Entanglement wedge reconstruction and the information paradox

Abstract When absorbing boundary conditions are used to evaporate a black hole in AdS/CFT, we show that there is a phase transition in the location of the quantum Ryu-Takayanagi surface, at precisely the Page time. The new RT surface lies slightly inside the event horizon, at an infalling time appro...

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Main Author: Geoffrey Penington
Format: Article
Language:English
Published: SpringerOpen 2020-09-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP09(2020)002
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author Geoffrey Penington
author_facet Geoffrey Penington
author_sort Geoffrey Penington
collection DOAJ
description Abstract When absorbing boundary conditions are used to evaporate a black hole in AdS/CFT, we show that there is a phase transition in the location of the quantum Ryu-Takayanagi surface, at precisely the Page time. The new RT surface lies slightly inside the event horizon, at an infalling time approximately the scrambling time β/2πlogS BH into the past. We can immediately derive the Page curve, using the Ryu-Takayanagi formula, and the Hayden-Preskill decoding criterion, using entanglement wedge reconstruction. Because part of the interior is now encoded in the early Hawking radiation, the decreasing entanglement entropy of the black hole is exactly consistent with the semiclassical bulk entanglement of the late-time Hawking modes, despite the absence of a firewall. By studying the entanglement wedge of highly mixed states, we can understand the state dependence of the interior reconstructions. A crucial role is played by the existence of tiny, non-perturbative errors in entanglement wedge reconstruction. Directly after the Page time, interior operators can only be reconstructed from the Hawking radiation if the initial state of the black hole is known. As the black hole continues to evaporate, reconstructions become possible that simultaneously work for a large class of initial states. Using similar techniques, we generalise Hayden-Preskill to show how the amount of Hawking radiation required to reconstruct a large diary, thrown into the black hole, depends on both the energy and the entropy of the diary. Finally we argue that, before the evaporation begins, a single, state-independent interior reconstruction exists for any code space of microstates with entropy strictly less than the Bekenstein-Hawking entropy, and show that this is sufficient state dependence to avoid the AMPSS typical-state firewall paradox.
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spelling doaj.art-5e8644c242cb43908f0fc4957000eae82022-12-21T23:57:14ZengSpringerOpenJournal of High Energy Physics1029-84792020-09-012020918410.1007/JHEP09(2020)002Entanglement wedge reconstruction and the information paradoxGeoffrey Penington0Stanford Institute for Theoretical Physics, Stanford UniversityAbstract When absorbing boundary conditions are used to evaporate a black hole in AdS/CFT, we show that there is a phase transition in the location of the quantum Ryu-Takayanagi surface, at precisely the Page time. The new RT surface lies slightly inside the event horizon, at an infalling time approximately the scrambling time β/2πlogS BH into the past. We can immediately derive the Page curve, using the Ryu-Takayanagi formula, and the Hayden-Preskill decoding criterion, using entanglement wedge reconstruction. Because part of the interior is now encoded in the early Hawking radiation, the decreasing entanglement entropy of the black hole is exactly consistent with the semiclassical bulk entanglement of the late-time Hawking modes, despite the absence of a firewall. By studying the entanglement wedge of highly mixed states, we can understand the state dependence of the interior reconstructions. A crucial role is played by the existence of tiny, non-perturbative errors in entanglement wedge reconstruction. Directly after the Page time, interior operators can only be reconstructed from the Hawking radiation if the initial state of the black hole is known. As the black hole continues to evaporate, reconstructions become possible that simultaneously work for a large class of initial states. Using similar techniques, we generalise Hayden-Preskill to show how the amount of Hawking radiation required to reconstruct a large diary, thrown into the black hole, depends on both the energy and the entropy of the diary. Finally we argue that, before the evaporation begins, a single, state-independent interior reconstruction exists for any code space of microstates with entropy strictly less than the Bekenstein-Hawking entropy, and show that this is sufficient state dependence to avoid the AMPSS typical-state firewall paradox.http://link.springer.com/article/10.1007/JHEP09(2020)002AdS-CFT CorrespondenceBlack HolesBlack Holes in String Theory
spellingShingle Geoffrey Penington
Entanglement wedge reconstruction and the information paradox
Journal of High Energy Physics
AdS-CFT Correspondence
Black Holes
Black Holes in String Theory
title Entanglement wedge reconstruction and the information paradox
title_full Entanglement wedge reconstruction and the information paradox
title_fullStr Entanglement wedge reconstruction and the information paradox
title_full_unstemmed Entanglement wedge reconstruction and the information paradox
title_short Entanglement wedge reconstruction and the information paradox
title_sort entanglement wedge reconstruction and the information paradox
topic AdS-CFT Correspondence
Black Holes
Black Holes in String Theory
url http://link.springer.com/article/10.1007/JHEP09(2020)002
work_keys_str_mv AT geoffreypenington entanglementwedgereconstructionandtheinformationparadox