2022
DOI: 10.1007/jhep01(2022)078
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Ephemeral islands, plunging quantum extremal surfaces and BCFT channels

Abstract: We consider entanglement entropies of finite spatial intervals in Minkowski radiation baths coupled to the eternal black hole in JT gravity, and the related problem involving free fermion BCFT in the thermofield double state. We show that the non-monotonic entropy evolution in the black hole problem precisely matches that of the free fermion theory in a high temperature limit, and the results have the form expected for CFTs with quasiparticle description. Both exhibit rich behaviour that involves at intermedia… Show more

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Cited by 18 publications
(9 citation statements)
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“…See[72][73][74][75][76][77][78][79][80] and the references therein 4. See[44,57,[84][85][86] for the recent explorations of BCFT.…”
mentioning
confidence: 99%
“…See[72][73][74][75][76][77][78][79][80] and the references therein 4. See[44,57,[84][85][86] for the recent explorations of BCFT.…”
mentioning
confidence: 99%
“…. , p, with u 0 = 0 and where |u j − u j−1 | ∆t s , 12 then R can be taken to be a subset of {A j }. The set up is shown schematically in figure 5.…”
Section: General Radiation Region Rmentioning
confidence: 99%
“…By the notation S n i (N i ) we mean permutations of n i elements starting at N i + 1 where N i = j<i n j . For example, for S 3 (5) we would generate states such as |a (678) in the twist-3 sector or |a (68) (7) in the twist-2 times untwisted sector. The second sum over S N simply makes the state invariant under permutations so that it is a well-defined orbifold state.…”
Section: An Ansatz For the Boundary Statesmentioning
confidence: 99%
“…n = N î) and analyze the AdS/BCFT data for such states. 7 The notion of typicality will now constrain what type of representation vector r we pick. Since we pick all states to be the same, it involves understanding what a typical representation of S N looks like.…”
Section: Finite Seed Cftsmentioning
confidence: 99%
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