Bps Black Holes in Gauged N=4, D=4 Supergravity Typeset Using Revt E X 2
نویسنده
چکیده
We find solutions of the bosonic sector of gauged N=4, D=4 SU(2) × SU(2) supergravity, which represent dilaton black holes with toroidal or spherical event horizons. The axion is consistently truncated, and the gauge group is broken to U(1) × U(1). The spherical black holes carry two electric and two magnetic abelian charges, whereas the toroidal holes have vanishing magnetic charges. The spacetime metrics are warped products, and the manifolds turn out to be globally hyperbolic, in contrast to standard gauged supergravity ground states. It is shown that in the toroidal case, there are solutions preserving one quarter or one half of the supersymmetries, while for spherical topologies all supersymmetries are broken. In general, the toroidal BPS states represent naked singularities, but there is also a supersymmetric black hole with vanishing Hawking temperature. The 1/2 supersymmetric case arises for vanishing charges and mass, and represents the known domain wall solution of the Freedman-Schwarz model. It provides the background in which the black holes live. Finally, we use Chamseddine’s and Volkov’s Kaluza-Klein interpretation of gauged N=4, D=4 SU(2) × SU(2) supergravity to lift our solutions to ten and eleven dimensions and to consider them as solutions to email: [email protected]
منابع مشابه
ar X iv : h ep - t h / 98 10 09 0 v 1 1 3 O ct 1 99 8 UTF 423 BPS Black Holes in Gauged N = 4 , D = 4 Supergravity
We find solutions of the bosonic sector of gauged N=4, D=4 SU(2)×SU(2) supergravity, which represent dilaton black holes with toroidal or spherical event horizons. The axion is consistently truncated, and the gauge group is broken to U(1)×U(1). The spherical black holes carry two electric and two magnetic abelian charges, whereas the toroidal holes have vanishing magnetic charges. The spacetime...
متن کامل0 v 3 1 9 Ja n 19 99 UTF 423 BPS
We find solutions of the bosonic sector of gauged N=4, D=4 SU(2) × SU(2) supergravity, which represent dilaton black holes with toroidal or spherical event horizons. The axion is consistently truncated, and the gauge group is broken to U(1) × U(1). The spherical black holes carry two electric and two magnetic abelian charges, whereas the toroidal holes have vanishing magnetic charges. The space...
متن کاملNon-Extreme Black Holes of Five Dimensional N=2 AdS Supergravity
We derive and analyse the full set of equations of motion for non-extreme static black holes (including examples with the spatial curvatures k = −1 and k = 0) in D=5 N=2 gauged supergravity by employing the techniques of “very special geometry”. These solutions turn out to differ from those in the ungauged supergravity only in the non-extremality function, which has an additional term (proporti...
متن کاملBranes on the Brane
We show that four-dimensional N = 2 ungauged Einstein-Maxwell supergravity can be embedded on the Randall-Sundrum 3-brane, as a consistent Kaluza-Klein reduction of five-dimensional N = 4 gauged supergravity. In particular, this allows us to describe four-dimensional Reissner-Nordström black holes within the Randall-Sundrum scenario. Using earlier results on the embedding of five-dimensional N ...
متن کاملBps Black Holes in N = 2 Five Dimensional Ads Supergravity
BPS black hole solutions of U(1) gauged five-dimensional supergravity are obtained by solving the Killing spinor equations. These extremal static black holes live in an asymptotic AdS5 space time. Unlike black holes in asymptotic flat space time none of them possess a regular horizon. We also calculate the influence, of a particular class of these solutions, on the Wilson loops calculation. beh...
متن کامل