. It revisits conventional dogma from Oppenheimer and Snyder's work, which concluded that black holes are the inevitable end-state of massive stars collapsing under gravity. By considering quantum effects within general relativity, this paper probes whether the very existence of black holes might be refutable under certain physical assumptions.

The focal point of the paper is the backreaction impact of Hawking radiation—a predicted quantum effect whereby collapsing stars give rise to particle creation due to changing gravitational fields—on the interior dynamics of spherically symmetric, homogeneous stars. Using a Hartle-Hawking vacuum as the initial state of the quantum field, this paper reveals that the resulting negative energy density from Hawking radiation within the collapsing star can halt the collapse before reaching a singularity or forming an event horizon. It suggests that such a star will rebound, avoiding the conventional black hole formation.

The theoretical framework employs foundational hydrodynamic equations augmented by quantum inputs within general relativity. Applying the Hartle-Hawking vacuum, which embodies a symmetric arrangement of thermal radiation, the paper integrates the backreaction effects into a Friedmann-Robertson-Walker (FRW) metric to describe the star's interior. It demonstrates mathematically that the star effectively achieves a bounce when encountering a finite radius, rather than progressing toward a gravitational singularity.

While the interior of the star is described by an FRW-type cosmological model, the paper also ensures consistency with the Schwarzschild exterior solution. The analysis captures complex interactions between quantum field effects and relativistic gravity, particularly focusing on how the Hawking radiation backreaction dynamically influences the collapse trajectory.

A noteworthy result is the temporary presence of trapped surfaces within the collapsing star. Although these phenomena mirror some aspects of black hole behavior, they are ephemeral, suggesting that information might not be entirely lost as traditionally predicted. Furthermore, the paper argues that understanding whether such temporary trapped surfaces exist could vary depending on collapse specifics and rates, notwithstanding the non-dependence of Hawking radiation on the collapse details themselves. This nuance suggests an intricate interplay between theoretical formulations and physical parameters in determining the existence of trapped surfaces.

The paper also references the significant role of negative energy density contributions from Hawking radiation—crucial in defusing the conventional singularity formation scenario posited by the Penrose-Hawking singularity theorems. This serves to highlight a unique interaction where classical singularity resolution might be mediated by quantum effects in extreme astrophysical settings.

In conclusion, this research offers a novel outlook on gravitational collapse by incorporating quantum processes, rendering a potential theoretical scenario where black holes might not form as traditionally envisioned. While the paper’s findings rest on simplified stellar models retaining homogeneity and isotropy, its implications motivate further theoretical and computational inquiries into more realistic settings. Exploring inhomogeneities and perturbations around these symmetric assumptions could provide deeper insights into the stability and robustness of the suggested star bounce phenomenon. Additionally, extending the analysis to other vacuum states, notably the Unruh vacuum in subsequent work, could fortify or challenge the conclusions drawn here by offering comparisons.

This investigation onto the quantum backreaction presents a compelling dialogue between quantum field theory and gravitational physics, imbuing a more intricate understanding of potential end-states of stellar evolution. As numerical methods advance, conceivably incorporating further complex interactions within realistic astrophysical environments, the prospect of recasting our understanding of black hole formation remains a promising avenue for future research.

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