In these lectures we give a geometrical formulation of N-extrended supergravities which generalizes N = 2 special geometry of N = 2 theories. In all these theories duality symmetries are related to the notion of “flat symplectic bundles” and central charges may be defined as “sections” over these bundles. Attractor points giving rise to “fixed scalars” of the horizon geometry and Bekenstein-Hawking entropy formula for extremal black-holes are discussed in some details
Extremal black holes are states in the non-perturbative spectrum of Supergravity theories. They may ...
Abstract Freudenthal duality is, as of now, the unique non-linear map on electric-magnetic (e.m.) ch...
We consider supersymmetric AdS3 × Y7 and AdS2 × Y9 solutions of type IIB and D = 11 supergravity, re...
We report on some general results on the physics of extremal BPS black holes in four and five dimens...
We generalize central-charge relations and differential identities of N=2 Special Geometry to N exte...
A geometric formulation which describes extended supergravities in any dimension in the presence of ...
We consider the Bekenstein-Hawking entropy-area formula in four dimensional extended ungauged superg...
Electric-magnetic duality invariance of extended Supergravity theories has been a very powerful tool...
We report on recent results in the study of extremal black hole attractors in N=2, d=4 ungauged Maxw...
We discuss various topics in supergravity: gaugings, double field theory and $N=2$ $D=4$ BPS multice...
We report on some general results on the physics of extremal BPS black holes in four and five dimens...
In these lectures we explain the concept of supergravity p-branes and BPS black holes. Introducing a...
Abstract Freudenthal duality in N = 2, D = 4 ungauged supergravity is generated by an anti-involutiv...
Freudenthal duality, introduced in L. Borsten, D. Dahanayake, M. J. Duff and W. Rubens, Phys.Rev. D8...
In these lectures we introduce some of the principles and techniques that are relevant for the deter...
Extremal black holes are states in the non-perturbative spectrum of Supergravity theories. They may ...
Abstract Freudenthal duality is, as of now, the unique non-linear map on electric-magnetic (e.m.) ch...
We consider supersymmetric AdS3 × Y7 and AdS2 × Y9 solutions of type IIB and D = 11 supergravity, re...
We report on some general results on the physics of extremal BPS black holes in four and five dimens...
We generalize central-charge relations and differential identities of N=2 Special Geometry to N exte...
A geometric formulation which describes extended supergravities in any dimension in the presence of ...
We consider the Bekenstein-Hawking entropy-area formula in four dimensional extended ungauged superg...
Electric-magnetic duality invariance of extended Supergravity theories has been a very powerful tool...
We report on recent results in the study of extremal black hole attractors in N=2, d=4 ungauged Maxw...
We discuss various topics in supergravity: gaugings, double field theory and $N=2$ $D=4$ BPS multice...
We report on some general results on the physics of extremal BPS black holes in four and five dimens...
In these lectures we explain the concept of supergravity p-branes and BPS black holes. Introducing a...
Abstract Freudenthal duality in N = 2, D = 4 ungauged supergravity is generated by an anti-involutiv...
Freudenthal duality, introduced in L. Borsten, D. Dahanayake, M. J. Duff and W. Rubens, Phys.Rev. D8...
In these lectures we introduce some of the principles and techniques that are relevant for the deter...
Extremal black holes are states in the non-perturbative spectrum of Supergravity theories. They may ...
Abstract Freudenthal duality is, as of now, the unique non-linear map on electric-magnetic (e.m.) ch...
We consider supersymmetric AdS3 × Y7 and AdS2 × Y9 solutions of type IIB and D = 11 supergravity, re...