2009
DOI: 10.1142/s0218271809015813
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Generating Static, Spherically Symmetric Black Holes in Lovelock Gravity

Abstract: Generalization of a known theorem to generate static, spherically symmetric black-hole solutions in higher dimensional Lovelock gravity is presented. Particular limits, such as Gauss-Bonnet (GB) and/or Einstein-Hilbert (EH) in any dimension N yield all the solutions known to date with an energy-momentum. In our generalization, with special emphasis on the third order Lovelock gravity, we have found two different class of solutions characterized by the matter field parameter.Several particular cases are studied… Show more

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Cited by 24 publications
(30 citation statements)
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“…[7] and the latter in Refs. [8][9][10]. The black hole solution in Einstein-Gauss-Bonnet theory in a string cloud model was considered in Refs.…”
Section: Introductionmentioning
confidence: 99%
“…[7] and the latter in Refs. [8][9][10]. The black hole solution in Einstein-Gauss-Bonnet theory in a string cloud model was considered in Refs.…”
Section: Introductionmentioning
confidence: 99%
“…The solution can be exactly verified through Ref. [14]. Since ω represents the mass it should be positive, ω ≥ 0.…”
Section: Spherically Symmetric Solution In Lovelock Gravitymentioning
confidence: 78%
“…Using Gauss-Bonnet gravity, static, spherically symmetric solutions were obtained later [11,12] with thermodynamic properties [13]. Static, spherically symmetric black hole solutions in Lovelock gravity with general energymomentum tensors in any arbitrary dimension can be found in [14] and [15][16][17][18][19][20][21][22] and its thermodynamics in [23]. Further extensive studies of Gauss-Bonnet black holes with a focus on the thermodynamic properties have been found in [24,25].…”
Section: Introductionmentioning
confidence: 99%
“…(63) do not belong to the Hilbert space H (we refer to the references; [46] for detailed mathematical analysis and [47][48][49][50][51][52][53][54][55][56][57][58][59][60] for applications of the HM approach in different spacetimes). This will be achieved by defining the function space on each t =constant hypersurface as H = { R| R < ∞} with the following norm given for the metric (2):…”
Section: Quantum Singularitiesmentioning
confidence: 99%