• Documents
  • Authors
  • Tables
  • Log in
  • Sign up
  • MetaCart
  • DMCA
  • Donate

CiteSeerX logo

Advanced Search Include Citations
Advanced Search Include Citations

Stationary black holes and attractor mechanism, Nucl. Phys. B794 (2008)

by D Astefanesei, H Yavartanoo
Add To MetaCart

Tools

Sorted by:
Results 11 - 20 of 38
Next 10 →

Realization of AdS Vacua in Attractor Mechanism on Generalized Geometry

by Tetsuji Kimura , 2008
"... We evaluate flux vacua attractor equations in type IIA string theory compactified on generalized geometry with orientifold projection. This model provides N = 1 superpotential as a sum of the Ramond-Ramond superpotential and the one described by the (non)geometric flux charges. We demonstrate a sing ..."
Abstract - Cited by 2 (1 self) - Add to MetaCart
We evaluate flux vacua attractor equations in type IIA string theory compactified on generalized geometry with orientifold projection. This model provides N = 1 superpotential as a sum of the Ramond-Ramond superpotential and the one described by the (non)geometric flux charges. We demonstrate a single modulus model in which supersymmetric AdS and Minkowski solutions are classified by means of the discriminants of the two superpotentials. We further study various configurations without the Ramond-Ramond flux charges. We also find supersymmetric AdS vacua both in the case of compactifications on the generalized geometry with SU(3) × SU(3) structure, and on the manifold with SU(3)-structure without the nongeometric flux charges. Especially, in the latter case, we should introduce a correction into the prepotential of the special geometry in order to realize consistent vacua. This deformation is interpreted as the back reaction of the geometric

stu Black Holes Unveiled

by Stefano Bellucci, Sergio Ferrara , 807
"... The general solutions of the radial attractor flow equations for extremal black holes, both for non-BPS with non-vanishing central charge Z and for Z = 0, are obtained for the so-called stu model, the minimal rank-3 N = 2 symmetric supergravity in d = 4 space-time dimensions. Comparisons with previo ..."
Abstract - Cited by 1 (0 self) - Add to MetaCart
The general solutions of the radial attractor flow equations for extremal black holes, both for non-BPS with non-vanishing central charge Z and for Z = 0, are obtained for the so-called stu model, the minimal rank-3 N = 2 symmetric supergravity in d = 4 space-time dimensions. Comparisons with previous results, as well as the fake supergravity (first order) formalism and an analysis of the BPS bound all along the non-BPS attractor flows and of the marginal stability of corresponding D-
(Show Context)

Citation Context

... recalled that for extremal BHs the solution converging at the BH event horizon (r → r + H ) does not depend on the initial, asymptotical values of the scalar fields. See e.g. discussions in [33] and =-=[44]-=-. 3We are grateful to E. G. Gimon for a clarifying discussion about the definition of “gap” above the BPS bound as given in [59]. 42 Basics of the stu Model We here recall some basic facts of the abo...

Double-Horizon Limit, AdS Geometry and Entropy Function

by H. Arfaei, R. Fareghbal , 2007
"... We start from a generic metric which describes four dimensional stationary black holes in an arbitrary theory of gravity and show that the AdS2 part of the near horizon geometry is a consequence of the double-horizon limit and finiteness. We also show that the field configurations of the near horizo ..."
Abstract - Cited by 1 (0 self) - Add to MetaCart
We start from a generic metric which describes four dimensional stationary black holes in an arbitrary theory of gravity and show that the AdS2 part of the near horizon geometry is a consequence of the double-horizon limit and finiteness. We also show that the field configurations of the near horizon are determined if the same conditions are applied to the equations of motion. This is done by showing that in the double-horizon limit field equations at the horizon decouple from the bulk of the space. Solving these equations gives the near horizon field configurations. It is shown that these decoupled equations can be obtained from an action derived from the original action by applying the double-horizon
(Show Context)

Citation Context

... possible to find a method like the entropy function for the non-extremal cases which do not have AdS part in the near horizon geometry? There has been several attempts to answer these questions [8]- =-=[10]-=-. In this paper we show that both of these two questions can be approached from a single point of view. This point is applying finiteness assumption on the physical quantities at the horizon of the do...

unknown title

by Predrag Dominis Prester, Tomislav Terzić , 809
"... Preprint typeset in JHEP style- PAPER VERSION ..."
Abstract - Add to MetaCart
Preprint typeset in JHEP style- PAPER VERSION
(Show Context)

Citation Context

...um on it, there are also Kaluza-Klein and H-monopoles (NS5-branes) wound around the same S 1 and T 4 (with ”nut” on second S 1 ). For extremal black holes one expects AdS2 × S 2 near-horizon geometry =-=[27, 28, 29]-=- which in the present case is given by: ds 2 ≡ Gµνdx µ dx ν = v1 e −2Φ = uS , T1 = u1 , T2 = u2 , F (1) rt = ˜e1, F (3) rt 2h1 ( −r 2 dt 2 + dr2 r2 ) + v2(dθ 2 + sin 2 θdφ 2 ), ˜e3 (2) ˜p2 = , F 16 θφ...

