We study asymptotically flat stationary solutions of four-dimensional supergravity theories via the associated G/H* pseudo-Riemannian non-linear sigma models in three spatial dimensions. The Noether charge C associated to G is shown to satisfy a characteristic equation that determines it as a function of the four-dimensional conserved charges. The matrix C is nilpotent for non-rotating extremal solutions. The nilpotency degree of C is directly related to the BPS degree of the corresponding solution when they are BPS. Equivalently, the charges can be described in terms of a Weyl spinor |C > of Spin*(2N), and then the characteristic equation becomes equivalent to a generalisation of the Cartan pure spinor constraint on |C>. The invariance of ...
We provide a general strategy to obtain the superpotential W for both BPS and non-BPS extremal black...
We provide a general strategy to obtain the superpotential W for both BPS and non-BPS extremal black...
We show that the 1/8 BPS condition for composite stationary black holes can be rewritten as a first ...
We study asymptotically flat stationary solutions of four-dimensional supergravity theories via the ...
We study asymptotically flat stationary solutions of four-dimensional supergravity theories via the ...
Dimensional reduction along time offers a powerful way to study stationary solutions of 4D symmetric...
Dimensional reduction along time offers a powerful way to study stationary solutions of 4D symmetric...
The stationary solutions of a large variety of (super)gravity theories can be described within a non...
The stationary solutions of a large variety of (super)gravity theories can be described within a non...
For N \ge 2 supergravities, BPS black hole solutions preserving four supersymmetries can be superpos...
For N \ge 2 supergravities, BPS black hole solutions preserving four supersymmetries can be superpos...
The complete classification of the nilpotent orbits of SO(2,2)2 in the representation (2,2,2,2), ach...
The complete classification of the nilpotent orbits of SO(2,2)2 in the representation (2,2,2,2), ach...
We provide a general strategy to obtain the superpotential W for both BPS and non-BPS extremal black...
We provide a general strategy to obtain the superpotential W for both BPS and non-BPS extremal black...
We provide a general strategy to obtain the superpotential W for both BPS and non-BPS extremal black...
We provide a general strategy to obtain the superpotential W for both BPS and non-BPS extremal black...
We show that the 1/8 BPS condition for composite stationary black holes can be rewritten as a first ...
We study asymptotically flat stationary solutions of four-dimensional supergravity theories via the ...
We study asymptotically flat stationary solutions of four-dimensional supergravity theories via the ...
Dimensional reduction along time offers a powerful way to study stationary solutions of 4D symmetric...
Dimensional reduction along time offers a powerful way to study stationary solutions of 4D symmetric...
The stationary solutions of a large variety of (super)gravity theories can be described within a non...
The stationary solutions of a large variety of (super)gravity theories can be described within a non...
For N \ge 2 supergravities, BPS black hole solutions preserving four supersymmetries can be superpos...
For N \ge 2 supergravities, BPS black hole solutions preserving four supersymmetries can be superpos...
The complete classification of the nilpotent orbits of SO(2,2)2 in the representation (2,2,2,2), ach...
The complete classification of the nilpotent orbits of SO(2,2)2 in the representation (2,2,2,2), ach...
We provide a general strategy to obtain the superpotential W for both BPS and non-BPS extremal black...
We provide a general strategy to obtain the superpotential W for both BPS and non-BPS extremal black...
We provide a general strategy to obtain the superpotential W for both BPS and non-BPS extremal black...
We provide a general strategy to obtain the superpotential W for both BPS and non-BPS extremal black...
We show that the 1/8 BPS condition for composite stationary black holes can be rewritten as a first ...