RECORD
On Holographic description of the Kerr-Newman-AdS-dS black holes
High Energy Physics - Theory · Submitted 1 Jun 2010
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Similar to the Kerr case, this suggests that the Kerr-Newman-AdS-dS black hole is dual to a two-dimensional CFT with central charges $c_L=c_R=\frac{6a(r_++r_\ast)}{k}$ and temperatures $T_L=\frac{k(r_+^2+r_\ast^2+2a^2)}{4\pi a\Xi(r_++r_\ast)}, T_R=\frac{k(r_+-r_\ast)}{4\pi a\Xi}$.
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.
Open the compiled record
The abstract, sentence by sentence
In this paper, we study the holographic description of the generic four-dimensional non-extremal Kerr-Newman-AdS-dS black holes. We find that if focusing on the near-horizon region, for the massless scalar scattering in the low-frequency limit, there exists hidden conformal symmetry on the solution space. Similar to the Kerr case, this suggests that the Kerr-Newman-AdS-dS black hole is dual to a two-dimensional CFT with central charges $c_L=c_R=\frac{6a(r_++r_\ast)}{k}$ and temperatures $T_L=\frac{k(r_+^2+r_\ast^2+2a^2)}{4\pi a\Xi(r_++r_\ast)}, T_R=\frac{k(r_+-r_\ast)}{4\pi a\Xi}$. The macroscopic Bekenstein-Hawking entropy could be recovered from the microscopic counting in dual CFT via the Cardy formula. Using the Minkowski prescription, we compute the real-time correlators of the scalar, photon and graviton in near horizon geometry of near extremal Kerr-AdS-dS black hole. In all these cases, the retarded Green's function and the corresponding absorption cross section are in perfect match with CFT prediction. We further discuss the low-frequency scattering of a charged scalar by a Kerr-Newman-AdS-dS black hole and find the dual CFT description.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | In this paper, we study the holographic description of the generic four-dimensional non-extremal Kerr-Newman-AdS-dS black holes. | contribution 0.93 | 0.82 | 0.04 | asserted 0.70 |
| s1 | We find that if focusing on the near-horizon region, for the massless scalar scattering in the low-frequency limit, there exists hidden conformal symmetry on the solution space. | result 1.00 | 0.95 | 0.24 | asserted 1.00 |
| s2 | Similar to the Kerr case, this suggests that the Kerr-Newman-AdS-dS black hole is dual to a two-dimensional CFT with central charges $c_L=c_R=\frac{6a(r_++r_\ast)}{k}$ and temperatures $T_L=\frac{k(r_+^2+r_\ast^2+2a^2)}{4\pi a\Xi(r_++r_\ast)}, T_R=\frac{k(r_+-r_\ast)}{4\pi a\Xi}$. | interpretation 0.57 | 0.87 | 0.46 | hedged possibility 0.97 |
| s3 | The macroscopic Bekenstein-Hawking entropy could be recovered from the microscopic counting in dual CFT via the Cardy formula. | result 0.89 | 0.71 | 0.23 | hedged possibility 0.98 |
| s4 | Using the Minkowski prescription, we compute the real-time correlators of the scalar, photon and graviton in near horizon geometry of near extremal Kerr-AdS-dS black hole. | method 0.68 | 0.95 | 0.06 | asserted 1.00 |
| s5 | In all these cases, the retarded Green's function and the corresponding absorption cross section are in perfect match with CFT prediction. | result 1.00 | 0.90 | 0.18 | asserted 1.00 |
| s6 | We further discuss the low-frequency scattering of a charged scalar by a Kerr-Newman-AdS-dS black hole and find the dual CFT description. | contribution 0.86 | 0.96 | 0.12 | asserted 1.00 |
What was examined, and what was not
- arXiv listing abstract v3
- full text
- figures and tables
- references and citing sentences
- relations to other papers
- P abstract
- S sections
- T body sentences
- C citations
- R cross-paper relations
The paper
Original abstract
In this paper, we study the holographic description of the generic four-dimensional non-extremal Kerr-Newman-AdS-dS black holes. We find that if focusing on the near-horizon region, for the massless scalar scattering in the low-frequency limit, there exists hidden conformal symmetry on the solution space. Similar to the Kerr case, this suggests that the Kerr-Newman-AdS-dS black hole is dual to a two-dimensional CFT with central charges $c_L=c_R=\frac{6a(r_++r_\ast)}{k}$ and temperatures $T_L=\frac{k(r_+^2+r_\ast^2+2a^2)}{4\pi a\Xi(r_++r_\ast)}, T_R=\frac{k(r_+-r_\ast)}{4\pi a\Xi}$. The macroscopic Bekenstein-Hawking entropy could be recovered from the microscopic counting in dual CFT via the Cardy formula. Using the Minkowski prescription, we compute the real-time correlators of the scalar, photon and graviton in near horizon geometry of near extremal Kerr-AdS-dS black hole. In all these cases, the retarded Green's function and the corresponding absorption cross section are in perfect match with CFT prediction. We further discuss the low-frequency scattering of a charged scalar by a Kerr-Newman-AdS-dS black hole and find the dual CFT description.
