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Nariai, Bertotti-Robinson, and anti-Nariai solutions in higher dimensions
Open accessAbstract
We find all higher dimensional solutions of Einstein-Maxwell theory that are the topological product of two manifolds of constant curvature. These solutions include the higher dimensional Nariai, Bertotti-Robinson and anti-Nariai solutions and the anti--de Sitter Bertotti-Robinson solutions with toroidal and hyperbolic topology (Pleba\ifmmode \acute{n}\else \'{n}\fi{}ski-Hacyan solutions). We give explicit results for any dimension $D>~4.$ These solutions are generated from the appropriate extremal limits of the higher dimensional near-extreme black holes in de Sitter and anti--de Sitter backgrounds. Thus, we also find the mass and charge parameters of higher dimensional extreme black holes as a function of the radius of the degenerate horizon.
Overview
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TL;DR
The paper constructs all higher-dimensional Einstein-Maxwell solutions that are topological products of two constant-curvature manifolds, including Nariai, Bertotti-Robinson, anti-Nariai, and Plebański-Hacyan solutions for any \(D \ge 4\). These are generated as extremal limits of near-extreme higher-dimensional de Sitter and anti-de Sitter black holes.
Key findings
- The higher-dimensional Nariai solution is the product \(dS_2 \times S^{D-2}\), with fixed \((D-2)\)-sphere radius \(B^{-1/2}\); the Bertotti-Robinson solution is \(AdS_2 \times S^{D-2}\), and the flat Bertotti-Robinson is its \(\Lambda=0\) limit.
- The Nariai-Bertotti-Robinson solution is \(M^{1,1} \times S^{D-2}\), with \(M^{1,1}\) two-dimensional Minkowski spacetime in Rindler coordinates, and is identified as a Plebański-Hacyan solution.
- In the AdS case, the solutions include spherical \(AdS_2 \times S^{D-2}\), toroidal/cylindrical/planar \(AdS_2 \times E^{D-2}\), and anti-Nariai \(AdS_2 \times H^{D-2}\); only the \(k=-1\) anti-Nariai case admits a neutral \(Q=0\) solution.
- For extreme dS black holes, the mass and charge parameters as functions of the degenerate horizon \(\rho\) are \(M = 2\rho^{D-3}\left(1 - \frac{D-2}{D-3}\frac{\Lambda}{3}\rho^2\right)\) and \(Q^2 = \rho^{2(D-3)}\left(1 - \frac{D-1}{D-3}\frac{\Lambda}{3}\rho^2\right)\), with \(\rho_{\max} = \sqrt{\frac{D-3}{D-1}\frac{3}{\Lambda}}\). For extreme AdS black holes, \(M = 2\rho^{D-3}\left(k - \frac{D-2}{D-3}\frac{\Lambda}{3}\rho^2\right)\) and \(Q^2 = \rho^{2(D-3)}\left(k - \frac{D-1}{D-3}\frac{\Lambda}{3}\rho^2\right)\).
Methods
- Theoretical study of the \(D\)-dimensional Einstein-Maxwell action with cosmological constant \(\Lambda\), using static higher-dimensional Tangherlini black-hole metrics in asymptotically dS and AdS backgrounds.
- The authors apply the Ginsparg-Perry near-extremal limiting procedure: set horizons to differ by a small parameter \(\varepsilon\), introduce new time and radial coordinates, and take \(\varepsilon \to 0\) to generate Nariai-like, Bertotti-Robinson-like, and anti-Nariai-like solutions.
- They derive explicit mass and charge parameters for extreme black holes as functions of the degenerate horizon \(\rho\), then identify the resulting product spacetimes and their topology for \(k=1,0,-1\).
Limitations
- The paper states that for \(D \ge 6\) it was not able to write \(f(r)\) as a function of the degenerate horizon \(\rho\), because one must deal with polynomial functions of degree higher than four.
- The text makes evident that stability analyses, including quasinormal modes and quantum stability, are left for future work; the paper focuses on constructing the exact solutions and their extremal black-hole parameters.
- The construction is limited to solutions generated from extremal limits of near-extreme static black holes; the paper does not present empirical data or observational tests.
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“Thus, besides the degenerate horizon r = ρ, there is another horizon at σ = 3/Λ -2ρ 2 .”
§ Nariai, Bertotti-Robinson and anti-Nariai solutions in higher dimensions > A. Higher dimensional extreme black holes in an asymptotically dS background
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“There is no neutral (Q = 0) Bertotti-Robinson solution.”
