Hayden-Preskill model via local quenches

A bstract We model the Hayden-Preskill (HP) information recovery protocol in 2d CFTs via local joining quenches. Euclidean path integrals with slits prepare the HP subsystems: the message M , its reference N , the Page-time black hole B , the early radiation E , and the late radiation R ; the remaining black hole after emitting R is denoted as B ′ . The single-slit geometry provides an analytically tractable toy model, while the bounded-slit geometry more closely captures the HP setup. In the free Dirac fermion 2d CFT, the mutual information I ( N : B ′ ) shows quasi-particle dynamics with partial or full revivals, whereas that in holographic 2d CFTs, which are expected to be maximally chaotic, exhibits sharp transitions: in the bounded-slit case, when the size of the late radiation becomes comparable to that of the reference N , I ( N : B ′ ) vanishes at late time, otherwise it remains finite. This contrast between free CFTs and holographic CFTs gives a clear characterization of the HP recovery threshold.

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Publication Details

Journal
Journal of High Energy Physics
Published
2026-03-24
DOI
https://doi.org/10.1007/jhep03(2026)232
Primary Topic
Black Holes and Theoretical Physics
Type
article
Field-Weighted Citation Impact
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article

Hayden-Preskill model via local quenches

Journal of High Energy Physics
Black Holes and Theoretical Physics
article

Hayden-Preskill model via local quenches

article en

Abstract

A bstract We model the Hayden-Preskill (HP) information recovery protocol in 2d CFTs via local joining quenches. Euclidean path integrals with slits prepare the HP subsystems: the message M , its reference N , the Page-time black hole B , the early radiation E , and the late radiation R ; the remaining black hole after emitting R is denoted as B ′ . The single-slit geometry provides an analytically tractable toy model, while the bounded-slit geometry more closely captures the HP setup. In the free Dirac fermion 2d CFT, the mutual information I ( N : B ′ ) shows quasi-particle dynamics with partial or full revivals, whereas that in holographic 2d CFTs, which are expected to be maximally chaotic, exhibits sharp transitions: in the bounded-slit case, when the size of the late radiation becomes comparable to that of the reference N , I ( N : B ′ ) vanishes at late time, otherwise it remains finite. This contrast between free CFTs and holographic CFTs gives a clear characterization of the HP recovery threshold.

Journal of High Energy PhysicsVol. 2026(3)
Kyoto University (JP), University of Chinese Academy of Sciences (CN)
Openalex Percentile: Top 11%
Black Holes and Theoretical Physics
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