1988
DOI: 10.1007/bf01217967
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4-Dimensional black holes from Kaluza-Klein theories

Abstract: In this paper we consider generalizations in 4 dimensions of the Einstein-Maxwell equations which typically arise from Kaluza-Klein theories. We specify conditions such that stationary solutions lead to non-linear σ-models for symmetric spaces. Using both this group theoretic structure and some properties of harmonic maps we are able to generalize many of the known existence and uniqueness theorems for black holes in Einstein-Maxwell theory to this more general setting.

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Cited by 426 publications
(993 citation statements)
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“…The technique of studying stationary configurations of 4D supergravities by dimensionally reducing the 4D theories to 3D non-linear σ-models coupled to gravity was described in the pioneering work [24]. The 3D moduli space for 4D N = 2 supergravity coupled to n V vector-multiplets is well-studied, for example in [25,26,27,28].…”
Section: D Moduli Space M 3dmentioning
confidence: 99%
“…The technique of studying stationary configurations of 4D supergravities by dimensionally reducing the 4D theories to 3D non-linear σ-models coupled to gravity was described in the pioneering work [24]. The 3D moduli space for 4D N = 2 supergravity coupled to n V vector-multiplets is well-studied, for example in [25,26,27,28].…”
Section: D Moduli Space M 3dmentioning
confidence: 99%
“…Although the numerator group G for a timelike reduction is the same as that obtained in a spacelike reduction, the divisor group H * for a timelike reduction is a noncompact form of the spacelike divisor group H [2]. A consequence of this H → H * change and the dualization of vectors is the appearance of negative-sign kinetic terms for some 3D scalars.…”
mentioning
confidence: 99%
“…The search for supergravity solutions with assumed Killing symmetries can be recast as a Kaluza-Klein problem [1,2,3]. To see this, consider a 4D theory with a nonlinear bosonic symmetry G 4 (e.g.…”
Section: Introductionmentioning
confidence: 99%
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