Higgs couplings and new signals from Flavon-Higgs mixing effects within multi-scalar models

TL;DR

This paper explores how mixing effects in multi-scalar models with extended Higgs sectors and Froggatt-Nielsen mechanisms can lead to observable deviations in Higgs couplings, flavor-violating processes, and new signals at colliders.

Contribution

It introduces a specific 3+1 Higgs doublet model with a singlet FN field, analyzing its phenomenology and experimental constraints, including dark matter and flavor violation.

Findings

Modified Higgs couplings due to mixing effects

Potential signals from flavon fields and heavy Higgs bosons

Constraints on flavor-changing top decays from LHC data

Abstract

Testing the properties of the Higgs particle discovered at the LHC and searching for new physics signals, are some of the most important tasks of Particle Physics today. Current measurements of the Higgs couplings to fermions and gauge bosons, seem consistent with the Standard Model, and when taken as a function of the particle mass, should lay on a single line. However, in models with an extended Higgs sector the diagonal Higgs couplings to up-quarks, down-quarks and charged leptons, could lay on different lines, while non-diagonal flavor-violating Higgs couplings could appear too. We describe these possibilities within the context of multi-Higgs doublet models that employ the Froggatt-Nielsen (FN) mechanism to generate the Yukawa hierarchies. Furthermore, one of the doublets can be chosen to be of the inert type, which provides a viable dark matter candidate. The mixing of the Higgs doublets with the flavon field, can provide plenty of interesting signals, including: i) small corrections to the couplings of the SM-like Higgs, ii) exotic signals from the flavon fields, iii) new signatures from the heavy Higgs bosons. These aspects are studied within a specific model with 3+1 Higgs doublets and a singlet FN field. Constraints on the model are derived from the study of K and D mixing and the Higgs search at the LHC. For last, the implications from the latter aforementioned constraints to the FCNC top decay $t\to ch$ are presented too.