2008
DOI: 10.1002/prop.200810552
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Warped generalized geometry compactifications, effective theories and non‐perturbative effects

Abstract: Summarizing the results of [1], we discuss the four-dimensional effective approach to type II N = 1 supersymmetric flux compactifications with general SU (3) × SU (3)-structure. In particular, we study the effect of a non-trivial warp factor, which we argue leads naturally to a supergravity formulation invariant under local complexified Weyl transformations. We show that the full ten-dimensional supersymmetry equations can be obtained as F-flatness and D-flatness conditions from the superpotential and Kähler p… Show more

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Cited by 16 publications
(55 citation statements)
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“…Thus, at large distances the structure is approximately SU (3), but the presence of a small cosmological constant remains. This indicates that the description proposed in [23,24] in terms of smeared instantons can capture the important physics as seen from a distant observer. Also, the fact that µ and the deformation parameter ϕ are small far away from the region where NP effects are large could allow for a perturbative treatment.…”
Section: Further Commentsmentioning
confidence: 84%
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“…Thus, at large distances the structure is approximately SU (3), but the presence of a small cosmological constant remains. This indicates that the description proposed in [23,24] in terms of smeared instantons can capture the important physics as seen from a distant observer. Also, the fact that µ and the deformation parameter ϕ are small far away from the region where NP effects are large could allow for a perturbative treatment.…”
Section: Further Commentsmentioning
confidence: 84%
“…We would also like to point out that a connection between the non-perturbatively modified supersymmetry equation (3.7) and a would-be ten-dimensional description of the supersymmetric AdS 4 solution of [1] was attempted in [23,24]. However, this was done by using smeared instatons, that is, roughly speaking, by replacing the NP current δ 2 [Σ 4 ] in (3.4) by a suitably normalized two-form proportional to Im Ψ 1 ∼ J, allowing the authors to keep the original SU (3) structure.…”
Section: Discussionmentioning
confidence: 99%
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