2011
DOI: 10.1016/j.physletb.2011.10.055
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On marginal deformations of (0,2) non-linear sigma models

Abstract: An N=1, d=4 supersymmetric compactification of the perturbative heterotic string is described by a d=2 (0,2) superconformal field theory. The first-order marginal deformations of the internal (0,2) SCFT are in 1 to 1 correspondence with massless gaugeneutral scalars in the spacetime theory. Working at tree-level in the α ′ expansion, we describe these first order deformations for SCFTs with a (0,2) non-linear sigma model description. Our results clarify the structure of deformations of heterotic Calabi-Yau com… Show more

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Cited by 24 publications
(37 citation statements)
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“…We derive results valid through first order 1 in α ′ , a technical improvement over the discussion of [5], with our results being in agreement with that work in the limit where α ′ → 0. On the other hand, unlike [5], we 'overcount' the massless degrees of freedom of the compactification as, as we will describe, we shall only analyze a subset of the conditions imposed upon the system by Strominger. Our supergravity deformation analysis will also be restricted to compactifications on spaces satisfying the ∂∂-lemma, which can be stated as follows:…”
Section: Introductionsupporting
confidence: 83%
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“…We derive results valid through first order 1 in α ′ , a technical improvement over the discussion of [5], with our results being in agreement with that work in the limit where α ′ → 0. On the other hand, unlike [5], we 'overcount' the massless degrees of freedom of the compactification as, as we will describe, we shall only analyze a subset of the conditions imposed upon the system by Strominger. Our supergravity deformation analysis will also be restricted to compactifications on spaces satisfying the ∂∂-lemma, which can be stated as follows:…”
Section: Introductionsupporting
confidence: 83%
“…More precisely, we will show that fluctuations satisfying (2.54) and (2.55) are classified by the cohomology H 1 (H) of a bundle H that we will specify. In section 5 we will see that, in the limit α ′ → 0, the equations above precisely duplicate the cocycle conditions found in the worldsheet analysis of [5].…”
Section: Jhep07(2014)037mentioning
confidence: 59%
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