§ Nariai, Bertotti-Robinson and anti-Nariai solutions in higher dimensions > 2. Higher dimensional dS Bertotti-Robinson solution
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In the paper
“F = - Q ADM ρ D-2 u dt ∧ dx , (29”
§ Nariai, Bertotti-Robinson and anti-Nariai solutions in higher dimensions > 3. Higher dimensional Nariai-Bertotti-Robinson solution
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In the paper
“The condition Q 2 ≥ 0 implies that ρ ≤ 3/(2Λ).”
§ Nariai, Bertotti-Robinson and anti-Nariai solutions in higher dimensions > A. Higher dimensional extreme black holes in an asymptotically dS background
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In the paper
“Now, the above construction can be extended to Ddimensional extreme dS black holes.”
§ Nariai, Bertotti-Robinson and anti-Nariai solutions in higher dimensions > A. Higher dimensional extreme black holes in an asymptotically dS background
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In the paper
§ Nariai, Bertotti-Robinson and anti-Nariai solutions in higher dimensions > 3. Higher dimensional Nariai-Bertotti-Robinson solution
“F = - Q ADM ρ D-2 u dt ∧ dx , (29”
§ Nariai, Bertotti-Robinson and anti-Nariai solutions in higher dimensions > 3. Higher dimensional Nariai-Bertotti-Robinson solution
“the Maxwell field (9) of the higher dimensional Nariai-Bertotti-Robinson solution is F = Q ADM ρ -D+2 u χ dT ∧ dχ.Now, the spacetime factor -χ 2 dT 2 + dχ 2 is just M 1,1 (2-dimensional Minkowski spacetime) in Rindler coordinates.Therefore, under the usual coordinate transformation χ = √ x 2 -t 2 and T = arctanh(t/x)”
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In the paper
§ Nariai, Bertotti-Robinson and anti-Nariai solutions in higher dimensions > 3. Higher dimensional AdS black holes with hyperbolic topology
“One has mmin = -4 D-1 ( D-3 D-2 ) (D-3)/2 , and q0 = ( D-3 D-2 ) (D-3)/2 / √ D -2.”
§ Nariai, Bertotti-Robinson and anti-Nariai solutions in higher dimensions > 3. Higher dimensional AdS black holes with hyperbolic topology
“ρ min = - D -3 D -1 3 Λ .(35) For ρ = ρ min , the extreme black hole has no electric charge (Q = 0) and its mass is negative, M = -4ρ D-3 min /(D -1).”
Citations
Cites
The hierarchy problem and new dimensions at a millimeter
Arkani–Hamed, N., Dimopoulos, S., & Dvali, G. (1998) · Physics Letters B · doi:10.1016/s0370-2693(98)00466-3 · Cited by 6,563
New dimensions at a millimeter to a fermi and superstrings at a TeV
Antoniadis, I., Arkani-Hamed, N., Dimopoulos, S., & Dvali, G. (1998) · Physics Letters B · doi:10.1016/s0370-2693(98)00860-0 · Cited by 3,915
Cosmological event horizons, thermodynamics, and particle creation
Gibbons, G. W., & Hawking, S. W. (1977) · Physical Review D · doi:10.1103/physrevd.15.2738 · Cited by 3,192
Nima Arkani-hamed, A., Dimopoulos, S., & Dvali, G. (1999) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.59.086004 · Cited by 2,396
Black holes in higher dimensional space-times
Myers, R. C., & Perry, M. J. (1986) · Annals of Physics · doi:10.1016/0003-4916(86)90186-7 · Cited by 2,125
Black Holes at the Large Hadron Collider
Dimopoulos, S., & Landsberg, G. (2001) · Physical Review Letters · doi:10.1103/physrevlett.87.161602 · Cited by 1,096
Charged AdS black holes and catastrophic holography
Chamblin, A., Emparan, R., Johnson, C. V., & Myers, R. C. (1999) · Physical Review D · doi:10.1103/physrevd.60.064018 · Cited by 1,016
Schwarzschild field inn dimensions and the dimensionality of space problem
Tangherlini, F. R. (1963) · Il Nuovo Cimento · doi:10.1007/bf02784569 · Cited by 1,003
Holography, thermodynamics, and fluctuations of charged AdS black holes
Andrew Chamblin, A., Emparan, R., Johnson, C. V., & Myers, R. C. (1999) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.60.104026 · Cited by 955
Topological black holes in anti-de Sitter space
Birmingham, D. (1999) · Classical and Quantum Gravity · doi:10.1088/0264-9381/16/4/009 · Cited by 533
