We find a new non BPS solution in N = 2 D = 4 gauged supergravity coupled to U(1) gauge fields and matter. It consists in a closed universe with two extremal black holes of equal size, surrounding two singularities. They have opposite magnetic charges (and no electric charges), but stay in static equilibrium thanks to the positive pressure of a cosmological constant. The geometry is perfectly symmetric under the exchange of the black holes and the flip of the sign of the charges. However the scalar field is non constant and non symmetric, with different values at the horizons, which depend on a real modulus. Remarkably we show that it satisfies the attractor mechanism and the entropy indeed depends only on the magnetic charges. At one of ...
We present new results towards the construction of the most general black hole solutions in four-dim...
We study static BPS black hole horizons in four dimensional $ \mathcal{N} $ = 2 gauged supergravity ...
We consider four-dimensional N = 2 supergravity coupled to vector- and hypermultiplets, where abelia...
We find a new non BPS solution in N = 2 D = 4 gauged supergravity coupled to U(1) gauge fields and ...
We find a new non BPS solution in N = 2 D = 4 gauged supergravity coupled to U(1) gauge fields and ...
We find a new non BPS solution in N = 2 D = 4 gauged supergravity coupled to U(1) gauge fields and ...
We find a new non BPS solution in N = 2 D = 4 gauged supergravity coupled to U(1) gauge fields and ...
The general solutions of the radial attractor flow equations for extremal black holes, both for non-...
We consider a deformation of the well-known stu model of N = 2, D = 4 supergravity, characterized by...
We consider a deformation of the well-known stu model of $N=2$, $D=4$ supergravity, characterized by...
We construct extremal, spherically symmetric black hole solutions to 4D supergravity with charge ass...
We construct extremal, spherically symmetric black hole solutions to 4D supergravity with charge ass...
We classify the critical points of the effective black hole potential which governs the attractor me...
We present the main features of the physics of extremal black holes embedded in supersymmetric theor...
We investigate four-dimensional spherically symmetric black hole solutions in gravity theories with ...
We present new results towards the construction of the most general black hole solutions in four-dim...
We study static BPS black hole horizons in four dimensional $ \mathcal{N} $ = 2 gauged supergravity ...
We consider four-dimensional N = 2 supergravity coupled to vector- and hypermultiplets, where abelia...
We find a new non BPS solution in N = 2 D = 4 gauged supergravity coupled to U(1) gauge fields and ...
We find a new non BPS solution in N = 2 D = 4 gauged supergravity coupled to U(1) gauge fields and ...
We find a new non BPS solution in N = 2 D = 4 gauged supergravity coupled to U(1) gauge fields and ...
We find a new non BPS solution in N = 2 D = 4 gauged supergravity coupled to U(1) gauge fields and ...
The general solutions of the radial attractor flow equations for extremal black holes, both for non-...
We consider a deformation of the well-known stu model of N = 2, D = 4 supergravity, characterized by...
We consider a deformation of the well-known stu model of $N=2$, $D=4$ supergravity, characterized by...
We construct extremal, spherically symmetric black hole solutions to 4D supergravity with charge ass...
We construct extremal, spherically symmetric black hole solutions to 4D supergravity with charge ass...
We classify the critical points of the effective black hole potential which governs the attractor me...
We present the main features of the physics of extremal black holes embedded in supersymmetric theor...
We investigate four-dimensional spherically symmetric black hole solutions in gravity theories with ...
We present new results towards the construction of the most general black hole solutions in four-dim...
We study static BPS black hole horizons in four dimensional $ \mathcal{N} $ = 2 gauged supergravity ...
We consider four-dimensional N = 2 supergravity coupled to vector- and hypermultiplets, where abelia...