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F-theory and All Things Rational: Surveying U(1) Symmetries with Rational Sections

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arxiv 1504.05593 v2 pith:O6DCQK3X submitted 2015-04-21 hep-th math.AG

classification hep-thmath.AG
keywords rationalfibersgaugesectionssymmetriescodimensionf-theorytheories
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We study elliptic fibrations for F-theory compactifications realizing 4d and 6d supersymmetric gauge theories with abelian gauge factors. In the fibration these U(1) symmetries are realized in terms of additional rational sections. We obtain a universal characterization of all the possible U(1) charges of matter fields by determining the corresponding codimension two fibers with rational sections. In view of modelling supersymmetric Grand Unified Theories, one of the main examples that we analyze are U(1) symmetries for SU(5) gauge theories with \bar{5} and 10 matter. We use a combination of constraints on the normal bundle of rational curves in Calabi-Yau three- and four-folds, as well as the splitting of rational curves in the fibers in codimension two, to determine the possible configurations of smooth rational sections. This analysis straightforwardly generalizes to multiple U(1)s. We study the flops of such fibers, as well as some of the Yukawa couplings in codimension three. Furthermore, we carry out a universal study of the U(1)-charged GUT singlets, including their KK-charges, and determine all realizations of singlet fibers. By giving vacuum expectation values to these singlets, we propose a systematic way to analyze the Higgsing of U(1)s to discrete gauge symmetries in F-theory.

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Cited by 2 Pith papers

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  1. Heterotic-$\mathbf{F}$-theory Duality with Wilson Line Symmetry-breaking

    hep-th 2019-08 conditional novelty 7.0 of 10

    A new F-theory construction with two elliptic sections gives an MSSM spectrum with no vector-like exotics via Wilson line breaking.

  2. F-theory models with $U(1)\times \mathbb{Z}_2,\, \mathbb{Z}_4$ and transitions in discrete gauge groups

    hep-th 2019-08 conditional novelty 4.0 of 10

    On bisection loci in a four-section geometry, the F-theory gauge group enlarges from Z2 to U(1) times Z2, and Higgsing can break it down to a discrete Z4 gauge group.

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