Abstract

A coherent picture of the quantum mechanics of a collapse-formed, evaporating black hole is presented. In a distant frame, semiclassical theory in the zone describes microscopic dynamics of only the "hard modes," the modes that are hard enough to be discriminated in the timescale of Hawking emission. The thermal nature of these modes arises from microcanonical typicality of the full black hole degrees of freedom, mostly composed of the "soft modes," the modes that cannot be discriminated at the semiclassical level. The hard modes are purified by a combined system of the soft modes and early Hawking radiation, but not by either of them separately. This intrinsically tripartite structure of entanglement is general, regardless of the age of the black hole. The interior spacetime emerges only at a coarse-grained level. To describe it, an effective theory can be erected at each time, which applies only to a limited spacetime region determined by the time at which the theory is erected. The entire interior of the black hole can be described only using multiple effective theories erected at different times, realizing the idea of complementarity. We analyze implications of the entanglement structure described here for various phenomena, including Hawking evaporation and general information retrieval. For multiple entangled black holes, it implies that semiclassical objects dropped into different black holes cannot meet in the interior, although each object smoothly enters the horizon of the black hole to which it is falling. We also discuss physics in Rindler space, elucidating how it is obtained as a smooth limit of the black hole physics.

Highlights

  • A black hole is an object in general relativity from which nothing can escape

  • We find that entanglement between the hard mode, soft mode, and early radiation d.o.f. takes an intrinsically tripartite form, regardless of the age of the black hole

  • A key ingredient is that semiclassical theory in a distant view describes microscopic dynamics of only the hard modes: the d.o.f. that are hard enough to be discriminated within the characteristic timescale of black hole evolution, tH ≈ Ml2P

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Summary

INTRODUCTION

A black hole is an object in general relativity from which nothing can escape. As in any other object, its entropy, formally defined as the logarithm of the number of independent states in a fixed energy interval, is infinity at the classical level Scl 1⁄4 ∞, which would give zero temperature Tcl 1⁄4 ð∂Scl=∂EÞ−1 1⁄4 0. (iv) Since the spacetime region described by each effective theory is limited, the entire interior of a black hole can be covered only using multiple effective theories erected at different times, which are generally not mutually independent. This provides a specific way in which the idea of complementarity is implemented. The entanglement structure between the hard modes, soft modes, and early radiation described above is intrinsically tripartite and, in a sense, is reminiscent of the GreenbergerHorne-Zeilinger (GHZ) form [29] It implies, together with a simple assumption about the dynamics of the black hole, that manipulating early Hawking radiation alone cannot destroy a smooth horizon of the black hole. It clarifies “information flow” associated with the Unruh effect

Relation to other work
Outline
BLACK HOLE AND INFORMATION
Black hole microstates
Semiclassical description and the static background approximation
Hawking emission
Distribution of microscopic information
Information transfer
Evolution of microscopic entanglement
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INTERIOR SPACETIME
An object falling into a black hole
Emergence of the interior
Two-sided description
Effective theories of the interior
Resolution of the cloning paradox
RINDLER LIMIT
Black hole mining
Unruh effect
Mirror operators
Information retrieval
ENTANGLED BLACK HOLES
A pair of black holes
Entanglement structure
Interior spacetime without a wormhole
More than two black holes
CONCLUSIONS AND DISCUSSION
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