English

Three Generations and a Trio of Trialities

High Energy Physics - Phenomenology 2025-04-18 v2 High Energy Physics - Theory

Abstract

We identify the Standard Model's su(3)su(2)u(1)\mathfrak{su}(3)\oplus \mathfrak{su}(2)\oplus \mathfrak{u}(1) internal symmetries within the triality symmetries tri(C)tri(H)tri(O)\mathfrak{tri}(\mathbb{C}) \oplus \mathfrak{tri}(\mathbb{H}) \oplus \mathfrak{tri}(\mathbb{O}). From here, the corresponding Standard Model group action is applied to the triality triple (Ψ+,Ψ,V)\left( \Psi_+, \Psi_-,V\right) for Ψ+,Ψ,VCHO\Psi_+, \Psi_-, V \in \mathbb{C}\otimes\mathbb{H}\otimes\mathbb{O}. Together, Ψ+\Psi_+ and Ψ\Psi_- provide the correct irreducible representations for two generations. Owing to a certain Cartan Factorization, which we define, VV provides the irreducible representations for a third generation. Said more explicitly in another way, division algebraic multiplication merges a third generation of spinor representations into a set of scalar bosons. This set of scalar bosons includes the familiar Standard Model Higgs representation.

Keywords

Cite

@article{arxiv.2409.17948,
  title  = {Three Generations and a Trio of Trialities},
  author = {N. Furey and M. J. Hughes},
  journal= {arXiv preprint arXiv:2409.17948},
  year   = {2025}
}

Comments

11 pages, 6 figures