unknown title

by Predrag Dominis Prester, Tomislav Terzić , 809
"... Preprint typeset in JHEP style- PAPER VERSION ..."
Abstract - Add to MetaCart
Preprint typeset in JHEP style- PAPER VERSION
(Show Context)

Citation Context

...um on it, there are also Kaluza-Klein and H-monopoles (NS5-branes) wound around the same S 1 and T 4 (with ”nut” on second S 1 ). For extremal black holes one expects AdS2 × S 2 near-horizon geometry =-=[27, 28, 29]-=- which in the present case is given by: ds 2 ≡ Gµνdx µ dx ν ( = v1 −r 2 dt 2 + dr2 r2 ) + v2(dθ 2 + sin 2 θdφ 2 ), e −2Φ = uS , T1 = u1 , T2 = u2 , F (1) rt = ˜e1, F (3) ˜e3 (2) ˜p2 (4) ˜p4 rt = , F 1...

unknown title

by Xian-hui Ge, Fu-wen Shu , 804
"... Preprint typeset in JHEP style- HYPER VERSION ..."
Abstract - Add to MetaCart
Preprint typeset in JHEP style- HYPER VERSION
(Show Context)

Citation Context

...matter fields, the near horizon geometry of a spherically symmetric extremal black hole in n dimensions has SO(2,1) × SO(D − 1) isometry[20]. In four and five dimensions, this postulate was proved in =-=[21, 22, 23]-=-. The near horizon geometry of non-extremal black holes in the presence of higher derivative gravity terms might not have the SO(2,1) × SO(D − 1) isometry, and also there is no attractor mechanism for...

“Constituents, Fundamental Forces and Symmetries of the Universe”,

by Stefano Bellucci, Sergio Ferrara, Alessio Marrani, Museo Storico Della Fisica E , 805
"... Contribution to the Proceedings of the 3rd RTN Workshop ..."
Abstract - Add to MetaCart
Contribution to the Proceedings of the 3rd RTN Workshop

arXiv:0804.3811 The Entropy Function for the extremal Kerr-(anti-)de Sitter Black Holes

by Jin-ho Cho, Yumi Ko, Soonkeon Nam , 804
"... Preprint typeset in JHEP style- HYPER VERSION ..."
Abstract - Add to MetaCart
Preprint typeset in JHEP style- HYPER VERSION
(Show Context)

Citation Context

... function formalism is applicable. There have been several works on non-supersymmetric extremal black holes. The examples include charged black holes in de Sitter background [6], rotating black holes =-=[7, 8, 9]-=-, and black holes of Nariai class [10]. In these cases, the entropy function formalism gives the correct values of the Bekenstein-Hawking entropy. In this paper, we would like to study yet another exa...

DCPT-08/17

by unknown authors , 803
"... Extremal vacuum black holes in higher dimensions ..."
Abstract - Add to MetaCart
Extremal vacuum black holes in higher dimensions
(Show Context)

Citation Context

...e assumption of SO(2, 1) symmetry in the nearhorizon limit (subsequently proved in [42]) has been used to establish an attractor mechanism for rotating extremal black holes in D = 4, 5 [51] (see also =-=[52]-=-). 3of an asymptotically flat extremal black ring in D = 2n + 3 spacetime dimensions, provided one takes a particular value for the boost parameter. This value must be such that the MP string is tens...

CERN-PH-TH/2008-002 UCLA/08/TEP/11 Erice Lectures on Black Holes and Attractors

by Sergio Ferrara, Kuniko Hayakawa, Alessio Marrani, Museo Storico Della Fisica E
"... These lectures give an elementary introduction to the subject of four dimensional black holes (BHs) in supergravity and the Attractor Mechanism in the extremal case. Some thermodynamical properties are discussed and some relevant formulæ for the critical points of the BH effective potential are give ..."
Abstract - Add to MetaCart
These lectures give an elementary introduction to the subject of four dimensional black holes (BHs) in supergravity and the Attractor Mechanism in the extremal case. Some thermodynamical properties are discussed and some relevant formulæ for the critical points of the BH effective potential are given. The case of Maxwell-Einstein-axion-dilaton (super)gravity is discussed in detail. Analogies among BH entropy and multipartite entanglement of qubits in quantum information theory, as well moduli spaces of extremal BH attractors, are also
Powered by: Apache Solr
  • About CiteSeerX
  • Submit and Index Documents
  • Privacy Policy
  • Help
  • Data
  • Source
  • Contact Us

Developed at and hosted by The College of Information Sciences and Technology

© 2007-2019 The Pennsylvania State University