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Firewalls, smoke and mirrors

High Energy Physics - Theory · Submitted 7 Jan 2014

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim And so our previously proposed model which has $N_{coh}=S_{BH}^{1/2}$ is singled out.

how it is stated · asserted 1.00 read the record →

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arXiv ID1401.1401 (version 1)
Pith IDFMQ7E4AV, Pith's permanent record of this paper and its review
CitationA.J.M. Medved, Ram Brustein. "Firewalls, smoke and mirrors." arXiv:1401.1401 (2014). https://pith.science/paper/FMQ7E4AV
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The compiled record

The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.

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Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 7,749 input tokens, $0.0003 reported.

What the abstract itself states, as probabilities: claims first 0.05 · states limitation 0.61 · human participants 0.01 · controlled comparison 0.03 · randomized assignment 0.01 · states quantitative result 0.94 · compares with prior results 0.53 · mentions code or data availability 0.01.

The abstract, sentence by sentence

arXiv listing abstract v1. Results and the main claim are underlined; .

The radiation emitted by a black hole (BH) during its evaporation has to have some degree of quantum coherence to accommodate a unitary time evolution. We parametrize the degree of coherence by the number of coherently emitted particles $N_{coh}$ and show that it is severely constrained by the equivalence principle. We discuss, in this context, the fate of a shell of matter that falls into a Schwarzschild BH. Two points of view are considered, that of a stationary external observer and that of the shell itself. From the perspective of the shell, the near-horizon region has an energy density proportional to $N_{coh}^2$ in Schwarzschild units. So, if $N_{coh}$ is parameterically larger than the square root of the BH entropy $S_{BH}^ {1/2}$, a firewall or more generally a "wall of smoke" forms and the equivalence principle is violated while the BH is still semiclassical. To have a degree of coherence that is parametrically smaller than $S_{BH}^{1/2}$, one has to introduce a new sub-Planckian gravitational length scale, which likely also violates the equivalence principle. And so our previously proposed model which has $N_{coh}=S_{BH}^{1/2}$ is singled out. From the external-observer perspective, we find that the time it takes for the information about the state of the shell to get re-emitted from the BH is inversely proportional to $N_{coh}$. When the rate of information release becomes order unity, the semiclassical approximation starts to break down and the BH becomes a perfect reflecting information mirror.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 The radiation emitted by a black hole (BH) during its evaporation has to have some degree of quantum coherence to accommodate a unitary time evolution. background 1.00 0.09 0.06 asserted 0.83
s1 We parametrize the degree of coherence by the number of coherently emitted particles $N_{coh}$ and show that it is severely constrained by the equivalence principle. contribution 0.52 0.93 0.15 asserted 1.00
s2 We discuss, in this context, the fate of a shell of matter that falls into a Schwarzschild BH. contribution 0.72 0.58 0.03 unclear 0.70
s3 Two points of view are considered, that of a stationary external observer and that of the shell itself. method 0.80 0.60 0.02 asserted 0.76
s4 From the perspective of the shell, the near-horizon region has an energy density proportional to $N_{coh}^2$ in Schwarzschild units. result 0.97 0.82 0.05 asserted 1.00
s5 So, if $N_{coh}$ is parameterically larger than the square root of the BH entropy $S_{BH}^ {1/2}$, a firewall or more generally a "wall of smoke" forms and the equivalence principle is violated while the BH is still semiclassical. result 0.92 0.80 0.34 asserted 0.97
s6 To have a degree of coherence that is parametrically smaller than $S_{BH}^{1/2}$, one has to introduce a new sub-Planckian gravitational length scale, which likely also violates the equivalence principle. result 0.89 0.77 0.09 hedged possibility 0.93
s7 And so our previously proposed model which has $N_{coh}=S_{BH}^{1/2}$ is singled out. result 0.57 0.63 0.55 asserted 1.00
s8 From the external-observer perspective, we find that the time it takes for the information about the state of the shell to get re-emitted from the BH is inversely proportional to $N_{coh}$. result 0.99 0.93 0.09 asserted 1.00
s9 When the rate of information release becomes order unity, the semiclassical approximation starts to break down and the BH becomes a perfect reflecting information mirror. result 0.83 0.83 0.20 asserted 1.00

What kind of paper the classifier reports this is: theoretical result 0.99 · evidence from proof or derivation 0.79.

What was examined, and what was not

sources read
  • arXiv listing abstract v1
not examined
  • full text
  • figures and tables
  • references and citing sentences
  • relations to other papers
levels run
  • P abstract
not run
  • S sections
  • T body sentences
  • C citations
  • R cross-paper relations

Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

The paper
Original abstract

The radiation emitted by a black hole (BH) during its evaporation has to have some degree of quantum coherence to accommodate a unitary time evolution. We parametrize the degree of coherence by the number of coherently emitted particles $N_{coh}$ and show that it is severely constrained by the equivalence principle. We discuss, in this context, the fate of a shell of matter that falls into a Schwarzschild BH. Two points of view are considered, that of a stationary external observer and that of the shell itself. From the perspective of the shell, the near-horizon region has an energy density proportional to $N_{coh}^2$ in Schwarzschild units. So, if $N_{coh}$ is parameterically larger than the square root of the BH entropy $S_{BH}^ {1/2}$, a firewall or more generally a "wall of smoke" forms and the equivalence principle is violated while the BH is still semiclassical. To have a degree of coherence that is parametrically smaller than $S_{BH}^{1/2}$, one has to introduce a new sub-Planckian gravitational length scale, which likely also violates the equivalence principle. And so our previously proposed model which has $N_{coh}=S_{BH}^{1/2}$ is singled out. From the external-observer perspective, we find that the time it takes for the information about the state of the shell to get re-emitted from the BH is inversely proportional to $N_{coh}$. When the rate of information release becomes order unity, the semiclassical approximation starts to break down and the BH becomes a perfect reflecting information mirror.

Human review
References
How the literature uses it

9 arXiv papers cite this in 16 sentences

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers citing it · 13 sentences without a confident label

Cites it as background 3 papers

What it cites · 21 sentences without a confident label

Uses the method or tool of 7 papers
  • We do this, following ideas from [ref] (also see [ref] as well as [ref] ), by endowing the collapsing shell with a wavefunction and calculating expectation values where appropriate.

    Black hole entropy divergence and the uncertainty principle · Introduction · 0.97

  • We do this, following ideas from [ref] (also see [ref] as well as [ref] ), by endowing the collapsing shell with a wavefunction and calculating expectation values where appropriate.

    Black Hole's Quantum N-Portrait · Introduction · 0.97

  • We do this, following ideas from [ref] (also see [ref] as well as [ref] ), by endowing the collapsing shell with a wavefunction and calculating expectation values where appropriate.

    Wave function of the quantum black hole · Introduction · 0.97

Uses data or values from 1 paper
  • The off-diagonal matrix $Δρ_OD(ω_out,ω_in)$ was calculated in [ref] and can be treated as a uniform matrix within the thermal window, when $ω_out$, $ω_in∼T_H$.

    Horizons of semiclassical black holes are cold · Introduction · 0.84

Cites as background 22 papers

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