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Non-Kaehler attracting manifolds
High Energy Physics - Theory · Submitted 4 Feb 2006
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We observe that the new attractor mechanism describing IIB flux vacua for Calabi-Yau compactifications has a possible extension to the landscape of non-Kaehler vacua that emerge in heterotic compactifications with fluxes.
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We observe that the new attractor mechanism describing IIB flux vacua for Calabi-Yau compactifications has a possible extension to the landscape of non-Kaehler vacua that emerge in heterotic compactifications with fluxes. We focus on the effective theories coming from compactifications on generalized half-flat manifolds, showing that the Minkowski "attractor points'' for 3-form fluxes are special-hermitian manifolds.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We observe that the new attractor mechanism describing IIB flux vacua for Calabi-Yau compactifications has a possible extension to the landscape of non-Kaehler vacua that emerge in heterotic compactifications with fluxes. | result 0.75 | 0.76 | 0.48 | hedged possibility 1.00 |
| s1 | We focus on the effective theories coming from compactifications on generalized half-flat manifolds, showing that the Minkowski "attractor points'' for 3-form fluxes are special-hermitian manifolds. | result 0.60 | 0.88 | 0.43 | asserted 1.00 |
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Original abstract
We observe that the new attractor mechanism describing IIB flux vacua for Calabi-Yau compactifications has a possible extension to the landscape of non-Kaehler vacua that emerge in heterotic compactifications with fluxes. We focus on the effective theories coming from compactifications on generalized half-flat manifolds, showing that the Minkowski "attractor points'' for 3-form fluxes are special-hermitian manifolds.
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4 arXiv papers cite this in 4 sentences
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By comparing their result with [ref] we can read off the corresponding embedding tensor as [equation] $Θ^λ̃_Λ$ precisely coincides with the `doubly symplectic' charge matrix $Q$ discussed in [ref] .
Spontaneous N=2 to N=1 Supersymmetry Breaking in Supergravity and Type II String Theory · Realisation in String Theory · 0.98
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