Towards UV-Models of Kinetic Mixing and Portal Matter IV: Quartification

TL;DR

This paper explores a quartification extension of the Standard Model with an additional dark gauge group, predicting new portal matter fields and collider signatures, especially focusing on kinetic mixing and dark photon phenomenology.

Contribution

It introduces a quartification model with a dark gauge group, analyzing its structure, kinetic mixing, and collider phenomenology with a simplified fermion generation.

Findings

Predicts the existence of color-singlet portal matter fields.

Identifies potential collider signatures at LHC and future colliders.

Links portal matter masses to new gauge bosons from the extended gauge sector.

Abstract

As is well-known, Trinification, \ie, the extension of the Standard Model (SM) to $[SU(3)]^3=SU(3)_c\times SU(3)_L\times SU(3)_R$ as occurs in $E_6$ models, allows for a partial unification of the gauge forces even though quarks and leptons remain in separate multiplets so that no heavy gauge or scalar fields exist which can generate proton decay. The extension of this idea to Quartification, by including an additional $SU(3)'$ factor, has also been considered in the literature maintaining the basic attributes of Trinification but now allowing, \eg, for a more symmetric treatment of quarks and leptons at the price of new matter fields and gauge interactions. In this paper, we will consider this $SU(3)'$ to be the `dark' gauge group, now containing the familiar $U(1)_D$ subgroup, under which the SM fields are all neutral, which is associated with kinetic mixing (KM) and the existence of a light, $\lsim 1 $ GeV dark photon. This setup naturally predicts the existence of color-singlet portal matter (PM) fields, carrying both electromagnetic and $U(1)_D$ dark charges, that are necessary to generate this KM at the 1-loop level and whose masses are directly tied with those of the many new gauge bosons that originate from the extended gauge sector. In this paper, after a discussion of the detailed structure of this model, we present a broad survey of the collider phenomenology of the large set of new fields that must necessarily arise from this setup in a simplified version involving only a single generation of fermions. We demonstrate that several new signatures may be anticipated at the LHC as well as at future hadron and lepton colliders if such models are realized in nature.