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Extremal non-BPS black holes and entropy extremization

High Energy Physics - Theory · Submitted 25 Jul 2006

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

The authors' main claim For the non-BPS solution the region of attractivity and the maximum of the entropy do not coincide with the conifold point.

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arXiv IDhep-th/0607202 (version 2)
Pith IDFAKFBFMG, Pith's permanent record of this paper and its review
CitationDieter Lust, Gabriel Lopes Cardoso, Jan Perz, Viviane Grass. "Extremal non-BPS black holes and entropy extremization." arXiv:hep-th/0607202 (2006). https://pith.science/paper/FAKFBFMG
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What the abstract itself states, as probabilities: claims first 0.03 · states limitation 0.30 · human participants 0.01 · controlled comparison 0.28 · randomized assignment 0.01 · states quantitative result 0.07 · compares with prior results 0.84 · mentions code or data availability 0.02.

The abstract, sentence by sentence

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

At the horizon, a static extremal black hole solution in N=2 supergravity in four dimensions is determined by a set of so-called attractor equations which, in the absence of higher-curvature interactions, can be derived as extremization conditions for the black hole potential or, equivalently, for the entropy function. We contrast both methods by explicitly solving the attractor equations for a one-modulus prepotential associated with the conifold. We find that near the conifold point, the non-supersymmetric solution has a substantially different behavior than the supersymmetric solution. We analyze the stability of the solutions and the extrema of the resulting entropy as a function of the modulus. For the non-BPS solution the region of attractivity and the maximum of the entropy do not coincide with the conifold point.

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 At the horizon, a static extremal black hole solution in N=2 supergravity in four dimensions is determined by a set of so-called attractor equations which, in the absence of higher-curvature interactions, can be derived as extremization conditions for the black hole potential or, equivalently, for the entropy function. background 1.00 0.08 0.05 asserted 1.00
s1 We contrast both methods by explicitly solving the attractor equations for a one-modulus prepotential associated with the conifold. method 0.65 0.95 0.05 asserted 0.97
s2 We find that near the conifold point, the non-supersymmetric solution has a substantially different behavior than the supersymmetric solution. result 1.00 0.96 0.28 asserted 1.00
s3 We analyze the stability of the solutions and the extrema of the resulting entropy as a function of the modulus. contribution 0.60 0.93 0.07 asserted 0.66
s4 For the non-BPS solution the region of attractivity and the maximum of the entropy do not coincide with the conifold point. result 1.00 0.92 0.58 asserted 1.00

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

At the horizon, a static extremal black hole solution in N=2 supergravity in four dimensions is determined by a set of so-called attractor equations which, in the absence of higher-curvature interactions, can be derived as extremization conditions for the black hole potential or, equivalently, for the entropy function. We contrast both methods by explicitly solving the attractor equations for a one-modulus prepotential associated with the conifold. We find that near the conifold point, the non-supersymmetric solution has a substantially different behavior than the supersymmetric solution. We analyze the stability of the solutions and the extrema of the resulting entropy as a function of the modulus. For the non-BPS solution the region of attractivity and the maximum of the entropy do not coincide with the conifold point.

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6 arXiv papers cite this in 6 sentences

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