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Entropy and temperature of black holes in a gravity's rainbow

General Relativity and Quantum Cosmology · Submitted 11 Aug 2006

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

The authors' main claim We show that, for a family of doubly special relativity theories satisfying certain properties, the temperature can vanish in the limit of zero black hole mass.

how it is stated · asserted 0.96 read the record →

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arXiv IDgr-qc/0608061 (version 2)
Pith IDEOKDFINN, Pith's permanent record of this paper and its review
CitationGuillermo A. Mena Marugan, Pablo Galan. "Entropy and temperature of black holes in a gravity's rainbow." arXiv:gr-qc/0608061 (2006). https://pith.science/paper/EOKDFINN
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What the abstract itself states, as probabilities: claims first 0.04 · states limitation 0.66 · human participants 0.01 · controlled comparison 0.07 · randomized assignment 0.01 · states quantitative result 0.16 · compares with prior results 0.82 · mentions code or data availability 0.02.

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arXiv listing abstract v2. Results and the main claim are underlined; .

The linear relation between the entropy and area of a black hole can be derived from the Heisenberg principle, the energy-momentum dispersion relation of special relativity, and general considerations about black holes. There exist results in quantum gravity and related contexts suggesting the modification of the usual dispersion relation and uncertainty principle. One of these contexts is the gravity's rainbow formalism. We analyze the consequences of such a modification for black hole thermodynamics from the perspective of two distinct rainbow realizations built from doubly special relativity. One is the proposal of Magueijo and Smolin and the other is based on a canonical implementation of doubly special relativity put forward recently by the authors. In these scenarios, we obtain modified expressions for the entropy and temperature of black holes. We show that, for a family of doubly special relativity theories satisfying certain properties, the temperature can vanish in the limit of zero black hole mass. For the Magueijo and Smolin proposal, this is only possible for some restricted class of models with bounded energy and unbounded momentum. With the proposal of a canonical implementation, on the other hand, the temperature may vanish for more general theories; in particular, the momentum may also be bounded, with bounded or unbounded energy. This opens new possibilities for the outcome of black hole evaporation in the framework of a gravity's rainbow.

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 linear relation between the entropy and area of a black hole can be derived from the Heisenberg principle, the energy-momentum dispersion relation of special relativity, and general considerations about black holes. background 1.00 0.12 0.03 asserted 0.97
s1 There exist results in quantum gravity and related contexts suggesting the modification of the usual dispersion relation and uncertainty principle. background 1.00 0.04 0.02 hedged possibility 0.77
s2 One of these contexts is the gravity's rainbow formalism. background 1.00 0.04 0.02 asserted 0.98
s3 We analyze the consequences of such a modification for black hole thermodynamics from the perspective of two distinct rainbow realizations built from doubly special relativity. contribution 0.95 0.85 0.06 asserted 0.92
s4 One is the proposal of Magueijo and Smolin and the other is based on a canonical implementation of doubly special relativity put forward recently by the authors. method 0.71 0.19 0.03 asserted 0.99
s5 In these scenarios, we obtain modified expressions for the entropy and temperature of black holes. result 0.86 0.94 0.23 asserted 1.00
s6 We show that, for a family of doubly special relativity theories satisfying certain properties, the temperature can vanish in the limit of zero black hole mass. result 1.00 0.93 0.39 asserted 0.96
s7 For the Magueijo and Smolin proposal, this is only possible for some restricted class of models with bounded energy and unbounded momentum. result 0.92 0.76 0.09 hedged possibility 0.57
s8 With the proposal of a canonical implementation, on the other hand, the temperature may vanish for more general theories; in particular, the momentum may also be bounded, with bounded or unbounded energy. result 0.99 0.84 0.20 hedged possibility 0.99
s9 This opens new possibilities for the outcome of black hole evaporation in the framework of a gravity's rainbow. interpretation 1.00 0.53 0.27 hedged possibility 0.71

What kind of paper the classifier reports this is: theoretical result 1.00 · evidence from proof or derivation 0.99.

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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 linear relation between the entropy and area of a black hole can be derived from the Heisenberg principle, the energy-momentum dispersion relation of special relativity, and general considerations about black holes. There exist results in quantum gravity and related contexts suggesting the modification of the usual dispersion relation and uncertainty principle. One of these contexts is the gravity's rainbow formalism. We analyze the consequences of such a modification for black hole thermodynamics from the perspective of two distinct rainbow realizations built from doubly special relativity. One is the proposal of Magueijo and Smolin and the other is based on a canonical implementation of doubly special relativity put forward recently by the authors. In these scenarios, we obtain modified expressions for the entropy and temperature of black holes. We show that, for a family of doubly special relativity theories satisfying certain properties, the temperature can vanish in the limit of zero black hole mass. For the Magueijo and Smolin proposal, this is only possible for some restricted class of models with bounded energy and unbounded momentum. With the proposal of a canonical implementation, on the other hand, the temperature may vanish for more general theories; in particular, the momentum may also be bounded, with bounded or unbounded energy. This opens new possibilities for the outcome of black hole evaporation in the framework of a gravity's rainbow.

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References
How the literature uses it

13 arXiv papers cite this in 17 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 · 8 sentences without a confident label

Uses its method or tool 1 paper
  • Suppose we make the measurement with the use of radiation photons with average energy $E=<E>$, then we expect that the temperature of black holes can be identified with the energy of photons emitted from black hole [ref] , namely $T = E$.

    Modified (A)dS Schwarzschild black holes in Rainbow spacetime · Thermodynamics with the modified (A)dS Schwarzschild black holes · 0.87

Cites it as background 7 papers
  • Out of such theories, the Rastall [ref] and Rainbow [ref] and combined Rastall-Rainbow [ref] formalisms have attracted a lot of interest in the fields of astrophysics and cosmology in recent times [ref] .

    Bose-Einstein condensate stars in combined Rastall-Rainbow gravity · Introduction · 0.96

  • Rainbow black-hole thermodynamics was developed through energy-dependent temperature and entropy relations [ref] , while rainbow cosmology generalized the Friedmann description to energy-dependent geometries [ref] .

    Rainbow McVittie Horizons in an Expanding Universe · Introduction · 0.97

  • Rainbow gravity formalism has received a lot of attention recently and other stimulating work on this formalism can be found, for instance, in [ref] .

    The Big Bounce in Rainbow Universe · Introduction · 1.00

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