Self-Gravity and Bekenstein-Hawking Entropy
arXiv:2207.14274 · doi:10.1016/j.nuclphysb.2024.116531
Abstract
We study the effect of self-gravity on entropy by directly solving the 4D semi-classical Einstein equation. In particular, we focus on whether the Bekenstein-Hawking formula holds when self-gravity is extremely strong. As an example, we consider a simple spherically symmetric static configuration consisting of many quanta and construct a self-consistent non-perturbative solution for in which the entropy exactly follows the area law for many local degrees of freedom of any kind. This can be a candidate for black holes in quantum theory. It represents a compact dense configuration with near-Planckian curvatures, and the interior typically behaves like a local thermal state due to particle creation. Here, the information content is stored in the interior bulk, and the self-gravity plays an essential role in changing the entropy from the volume law to the area law. We finally discuss implications to black holes in quantum gravity and a speculative view of entropy as a gravitational charge.
20 pages + 3 figures. Version published in Nuclear Physics B. (With keeping the main results, change the title and abstract; modified and expanded Introduction and Conclusion including relations with other works and several new discussions; added references.)
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