Three dimensional black holes and cylindrical general relativity
Lemos, J. P. S. (1995) · Physics Letters B · doi:10.1016/0370-2693(95)00533-q · Cited by 493
Self-citationBlack holes and sub-millimeter dimensions
Argyres, P. C., Dimopoulos, S., & March-Russell, J. (1998) · Physics Letters B · doi:10.1016/s0370-2693(98)01184-8 · Cited by 489
Supersymmetric, cold and lukewarm black holes in cosmological Einstein-Maxwell theory
Romans, L. J. (1992) · Nuclear Physics B · doi:10.1016/0550-3213(92)90684-4 · Cited by 471
Uniform Electromagnetic Field in the Theory of General Relativity
Bertotti, B. (1959) · Physical Review · doi:10.1103/physrev.116.1331 · Cited by 411
Black holes with unusual topology
Vanzo, L. (1997) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.56.6475 · Cited by 391
Kodama, H., & Ishibashi, A. (2004) · Progress of Theoretical Physics · doi:10.1143/ptp.111.29 · Cited by 386
Thermodynamics of ( 3 + 1 ) -dimensional black holes with toroidal or higher genus horizons
Brill, D. R., Louko, J., & Peldán, P. (1997) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.56.3600 · Cited by 340
Rotating charged black strings and three-dimensional black holes
Lemos, J. P. S., & Zanchin, V. T. (1996) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.54.3840 · Cited by 312
Self-citationDuality between electric and magnetic black holes
Hawking, S. W., & Ross, S. F. (1995) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.52.5865 · Cited by 308
Semiclassical perdurance of de Sitter space
Ginsparg, P., & Perry, M. J. (1983) · Nuclear Physics B · doi:10.1016/0550-3213(83)90636-3 · Cited by 301
Instability of ultra-spinning black holes
Emparan, R., & Myers, R. C. (2003) · Journal of High Energy Physics · doi:10.1088/1126-6708/2003/09/025 · Cited by 277
Topological black holes in the dimensionally continued gravity
Cai, R.-G., & Soh, K. (1999) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.59.044013 · Cited by 251
Making anti-de Sitter black holes
Åminneborg, S., Bengtsson, I., Holst, S., & Peldán, P. (1996) · Classical and Quantum Gravity · doi:10.1088/0264-9381/13/10/010 · Cited by 212
Gravitational radiation in D -dimensional spacetimes
Cardoso, V., Dias, Ó. J. C., & Lemos, J. P. S. (2003) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.67.064026 · Cited by 209
Self-citationNojiri, S., ODINTSOV, S. D., & OGUSHI, S. (2002) · International Journal of Modern Physics A · doi:10.1142/s0217751x02012156 · Cited by 206
Cosmological and black hole brane-world universes in higher derivative gravity
Nojiri, S., Odintsov, S. D., & Ogushi, S. (2001) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.65.023521 · Cited by 204
Two-dimensional black holes and planar general relativity
Lemos, J. P. S. (1995) · Classical and Quantum Gravity · doi:10.1088/0264-9381/12/4/014 · Cited by 195
Self-citationCosmological production of charged black hole pairs
Mann, R. B., & Ross, S. F. (1995) · Physical Review D · doi:10.1103/physrevd.52.2254 · Cited by 194
Higher-dimensional black holes in compactified space-times
Myers, R. C. (1987) · Physical Review D · doi:10.1103/physrevd.35.455 · Cited by 185
Adventures in de Sitter spacePreprint
Raphael Bousso, A. (2002) · arXiv (Cornell University) · doi:10.48550/arxiv.hep-th/0205177 · Cited by 144
Rotating topological black holes
Klemm, D. S., Moretti, V., & Vanzo, L. (1998) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.57.6127 · Cited by 138
Mann, R. (1997) · Classical and Quantum Gravity · doi:10.1088/0264-9381/14/10/018 · Cited by 120
A Solution of the Maxwell-Einstein Equations
Robinson, I. (1959) · Cited by 108
Quantum cosmology, inflationary brane-world creation and dS/CFT correspondence
Nojiri, S., & Odintsov, S. D. (2001) · Journal of High Energy Physics · doi:10.1088/1126-6708/2001/12/033 · Cited by 95
Higher-dimensional charged rotating solutions in (A)dS spacetimes
