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Do Black Holes Store Negative Entropy?

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Peer-reviewed

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Abstract

Abstract The Bekenstein–Hawking equation states that black holes should have entropy proportional to their areas to make black hole physics compatible with the second law of thermodynamics. However, this equation leads to an inconsistency among the first law of black hole mechanics, the entropy conservation law of quantum mechanics, and a heuristic picture for Hawking radiation—creation of entangled pairs near the horizon. Here we propose an equation alternative to the Bekenstein–Hawking equation from the viewpoint of quantum information, to resolve this inconsistency without changing Hawking’s original pair-creation picture for the radiation. This argues that the area of any stationary black hole, including Kerr and charged ones, is proportional to the coherent information—which is “minus” the conditional entropy defined only in the quantum regime—from the outside, to the black hole excluding negative-frequency particles generated by Hawking’s pair creation. Our equation suggests that negative-frequency particles inside a black hole behave as if they have “negative” entropy. Our result implies that a black hole stores purely quantum information, rather than classical information, and the area of the event horizon describes the number of Bell pairs that can be distilled between the interior and exterior.

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Acknowledgements: We sincerely thank R. Jozsa for speculating about the possibility that the negative-frequency particles “falling into” a black hole may have negative entropy, M. Koashi for having informed K.A. of an interesting implication coming from an analogy between two-mode squeezed states and Hawking radiation ten years ago, and H.-K. Lo for emphasizing the observer dependence of quantum field theory in a curved spacetime. K.A. is especially grateful to R. Jozsa and the University of Cambridge for giving him an opportunity to stay in R. Jozsa’s group during his sabbatical. We also thank T. Honjo, M. Hotta, K. Inaba, W. J. Munro, Y. Nakata, K. Shimizu, and T. Takayanagi for helpful discussions. K.A. is grateful for the support, in part, from PRESTO, JST JP-MJPR1861; from CREST, JST JP-MJCR1671; from Moonshot R&D, JST JPMJMS2061; from MEXT-JSPS Grant-in-Aid for Transformative Research Areas (A), No. 21H05183; and from R&D of ICT Priority Technology (JPMI00316). S.S. is supported by a Royal Commission for the Exhibition of 1851 Research Fellowship. Part of this work was done when S.S. was a PhD student at DAMTP, University of Cambridge, supported by the SERB (Government of India) and the Cambridge Trust through a Cambridge–India Ramanujan scholarship. G.K. is grateful for the support, in part, from the JSPS Kakenhi (C) No. 17K05591, (C) No. 20K03779, (C) No. 21K03388, and JST CREST JPMJCR2113. Part of this work was done when G.K. belonged to NTT Communication Science Laboratories.


Funder: SCOAP

Journal Title

Progress of Theoretical and Experimental Physics

Conference Name

Journal ISSN

0033-068X
2050-3911

Volume Title

2025

Publisher

Oxford University Press (OUP)

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Except where otherwised noted, this item's license is described as https://creativecommons.org/licenses/by/4.0/