Cargando…

F-theory vacua with $\mathbb Z_3$ gauge symmetry

Discrete gauge groups naturally arise in F-theory compactifications on genus-one fibered Calabi-Yau manifolds. Such geometries appear in families that are parameterized by the Tate-Shafarevich group of the genus-one fibration. While the F-theory compactification on any element of this family gives r...

Descripción completa

Detalles Bibliográficos
Autores principales: Cvetič, Mirjam, Donagi, Ron, Klevers, Denis, Piragua, Hernan, Poretschkin, Maximilian
Lenguaje:eng
Publicado: 2015
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.nuclphysb.2015.07.011
http://cds.cern.ch/record/1994683
_version_ 1780945847468425216
author Cvetič, Mirjam
Donagi, Ron
Klevers, Denis
Piragua, Hernan
Poretschkin, Maximilian
author_facet Cvetič, Mirjam
Donagi, Ron
Klevers, Denis
Piragua, Hernan
Poretschkin, Maximilian
author_sort Cvetič, Mirjam
collection CERN
description Discrete gauge groups naturally arise in F-theory compactifications on genus-one fibered Calabi-Yau manifolds. Such geometries appear in families that are parameterized by the Tate-Shafarevich group of the genus-one fibration. While the F-theory compactification on any element of this family gives rise to the same physics, the corresponding M-theory compactifications on these geometries differ and are obtained by a fluxed circle reduction of the former. In this note, we focus on an element of order three in the Tate-Shafarevich group of the general cubic. We discuss how the different M-theory vacua and the associated discrete gauge groups can be obtained by Higgsing of a pair of five-dimensional U(1) symmetries. The Higgs fields arise from vanishing cycles in $I_2$-fibers that appear at certain codimension two loci in the base. We explicitly identify all three curves that give rise to the corresponding Higgs fields. In this analysis the investigation of different resolved phases of the underlying geometry plays a crucial rôle.
id cern-1994683
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2015
record_format invenio
spelling cern-19946832023-03-14T17:20:41Zdoi:10.1016/j.nuclphysb.2015.07.011http://cds.cern.ch/record/1994683engCvetič, MirjamDonagi, RonKlevers, DenisPiragua, HernanPoretschkin, MaximilianF-theory vacua with $\mathbb Z_3$ gauge symmetryParticle Physics - TheoryDiscrete gauge groups naturally arise in F-theory compactifications on genus-one fibered Calabi-Yau manifolds. Such geometries appear in families that are parameterized by the Tate-Shafarevich group of the genus-one fibration. While the F-theory compactification on any element of this family gives rise to the same physics, the corresponding M-theory compactifications on these geometries differ and are obtained by a fluxed circle reduction of the former. In this note, we focus on an element of order three in the Tate-Shafarevich group of the general cubic. We discuss how the different M-theory vacua and the associated discrete gauge groups can be obtained by Higgsing of a pair of five-dimensional U(1) symmetries. The Higgs fields arise from vanishing cycles in $I_2$-fibers that appear at certain codimension two loci in the base. We explicitly identify all three curves that give rise to the corresponding Higgs fields. In this analysis the investigation of different resolved phases of the underlying geometry plays a crucial rôle.Discrete gauge groups naturally arise in F-theory compactifications on genus-one fibered Calabi–Yau manifolds. Such geometries appear in families that are parameterized by the Tate–Shafarevich group of the genus-one fibration. While the F-theory compactification on any element of this family gives rise to the same physics, the corresponding M-theory compactifications on these geometries differ and are obtained by a fluxed circle reduction of the former. In this note, we focus on an element of order three in the Tate–Shafarevich group of the general cubic. We discuss how the different M-theory vacua and the associated discrete gauge groups can be obtained by Higgsing of a pair of five-dimensional U(1) symmetries. The Higgs fields arise from vanishing cycles in I2 -fibers that appear at certain codimension two loci in the base. We explicitly identify all three curves that give rise to the corresponding Higgs fields. In this analysis the investigation of different resolved phases of the underlying geometry plays a crucial rôle.Discrete gauge groups naturally arise in F-theory compactifications on genus-one fibered Calabi-Yau manifolds. Such geometries appear in families that are parameterized by the Tate-Shafarevich group of the genus-one fibration. While the F-theory compactification on any element of this family gives rise to the same physics, the corresponding M-theory compactifications on these geometries differ and are obtained by a fluxed circle reduction of the former. In this note, we focus on an element of order three in the Tate-Shafarevich group of the general cubic. We discuss how the different M-theory vacua and the associated discrete gauge groups can be obtained by Higgsing of a pair of five-dimensional U(1) symmetries. The Higgs fields arise from vanishing cycles in $I_2$-fibers that appear at certain codimension two loci in the base. We explicitly identify all three curves that give rise to the corresponding Higgs fields. In this analysis the investigation of different resolved phases of the underlying geometry plays a crucial r\^ole.arXiv:1502.06953CERN-PH-TH-2015-034CERN-PH-TH-2015-034oai:cds.cern.ch:19946832015-02-24
spellingShingle Particle Physics - Theory
Cvetič, Mirjam
Donagi, Ron
Klevers, Denis
Piragua, Hernan
Poretschkin, Maximilian
F-theory vacua with $\mathbb Z_3$ gauge symmetry
title F-theory vacua with $\mathbb Z_3$ gauge symmetry
title_full F-theory vacua with $\mathbb Z_3$ gauge symmetry
title_fullStr F-theory vacua with $\mathbb Z_3$ gauge symmetry
title_full_unstemmed F-theory vacua with $\mathbb Z_3$ gauge symmetry
title_short F-theory vacua with $\mathbb Z_3$ gauge symmetry
title_sort f-theory vacua with $\mathbb z_3$ gauge symmetry
topic Particle Physics - Theory
url https://dx.doi.org/10.1016/j.nuclphysb.2015.07.011
http://cds.cern.ch/record/1994683
work_keys_str_mv AT cveticmirjam ftheoryvacuawithmathbbz3gaugesymmetry
AT donagiron ftheoryvacuawithmathbbz3gaugesymmetry
AT kleversdenis ftheoryvacuawithmathbbz3gaugesymmetry
AT piraguahernan ftheoryvacuawithmathbbz3gaugesymmetry
AT poretschkinmaximilian ftheoryvacuawithmathbbz3gaugesymmetry