Abstract

We consider the Hawking radiation emitted by an evaporating black hole in JT gravity and compute the entropy of arbitrary subsets of the radiation in the slow evaporation limit, and find a zoo of possible island saddles. The Hawking radiation is shown to have long range correlations. We compute the mutual information between early and late modes and bound from below their squashed entanglement. A small subset of late modes are shown to be correlated with modes in a suitably large subset of the radiation previously emitted as well as later modes. We show how there is a breakdown of the semi-classical approximation in the form of a violation of the Araki–Lieb triangle entropy inequality, if the interior of the black hole and the radiation are considered to be separate systems. Finally, we consider how much of the radiation must be collected, and how early, to recover information thrown into the black hole as it evaporates.

Highlights

  • Recent work [1, 2] has led to a step change in understanding the information loss paradox of black holes

  • We consider the Hawking radiation emitted by an evaporating black hole in JT gravity and compute the entropy of arbitrary subsets of the radiation in the slow evaporation limit, and find a zoo of possible island saddles

  • We focussed attention on island saddles with only two QESs since we generically expect additional QES contributions to significantly increase the entropy

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Summary

Introduction

Recent work [1, 2] has led to a step change in understanding the information loss paradox of black holes. The Page curve has been derived in these, or related, scenarios [1, 2, 6,7,8] (see [9,10,11]) It is a goal of this work, to show that replica wormhole techniques, and the effective rules that they give rise to, mean that more refined information processing properties of black holes can be calculated from first principles via standard quantum field theory calculations.

Entropy as an observable
The evaporating black hole
Entropy of arbitrary intervals
Island saddles
Two-QES saddles: one behind shockwave
Both QES behind the shockwave
Position of the QES and scrambling time
Mutual information
Quantum correlations
Entropy consistency conditions
Hunt the purifier
Searching for RB in the past
Searching for RB in the future
Entanglement-monogamy problem
Recovering information
Black hole as a mirror scenario
Recovery after the fact
Behind the horizon in the bath
Findings
Discussion

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