Supersymmetric black holes

@article{Kallosh1992SupersymmetricBH,
  title={Supersymmetric black holes},
  author={Renata Kallosh},
  journal={Physics Letters B},
  year={1992},
  volume={282},
  pages={80-88}
}
  • R. Kallosh
  • Published 15 January 1992
  • Physics
  • Physics Letters B

BPS black holes in a non-homogeneous deformation of the stu model of N = 2, D = 4 gauged supergravity

A bstractWe consider a deformation of the well-known stu model of N = 2, D = 4 supergravity, characterized by a non-homogeneous special Kähler manifold, and by the smallest electric-magnetic duality

Static BPS black holes in U(1) gauged supergravity

A bstractWe consider the flow equations for 1/4-BPS asymptotically AdS4 static black holes in Fayet-Iliopoulos gauged supergravity, using very special geometry identities to obtain a simplified form

AdS black holes from duality in gauged supergravity

A bstractWe study and utilize duality transformations in a particular STU-model of four dimensional gauged supergravity. This model is a truncation of the de Wit-Nicolai $ \mathcal{N} $ =8 theory and

Massless string theory black holes as black diholes and quadruholes.

  • Ortín
  • Physics
    Physical review letters
  • 1996
TLDR
Massless BH solutions of the low-energy heterotic string effective action were recently discovered and some properties of these objects are as follows.
...

References

SHOWING 1-10 OF 31 REFERENCES

Renormalizability Properties of Supergravity

The possible local counterterms in supergravity are investigated to all loop orders. Supersymmetry implies that (1) supergravity-matter coupling is one-loop nonrenormalizable, with a specific

Supergravity and Superstrings

Over the last decade, theorists have been searching hard for a unified quantum field theory of physical interactions with or without gravitation. The “standard” SU_3 x SU_2 x U_1 theory has three

Special geometry without special coordinates

Presents a detailed geometric derivation of N=2, 4D supergravity coupled to Abelian vector multiplets (1,1/2,0). The theory is covariant under reparametrisations of the manifold M spanned by the