Unification, KK-thresholds and the top Yukawa coupling in F-theory GUTs

TL;DR

This paper develops a method to estimate Yukawa couplings in F-theory GUTs using wavefunction overlaps, KK thresholds, and topological invariants, successfully matching observed top and bottom quark masses.

Contribution

It introduces a novel approach to determine Yukawa couplings from U(1) charges and topological data, improving predictive power in F-theory GUT models.

Findings

Yukawa couplings depend solely on U(1) charges and topological torsion.

The model's top and bottom quark masses align with experimental data.

The approach constrains matter content using KK threshold effects.

Abstract

In a class of F-theory SU(5) GUTs the low energy chiral mass spectrum is obtained from rank one fermion mass textures with a hierarchical structure organised by U(1) symmetries embedded in the exceptional E_8 group. In these theories chiral fields reside on matter `curves' and the tree level masses are computed from integrals of overlapping wavefuctions of the particles at the triple intersection points. This calculation requires knowledge of the exact form of the wavefuctions. In this work we propose a way to obtain a reliable estimate of the various quantities which determine the strength of the Yukawa couplings. We use previous analysis of KK threshold effects to determine the (ratios of) heavy mass scales of the theory which are involved in the normalization of the wave functions. We consider similar effects from the chiral spectrum of these models and discuss possible constraints on the emerging matter content. In this approach, we find that the Yukawa couplings can be determined solely from the U(1) charges of the states in the `intersection' and the torsion which is a topological invariant quantity. We apply the results to a viable SU(5) model with minimal spectrum which satisfies all the constraints imposed by our analysis. We use renormalization group analysis to estimate the top and bottom masses and find that they are in agreement with the experimental values.