2006
DOI: 10.1016/j.physletb.2006.06.024
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Rotating Einstein–Maxwell–dilaton black holes in D dimensions

Abstract: We construct exact charged rotating black holes in Einstein-Maxwell-dilaton theory in D spacetime dimensions, D ≥ 5, by embedding the D dimensional Myers-Perry solutions in D + 1 dimensions, and performing a boost with a subsequent Kaluza-Klein reduction. Like the Myers-Perry solutions, these black holes generically possess N = [(D − 1)/2] independent angular momenta. We present the global and horizon properties of these black holes, and discuss their domains of existence.

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Cited by 61 publications
(94 citation statements)
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“…Attempts have been made to find similar solutions to the Einstein-Maxwell equations analytically (Aliev, 2006a(Aliev, ,b, 2007Aliev and Frolov, 2004;Chen and Lü, 2008;Kunz et al, 2006a) or numerically (Brihaye and Delsate, 2007;Kleihaus et al, 2008;Kunz et al, 2005Kunz et al, , 2007Kunz et al, , 2006b.…”
Section: Black Holes In Higher Dimensionsmentioning
confidence: 99%
“…Attempts have been made to find similar solutions to the Einstein-Maxwell equations analytically (Aliev, 2006a(Aliev, ,b, 2007Aliev and Frolov, 2004;Chen and Lü, 2008;Kunz et al, 2006a) or numerically (Brihaye and Delsate, 2007;Kleihaus et al, 2008;Kunz et al, 2005Kunz et al, , 2007Kunz et al, , 2006b.…”
Section: Black Holes In Higher Dimensionsmentioning
confidence: 99%
“…In spheroidal coordinates (r, θ) the asymptotic expansion (r → ∞) of the metric functions yields ( [24], [34])…”
Section: Generating Charged Dilatonic Black Objectsmentioning
confidence: 99%
“…In the case of Kaluza-Klein coupling the solutions can be obtained by adding a spatial dimension and performing a boost. A dimensional reduction then leads to the charged dilatonic black hole solutions (compare [14] - [24]). …”
Section: Introductionmentioning
confidence: 99%
“…This mass formula holds also in the presence of a dilaton field [9]. Introducing the dilaton charge into the mass formula via [9] …”
Section: Mass Formulamentioning
confidence: 82%