2008
DOI: 10.1088/1126-6708/2008/10/102
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Nonsupersymmetric flux vacua and perturbed 𝒩 = 2 systems

Abstract: We geometrically engineer N = 2 theories perturbed by a superpotential by adding 3-form flux with support at infinity to local Calabi-Yau geometries in type IIB. This allows us to apply the formalism of Ooguri, Ookouchi, and Park [arXiv:0704.3613] to demonstrate that, by tuning the flux at infinity, we can stabilize the dynamical complex structure moduli in a metastable, supersymmetry-breaking configuration. Moreover, we argue that this setup can arise naturally as a limit of a larger Calabi-Yau which separate… Show more

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Cited by 7 publications
(5 citation statements)
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References 107 publications
(255 reference statements)
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“…(2.2) 5 As usual, we notice that tree-level field theory results match with classical brane pictures at the lowest order in ℓ s under g s → 0, i.e. brane bending and string interaction are not taken into account.…”
Section: Type Iia Setupsupporting
confidence: 64%
See 1 more Smart Citation
“…(2.2) 5 As usual, we notice that tree-level field theory results match with classical brane pictures at the lowest order in ℓ s under g s → 0, i.e. brane bending and string interaction are not taken into account.…”
Section: Type Iia Setupsupporting
confidence: 64%
“…1 Applications and generalizations of these flux vacua are also discussed in a recent paper [5]. 2 As noted in [1], the degree of B 0 (v) polynomial is restricted to at most n − 1 for triviality of the operator Tr Φ k W ′ (Φ)W α W α in N = 1 gauge theory chiral ring.…”
Section: Introductionmentioning
confidence: 97%
“…The list of papers which discuss subjects closely related to that of this subsection include [97,100,[124][125][126][127][128][129][130][131][132][133].…”
Section: Practical Calculationmentioning
confidence: 99%
“…For the computation of higher orders as well as the inclusion of matter, see, for instance, [128,[131][132][133].…”
Section: Practical Calculationmentioning
confidence: 99%
“…On the local non-compact Calabi-Yau geometries of M 6 one cannot move d 6 onto Ω in (3.28). Therefore, the noncompact case allows to model the non-complex geometries by changing the boundary conditions for the non-compact cycles (see the recent discussion in [37,38]).…”
Section: The Scalar Potentialmentioning
confidence: 99%