arXiv:2510.13834v1 Announce Type: new
Abstract: This paper investigates how the gauge group $text{SU}_{I}(2) times text{U}_{Y}(1)$ of the electroweak interactions can be derived using recent geometric techniques within the real Clifford Algebra $mathbb{R}_4 = text{Cl}_4(mathbb{R})$. Central to this approach is a novel procedure for constructing the spinor space of $mathbb{R}_4$ directly, emph{without} complexification. We show that $mathbb{R}_4$ naturally accommodates representations for the $text{SU}_{I}(2) times text{U}_{Y}(1)$ gauge bosons and a single generation of chiral Standard Model leptons, with weak isospin acting exclusively on left-chiral states.
Specifically, under hypercharge and isospin $(Y, I_3)$, $mathbb{R}_4$ contains $(-1, mp tfrac{1}{2})$ irreps for left-chiral electrons and neutrinos, a $(-2, 0)$ irrep for a right-chiral electron, and a $(0, 0)$ irrep for a sterile right-chiral neutrino. The distinction between left- and right-chiral particles arises from the grade parity of the irreps, providing a natural geometric explanation for why only left-chiral particles couple to $text{SU}_{I}(2)$.
The emergence of the correct eigenvalues directly from first principles highlights the promise of this framework for the geometric foundations of Electroweak Theory and the Standard Model, as well as for Grand Unified Theories more broadly. This paper is the first panel of the Lepton Triptych, which will ultimately present the full Yang-Mills theory of the electroweak model based on these principles.