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Charged Dilaton Black Holes with Unusual Asymptotics
General Relativity and Quantum Cosmology · Submitted 27 Feb 1995
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We present a new class of black hole solutions in Einstein-Maxwell-dilaton gravity in $n \ge 4$ dimensions.
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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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The abstract, sentence by sentence
We present a new class of black hole solutions in Einstein-Maxwell-dilaton gravity in $n \ge 4$ dimensions. These solutions have regular horizons and a singularity only at the origin. Their asymptotic behavior is neither asymptotically flat nor (anti-) de Sitter. Similar solutions exist for certain Liouville-type potentials for the dilaton.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We present a new class of black hole solutions in Einstein-Maxwell-dilaton gravity in $n \ge 4$ dimensions. | contribution 1.00 | 0.95 | 0.48 | asserted 1.00 |
| s1 | These solutions have regular horizons and a singularity only at the origin. | result 0.91 | 0.82 | 0.13 | asserted 1.00 |
| s2 | Their asymptotic behavior is neither asymptotically flat nor (anti-) de Sitter. | result 0.91 | 0.84 | 0.45 | asserted 1.00 |
| s3 | Similar solutions exist for certain Liouville-type potentials for the dilaton. | result 0.73 | 0.51 | 0.08 | asserted 0.93 |
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The paper
Original abstract
We present a new class of black hole solutions in Einstein-Maxwell-dilaton gravity in $n \ge 4$ dimensions. These solutions have regular horizons and a singularity only at the origin. Their asymptotic behavior is neither asymptotically flat nor (anti-) de Sitter. Similar solutions exist for certain Liouville-type potentials for the dilaton.
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References
How the literature uses it
24 arXiv papers cite this in 53 sentences
Papers citing it · 34 sentences without a confident label
Builds on it 3 papers
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Therefore, we should consider at least $M=N=3$ to be the simplest non-trivial solution to go beyond the cases already contained in [ref] and [ref] .
Charged dilaton black hole with multiple Liouville potentials and gauge fields · Derivation of the solution · 0.88
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For $≠0$, our solution [ref] is a generalisation of that of [ref] .
Higher-derivative scalar-vector-tensor theories: black holes, Galileons, singularity cloaking and holography · Spherical dilatonic black hole · 0.93
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Closely after the work of [ref] , these black hole solutions were generalised to horizons of toroidal and hyperbolic geometry by Cai et al. ( [ref] ), again for specific couplings.
Einstein-Maxwell-Dilaton theories with a Liouville potential · Introduction · 0.88
Uses its method or tool 4 papers
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In order to determine the mass we use the quasi-local mass formalism described in [ref] .
Five-Dimensional Black Hole String Backgrounds and Brane Universe Acceleration · Characteristics of the Black Hole Solutions. · 1.00
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Furthermore, putting the ansatz into the Maxwell equation Maxwell_Eq and dilaton equation dilaton_Eq give [equation] Taking the difference between EE1a and EE2a leads to [equation] To make progress towards obtaining a solution, we shall follow [ref] and consider a specific ansatz for $h$ as [equation] for some constant $n$.
Charged dilaton black hole with multiple Liouville potentials and gauge fields · Derivation of the solution · 0.99
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As shown in Ref. [ref] , the mass of the BH can be computed by following the quasilocal mass definition of Brown and York [ref] as
Quasinormal modes of charged dilaton black holes and their entropy spectra · CDBH and the separation of the massless Klein Gordon equation on it · 0.86
Compares with it 4 papers
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After a translation and some redefinitions of parameters the solution takes the form of [ref] , s^2 = -U(x)t^2 + x^2/U(x) +R^2(x)dΩ^2, U=β/R^2,
Einstein-Maxwell-Dilaton theories with a Liouville potential · Maximally symmetric solutions in 4-dimensional spacetime · 0.80
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Let us note that the string case with non-trivial dilaton potential escapes from the black hole backgrounds already found in Maxwell-Dilaton gravity [ref] .
Five-Dimensional Black Hole String Backgrounds and Brane Universe Acceleration · Black Hole Solutions · 0.92
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If we set all but one of them to zero, we recover the charged dilaton black hole with two exponential potentials originally obtained in Ref. [ref] .
Charged dilaton black hole with multiple Liouville potentials and gauge fields · Derivation of the solution · 0.81
Cites it as background 7 papers
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In 1995, CHM obtained the CDBH solution to the above action in their landmark paper [ref] .
Quasinormal modes of charged dilaton black holes and their entropy spectra · CDBH and the separation of the massless Klein Gordon equation on it · 0.93
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An Einstein gravity theory minimally coupled with a scalar field plus a Liouville potential has been well studied in the literature, and many exact solutions have been obtained [ref] .
Rotation curves and orbits in the scalar field dark matter halo spacetime · Introduction · 1.00
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Exact black hole solutions have been known for a long time both in Lovelock theory, [ref] - [ref] , and for two-derivative scalar-tensor theories, [ref] - [ref] .
Higher-derivative scalar-vector-tensor theories: black holes, Galileons, singularity cloaking and holography · Introduction · 0.95
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