2007
DOI: 10.1088/1126-6708/2007/02/078
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Null deformed domain wall

Abstract: We study null 1/4 BPS deformations of flat Domain Wall solutions (NDDW) in N = 2, d = 5 gauged supergravity with hypermultiplets and vector multiplets coupled. These are uncharged timedependent configurations and contain as special case, 1/2 supersymmetric flat domain walls (DW) and, as well, 1/2 BPS null solutions of the ungauged supergravity. Combining our analysis with the classification method initiated by Gauntlett et al., we prove that all the possible deformations of the DW have origin in the hypermulti… Show more

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Cited by 10 publications
(5 citation statements)
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“…Instead, in this regime one recovers the previous analysis with the scalar potential (20). Thus V 2 0 /σ is assumed to be the coupling connecting asymptotic regimes of the exact potential (18) given in the form…”
Section: First-order Frameworkmentioning
confidence: 95%
See 1 more Smart Citation
“…Instead, in this regime one recovers the previous analysis with the scalar potential (20). Thus V 2 0 /σ is assumed to be the coupling connecting asymptotic regimes of the exact potential (18) given in the form…”
Section: First-order Frameworkmentioning
confidence: 95%
“…On the domain walls, the brane is flat assuming a four-dimensional Minkowski geometry [1], whereas far from the domain walls the brane is bent [7,8] and assumes a four-dimensional Anti-de-Sitter (AdS 4 ) geometry -see, e.g., Refs. [11,12,13,14,15,16,17,18,19,20,21,22].…”
Section: Introductionmentioning
confidence: 99%
“…When the domain-wall is supported by scalar fields (we neglect charged domain-walls like those constructed in [20,21]), and for p = 2, the effective action follows from the lagrangian…”
Section: Black Holes and Domain Wallsmentioning
confidence: 99%
“…Nevertheless, the domain walls, together with some of their deformations [22], are the only configurations studied in full generality for all the possible multiplets coupling. This is not true for black holes, which have been considered in full extent only in presence of vector multiplets [23,24,25,10,26,27,28,29,30].…”
Section: Introduction and Resultsmentioning
confidence: 99%
“…where the consistency imposes Λ 2 + f r f r = 1. By the use of the identities of the quaternionic manifold, the hyperini equation turns out to be equivalent (see also [12,22]) to…”
Section: A2 Bps Equation For Spherically Symmetric Configurationsmentioning
confidence: 99%