Human review
References
How the literature uses it
22 arXiv papers cite this in 42 sentences
Papers citing it · 22 sentences without a confident label
Builds on it 2 papers
-
We showed that, besides the angular momentum $J$-picture (associated with the Kerr/CFT duality, where the central charges of the dual 2D CFT are $c_L = c_R = 12J$) revealed in [ref] , another $Q$-picture (associated with the RN/CFT duality, in which the central charges are $c_L = c_R = 6Q^3/ℓ$, where $ℓ$ is the parameter depends on the embedding) does exist for the general nonextremal KN black hole by probing the 2D hidden conformal symmetries via an external charged scalar field [ref] .
The Kerr-Newman/CFTs Correspondence · Introduction · 0.81
-
For the near-extremal case, [ref] initiated some progress and we extend those results here by computing the entropies of near-extremal AdS$_4$ black holes via the Cardy formula.
Universal Entropy and Hawking Radiation of Near-Extremal AdS$_4$ Black Holes · Near-Extremal AdS$_4$ Black Hole Entropy from Cardy Formula · 0.99
Uses its method or tool 3 papers
-
Based on hidden conformal symmetry [ref] , the right temperature is T_R = k (r_+ - r_s)/4 πa Ξ .
Universal Entropy and Hawking Radiation of Near-Extremal AdS$_4$ Black Holes · Near-Extremal AdS$_4$ Black Hole Entropy from Cardy Formula · 0.92
-
Similar to the treatment in [ref] , we need to focus on the near-horizon region.
Holographic Q-picture of Kerr-Newman-AdS-dS Black Hole · Introduction · 0.94
-
Similar with the analysis in [ref] , we focus on the near-horizon region, where \(r-r_+\) is a small quantity, so we can series \(f_r^KNA Δ\) to the quadratic order, [equation] where \(r_+\) always stands for outer horizon, and [equation]
Hidden Conformal Symmetry for Vector Field on Various Black Hole Backgrounds · Low frequency limit at Near-Horizon region · 0.91
Compares with it 2 papers
-
From ([ref]) and ([ref]), we obtain the central charge and the temperature directly c_L^J=6k(r_+^2+a^2)Ξ=12r_+(1-r_+^2/ℓ^2)(r_+^2+3r_+^4/ℓ^2-q^2) 1+6r_+^2/ℓ^2-3r_+^4/ℓ^4-q^2/ℓ^2, T_L^J=12πk T_L=(1+6r_+^2/ℓ^2-3r_+^4/ℓ^4-q^2/ℓ^2)(2r_+^2+2r_+^4/ℓ^2-q^2) 4πr_+(1-2r_+^2/ℓ^2-3r_+^4/ℓ^2+q^2/ℓ^2) (1-r_+^2/ℓ^2)(r_+^2+3r_+^4/ℓ^2-q^2),which are in perfect match with the result in [ref] .
Novel CFT Duals for Extreme Black Holes · J-picture · 0.97
-
It should be noted that, unlike the case of higher dimensional black holes [ref] , where the near-region limit for the radial wave equation is taken into account, in the present case, no extra approximation is needed to match the wave equation of scalar field with the Casimir operator.
Hidden Conformal Symmetry of Self-Dual Warped AdS_3 Black Holes in Topological Massive Gravity · SL(2, R)$_L×$SL(2, R)$_R$ · 0.86
Cites it as support 1 paper
-
We expect that a general scattering theory around any near-extremal black hole solution of [ref] will also be consistent with a CFT description, as supported by all cases studied beyond the Kerr-Newman black hole [ref] .
The Kerr/CFT correspondence and its extensions: a comprehensive review · Microscopic greybody factors · 0.97
Cites it as background 10 papers
-
The most notable such example is by far the Kerr/$CFT$ correspondence and its extensions [ref] , where the general idea is that the asymptotic symmetry group (ASG), preserving certain metric boundary or fall off conditions, is generated by a Virasoro algebra with calculable central extension: [equation] The Bekenstein-Hawking entropy is then obtained from Cardy's Formula [ref] in terms of $c$ and the proper normalized lowest eigen-mode via: [equation] In the Kerr/$CFT$ case a thermal Cardy Formula is employed [equation] which depends on the left Frolov-Thorne vacuum temperature $T_L$ for generic Kerr geometry [ref] .
Near-Extremal Kerr AdS2xS2 Solution and Black-Hole/Near-Horizion-CFT Duality · Holographic Black Hole Entropy · 0.88
-
This concept is most notably exemplified by the $Kerr/CFT$ correspondence [ref] and its extensions [ref] .
Near-Extremal Black Hole Thermodynamics from AdS2/CFT1 Correspondence in The Low Energy Limit of 4D Heterotic String Theory · Introduction · 0.91
-
Following the introduction of the thermodynamic volume [ref] studies of the equation of state and phase transitions of AdS black holes have proceeded in a manner similiar from classical thermodynamics, for example by plotting isotherms on $P-V$ diagrams and utilizing the Gibbs free energy [ref] .
Cosmography of KNdS Black Holes and Isentropic Phase Transitions · Properties of Kerr-Newman deSitter black holes · 0.80
Discussion
Know something about this paper? Leave a comment, or highlight any passage above to comment on it.