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The Holographic Map of an Evaporating Black Hole

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arxiv 2301.08362 v2 pith:MYT45RCA submitted 2023-01-19 hep-th cond-mat.stat-mechgr-qcquant-ph

The Holographic Map of an Evaporating Black Hole

classification hep-th cond-mat.stat-mechgr-qcquant-ph
keywords blackholehawkingradiationunitaryevaporatingholographicmicroscopic
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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We construct a holographic map that takes the semi-classical state of an evaporating black hole and its Hawking radiation to a microscopic model that reflects the scrambling dynamics of the black hole. The microscopic model is given by a nested sequence of random unitaries, each one implementing a scrambling time step of the black hole evolution. Differently from other models, energy conservation and the thermal nature of the Hawking radiation are taken into account. We show that the QES formula follows for the entropy of multiple subsets of the radiation and black hole. We further show that a version of entanglement wedge reconstruction can be proved by computing suitable trace norms and quantum fidelities involving the action of a unitary on a subset of Hawking partners. If the Hawking partner is in an island, its unitary can be reconstructed by a unitary on the radiation. We also adopt a similar setup and analyse reconstruction of unitaries acting on an infalling system.

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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.