2009
DOI: 10.1016/j.nuclphysb.2009.05.019
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Relative periods and open-string integer invariants for a compact Calabi–Yau hypersurface

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Cited by 30 publications
(64 citation statements)
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(91 reference statements)
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“…The geometric structure of open/closed B-model and the associated off-shell superpotential depending on the open and closed string moduli has been studied from the viewpoint of N = 1 special geometry [19,20] for the case of non-compact Calabi-Yau threefolds [15,16]. In [17] (see also [41]), the study of off-shell superpotential was extended to com- In this section, we utilize the method of [17] in general dimensions and explicitly compute the open/closed Picard-Fuchs equation for septic Calabi-Yau fivefold X 7 . Then we will solve the resulting differential system in the vicinity of the Landau-Ginzburg point, and also check the consistency with the on-shell result.…”
Section: Off-shell Formalism Via Relative Periodsmentioning
confidence: 99%
“…The geometric structure of open/closed B-model and the associated off-shell superpotential depending on the open and closed string moduli has been studied from the viewpoint of N = 1 special geometry [19,20] for the case of non-compact Calabi-Yau threefolds [15,16]. In [17] (see also [41]), the study of off-shell superpotential was extended to com- In this section, we utilize the method of [17] in general dimensions and explicitly compute the open/closed Picard-Fuchs equation for septic Calabi-Yau fivefold X 7 . Then we will solve the resulting differential system in the vicinity of the Landau-Ginzburg point, and also check the consistency with the on-shell result.…”
Section: Off-shell Formalism Via Relative Periodsmentioning
confidence: 99%
“…Thus, we can interpret the seven-brane superpotential as a special case of the five-brane superpotential, where a description of the five-brane curve Σ in terms of seven-brane flux [F 2 ] = Σ is applicable [80], see also [100,120,121,123,[126][127][128][129] for a similar use of the seven-brane superpotential. 21 It is important to emphasize that the five-brane charge is only locally non-trivial, i.e.…”
Section: The Flux Superpotentialmentioning
confidence: 99%
“…away from the sublocus M P 1 (Σ) defined by (7.34), this embedding implies that the obstructed deformation space of the rational curves (7.35) is identified with the unobstructed moduli space M(Σ). This can be compared to the method presented in [115,120,121,123] where the obstructed deformations of a curve are identified with the unobstructed moduli of an appropriate divisor. For the curves we consider we depict the embedding of the deformation spaces of the rational curves into the moduli space M(Σ) of complete intersection Σ in figure 7.4, where we introduce new open moduliẑ 1 ,ẑ 2 that are functions of the u i .…”
Section: Matching Deformations and Obstructions: Concrete Examplesmentioning
confidence: 99%
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