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Distinguishing Random and Black Hole Microstates

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arxiv 2108.00011 v1 pith:6OV33NAN submitted 2021-07-30 hep-th cond-mat.stat-mechquant-ph

Distinguishing Random and Black Hole Microstates

classification hep-th cond-mat.stat-mechquant-ph
keywords blackrandomentropyholerelativemicrostatesnetworksstates
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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This is an expanded version of the short report [Phys. Rev. Lett. 126, 171603 (2021)], where the relative entropy was used to distinguish random states drawn from the Wishart ensemble as well as black hole microstates. In this work, we expand these ideas by computing many generalizations including the Petz R\'enyi relative entropy, sandwiched R\'enyi relative entropy, fidelities, and trace distances. These generalized quantities are able to teach us about new structures in the space of random states and black hole microstates where the von Neumann and relative entropies were insufficient. We further generalize to generic random tensor networks where new phenomena arise due to the locality in the networks. These phenomena sharpen the relationship between holographic states and random tensor networks. We discuss the implications of our results on the black hole information problem using replica wormholes, specifically the state dependence (hair) in Hawking radiation. Understanding the differences between Hawking radiation of distinct evaporating black holes is an important piece of the information problem that was not addressed by entropy calculations using the island formula. We interpret our results in the language of quantum hypothesis testing and the subsystem eigenstate thermalization hypothesis (ETH), deriving that chaotic (including holographic) systems obey subsystem ETH for all subsystems less than half the total system size.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Evaporating Black Hole Interior and Complexity Evolution

    hep-th 2026-05 conditional novelty 7.0

    In JT gravity with an end-of-the-world brane, the renormalized interior length — read as subsystem complexity — grows linearly, peaks around the Page time, and then decays exponentially, with growing relative fluctuat...

  2. Evaporating Black Hole Interior and Complexity Evolution

    hep-th 2026-05 unverdicted novelty 6.0

    In a JT gravity model with an EoW brane, black hole interior complexity grows linearly until the Page time then decays exponentially, with fluctuations growing large afterward and signaling loss of self-averaging.