Matter representations from geometry: under the spell of Dynkin
arXiv:2012.13401
Abstract
In the traditional Katz-Vafa method, matter representations are determined by decomposing the adjoint representation of a parent simple Lie algebra as the direct sum of irreducible representations of a semisimple subalgebra . The Katz-Vafa method becomes ambiguous as soon as contains several subalgebras isomorphic to but giving different decompositions of the adjoint representation. We propose a selection rule that characterizes the matter representations observed in generic constructions in F-theory and M-theory: the matter representations in generic F-theory compactifications correspond to linear equivalence classes of subalgebras with Dynkin index one along each simple components of . This simple yet elegant selection rule allows us to apply the Katz-Vafa method to a much large class of models. We illustrate on numerous examples how this proposal streamlines the derivation of matter representations in F-theory and resolves previously ambiguous cases.
arXiv comment66 pages, 14 tables, 10 figures
References in corpus (16)
- Compactifications of F-Theory on Calabi--Yau Threefolds -- II
- Geometric Singularities and Enhanced Gauge Symmetries
- Classifying bases for 6D F-theory models
- Matter and singularities
- The SO(32) Heterotic String on a K3 Surface
- Finite-Dimensional Lie Algebras and Their Representations for Unified Model Building
- A New Model for Elliptic Fibrations with a Rank One Mordell-Weil Group: I. Singular Fibers and Semi-Stable Degenerations
- Calabi-Yau Spaces and Five Dimensional Field Theories with Exceptional Gauge Symmetry
- Mordell-Weil Torsion, Anomalies, and Phase Transitions
- The Geometry of SO(3), SO(5), and SO(6) models
- The Geometry of G, Spin(7), and Spin(8)-models
- The Geometry of F-Models
- Characteristic numbers of elliptic fibrations with non-trivial Mordell-Weil groups
- 48 Crepant Paths to
- Characteristic numbers of crepant resolutions of Weierstrass models
- Flops and Fibral Geometry of E-models