Preprint Article Version 1 Preserved in Portico This version is not peer-reviewed

Black Hole Entropy from Non-Dirichlet Sectors, and Bounce Solution

Version 1 : Received: 19 September 2022 / Approved: 23 September 2022 / Online: 23 September 2022 (02:06:59 CEST)

How to cite: Park, I. Black Hole Entropy from Non-Dirichlet Sectors, and Bounce Solution. Preprints 2022, 2022090350 (doi: 10.20944/preprints202209.0350.v1). Park, I. Black Hole Entropy from Non-Dirichlet Sectors, and Bounce Solution. Preprints 2022, 2022090350 (doi: 10.20944/preprints202209.0350.v1).

Abstract

In a series of recent works the relevance of gravitational boundary degrees of freedom and their dynamics in gravity quantization and black hole information has been explored. In this work we further the progress by keenly focusing on the boundary degrees of freedom as the origin of black hole entropy. Wald's entropy formula is scrutinized, and the reason that the Wald's formula correctly captures the entropy of a black hole is examined. Afterwards, limitations of the Wald's method are discussed; a coherent view of entropy based on boundary dynamics is presented. The discrepancy observed in the literature between holographic and Wald's entropies is addressed. We generalize the entropy definition so as to handle a time-dependent black hole. Large gauge symmetry plays a pivotal role. Non-Dirichlet boundary conditions and gravitational analogues of Coleman-De Luccia bounce solutions are central in identifying the microstates and differentiating the origins of entropies associated with different classes of solutions. The result in the present work leads to a view that black hole entropy is entanglement entropy in a thermodynamic setup.

Keywords

black hole entropy; non-Dirichlet boundary condition; bounce

Subject

PHYSICAL SCIENCES, Acoustics

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