Awad, A. (2003) · Classical and Quantum Gravity · doi:10.1088/0264-9381/20/13/327 · Cited by 95
Black Holes of Negative MassPreprint
Mann, R. (1997) · Cited by 81
Quantum evolution of Schwarzschild–de Sitter (Nariai) black holes
Nojiri, S., & Odintsov, S. D. (1999) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.59.044026 · Cited by 79
Effects of a nonvanishing cosmological constant on the spherically symmetric vacuum manifold
Lake, K., & Roeder, R. C. (1977) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.15.3513 · Cited by 68
Black holes and causal structure in anti-de Sitter isometric spacetimes
Holst, S., & Peldán, P. (1997) · Classical and Quantum Gravity · doi:10.1088/0264-9381/14/12/025 · Cited by 66
Late-time tails of wave propagation in higher dimensional spacetimes
Cardoso, V., Yoshida, S., Dias, Ó. J. C., & Lemos, J. P. S. (2003) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.68.061503 · Cited by 63
Self-citationExplicit Kundt type II and N solutions as gravitational waves in various type D and O universes
Podolsk, J., & Ortaggio, M. (2003) · Classical and Quantum Gravity · doi:10.1088/0264-9381/20/9/307 · Cited by 61
Higher Dimensional Charged Rotating Solutions in (A)dS Space-timesPreprint
Awad, A. (2002) · Cited by 60
Proliferation of de Sitter space
Raphael Bousso, A. (1998) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.58.083511 · Cited by 59
Lorentzian 4 dimensional manifolds with “local isotropy”
Cahen, M., & Defrise, L. (1968) · Communications in Mathematical Physics · doi:10.1007/bf01654301 · Cited by 59
EFFECTIVE ACTION FOR CONFORMAL SCALARS AND ANTIEVAPORATION OF BLACK HOLES
Nojiri, S., & Odintsov, S. D. (1999) · International Journal of Modern Physics A · doi:10.1142/s0217751x9900066x · Cited by 55
Some exceptional electrovac type D metrics with cosmological constant
Plebański, J. F., & Hacyan, S. (1979) · Journal of Mathematical Physics · doi:10.1063/1.524174 · Cited by 52
Magnetic strings in anti-de Sitter general relativity
Dias, Ó. J. C., & Lemos, J. P. S. (2002) · Classical and Quantum Gravity · doi:10.1088/0264-9381/19/8/314 · Cited by 51
Self-citationBlack holes in three-dimensional dilaton gravity theories
Sá, P. M., Kleber, A., & Lemos, J. P. S. (1996) · Classical and Quantum Gravity · doi:10.1088/0264-9381/13/1/011 · Cited by 50
Self-citationStationary Einstein-Maxwell fields in arbitrary dimensions
Ida, D., & Uchida, Y. (2003) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.68.104014 · Cited by 45
Rotating topological black branes in various dimensions and AdS/CFT correspondence
Dehghani, M. H. (2002) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.65.124002 · Cited by 39
The Riemannian and Affine Differential Geometry of Product-Spaces
Ficken, F. A. (1939) · Annals of Mathematics · doi:10.2307/1968900 · Cited by 35
Barvinsky, A. O., & Solodukhin, S. N. (2003) · Nuclear Physics B · doi:10.1016/j.nuclphysb.2003.10.011 · Cited by 33
Impulsive waves in electrovac direct product spacetimes with
Ortaggio, M., & Podolsk, J. (2002) · Classical and Quantum Gravity · doi:10.1088/0264-9381/19/20/313 · Cited by 31
Impulsive waves in the Nariai universe
Ortaggio, M. (2002) · Physical Review D · doi:10.1103/physrevd.65.084046 · Cited by 29
Kerr–de Sitter spacetimes in various dimensions and dS/CFT correspondence
Dehghani, M. (2002) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.65.104003 · Cited by 27
Horizonless rotating solutions in (n+1)-dimensional Einstein-Maxwell gravity
Dehghani, M. H. (2004) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.69.044024 · Cited by 26
Dias, Ó. J. C., & Lemos, J. P. S. (2001) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.64.064001 · Cited by 26
Self-citationStationary black holes in a generalized three-dimensional theory of gravity
Sá, P. M., & Lemos, J. P. S. (1998) · Physics Letters B · doi:10.1016/s0370-2693(98)00084-7 · Cited by 24
