Self-gravity and Bekenstein-Hawking entropy

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 co...

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Main Author: Yuki Yokokura
Format: Article
Language:English
Published: Elsevier 2024-05-01
Series:Nuclear Physics B
Online Access:http://www.sciencedirect.com/science/article/pii/S055032132400097X
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author Yuki Yokokura
author_facet Yuki Yokokura
author_sort Yuki Yokokura
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description 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 ħ 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 inside. 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.
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spelling doaj.art-348cc777029f451fb041677991803e872024-04-13T04:20:56ZengElsevierNuclear Physics B0550-32132024-05-011002116531Self-gravity and Bekenstein-Hawking entropyYuki Yokokura0iTHEMS Program, RIKEN, Wako, Saitama 351-0198, JapanWe 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 ħ 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 inside. 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.http://www.sciencedirect.com/science/article/pii/S055032132400097X
spellingShingle Yuki Yokokura
Self-gravity and Bekenstein-Hawking entropy
Nuclear Physics B
title Self-gravity and Bekenstein-Hawking entropy
title_full Self-gravity and Bekenstein-Hawking entropy
title_fullStr Self-gravity and Bekenstein-Hawking entropy
title_full_unstemmed Self-gravity and Bekenstein-Hawking entropy
title_short Self-gravity and Bekenstein-Hawking entropy
title_sort self gravity and bekenstein hawking entropy
url http://www.sciencedirect.com/science/article/pii/S055032132400097X
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