Self-citationMagnetic point sources in three-dimensional Brans-Dicke gravity theories
Dias, Ó. J. C., & Lemos, J. P. S. (2002) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.66.024034 · Cited by 24
Self-citationOn product spacetime with 2-sphere of constant curvaturePreprint
DADHICH, N. K. (2000) · arXiv (Cornell University) · doi:10.48550/arxiv.gr-qc/0003026 · Cited by 22
Multi-Black-Holes in 3D and 4D anti-de Sitter SpacetimesPreprint
Brill, D. R. (1996) · arXiv (Cornell University) · doi:10.48550/arxiv.gr-qc/9608010 · Cited by 22
The extremal limit of D-dimensional black holesPreprint
Caldarelli, M., Vanzo, L., & Zerbini, S. (2000) · CERN Document Server (European Organization for Nuclear Research) · doi:10.48550/arxiv.hep-th/0008136 · Cited by 16
THE EXTREMAL LIMIT OF D -DIMENSIONAL BLACK HOLES
Caldarelli, M. M., VANZO, L., & Zerbini, S. (2001) · doi:10.1142/9789812810366_0005 · Cited by 12
Research works printed but not linked: 6
- J.L. Feng, 2002, Phys. Rev. Lett., 021303
- D.R. Brill, 1996, Helv. Phys. Acta, 69, 249
- H. Nariai, 1950, Sci. Rep. Tohoku Univ., Ser. 1, 34, 160
- H. Nariai, 1951, Sci. Rep. Tohoku Univ., Ser. 1, 35, 62
- I. Robinson, 1959, Bull. Acad. Pol. Sci., Ser. Sci., Math., Astron. Phys., 7, 351
- O.J.C. Dias, 2003, Phys. Rev. D, 68, 061503, 10.1103/physrevd.68.061503 · DOI
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Self-citationGarraffo, C., & Giribet, G. E. (2008) · Modern Physics Letters A · doi:10.1142/s0217732308027497 · Cited by 213
Lovelock black holes with a nonlinear Maxwell field
Maeda, H., Hassaïne, M., & Martínez, C. (2009) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.79.044012 · Cited by 176
Static response and Love numbers of Schwarzschild black holes
Hui, L., Joyce, A., Penco, R., Santoni, L., & Solomon, A. R. (2021) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2021/04/052 · Cited by 165
Classification of the Weyl tensor in higher dimensions and applications
Coley, A. A. (2008) · Classical and Quantum Gravity · doi:10.1088/0264-9381/25/3/033001 · Cited by 129
Metadata
- Authors
- Cardoso, V., Dias, Ó. J. C., & Lemos, J. P. S.
- Affiliations
- Instituto Superior Técnico (PT)
- Venue
- Physical Review D
- Publisher
- American Physical Society (APS)
- Published
- 2004-07-19
- Volume
- 70
- Issue
- 2
- ISSN
- 0556-2821 (ISSN-L)
- 1550-7998
- 1550-2368
- OpenAlex
- W1996802537
- Semantic Scholar
- a7883655b8fbb542977a5e8a20f7de99bd5b7895
- Cited by
- 107
- References
- 63
- Citations by year
- 2026: 3 · 2025: 2 · 2024: 8 · 2023: 4 · 2022: 3 · 2021: 2 · 2020: 4 · 2019: 2 · 2018: 5 · 2017: 2 · 2016: 4 · 2015: 2 · 2014: 2 · 2013: 4 · 2012: 6
- FWCI
- 3.85
- Type
- journal article
- Language
- en
- Open access
- green
- arxiv.org
- Locations
- Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields (publishedVersion)
- arXiv (Cornell University) (acceptedVersion)
- CERN Document Server (European Organization for Nuclear Research) (submittedVersion)
- ePrints Soton (University of Southampton) (submittedVersion)
- arXiv (Cornell University)
- Funders
- CERN
- Fundação para a Ciência e a Tecnologia
- Topics
- Physical Sciences › Physics and Astronomy › Nuclear and High Energy Physics › Black Holes and Theoretical Physics
- Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Relativity and Gravitational Theory
- Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Cosmology and Gravitation Theories
- Keywords
- Einstein-Maxwell theory, higher-dimensional black holes, extremal black holes, de Sitter space, anti-de Sitter space, constant curvature manifolds, degenerate horizons
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Bibliographic data: Semantic Scholar, OpenAlex, Crossref.
Contains information from the Semantic Scholar Academic Graph Datasets, made available under the ODC Attribution License (ODC-BY 1.0).
Semantic Scholar’s data is described in: Kinney, R., et al. (2023). The Semantic Scholar Open Data Platform. arXiv:2301.10140.