Yukawaon Model with U(3)$\times$O(3) Family Symmetries

TL;DR

This paper proposes a yukawaon model with U(3)×O(3) family symmetries to explain quark and lepton masses, allowing for a lower cutoff scale and providing a structured approach to neutrino mass matrices.

Contribution

It introduces a novel yukawaon model with combined U(3) and O(3) symmetries, enabling a reduced cutoff scale and specific mass matrix formulations.

Findings

Neutrino mass matrix expressed as M_ν = m_D M_R^{-1} m_D^T.

Charged lepton mass matrix given by M_e = k <Φ_e><Φ_e^T>.

Lowered cutoff scale in the yukawaon model due to symmetry choice.

Abstract

A quark and lepton mass matrix model with family symmetries U(3)$\times$O(3) is investigated on the basis of the so-called yukawaon model. In the present model, quarks and leptons are assigned to $(\ell, e^c, u^c) \sim ({\bf 3}, {\bf 3}, {\bf 3}^*)$ of U(3) and $(q, d^c, \nu^c) \sim ({\bf 3}, {\bf 3}, {\bf 3})$ of O(3). Then, the neutrino mass matrix is given by $M_\nu = m_D M_R^{-1} m_D^T$ with $m_D \propto < \Phi_e > $, where the charged lepton mass matrix $M_e$ is given by $M_e = k < \Phi_e ><\Phi_e^T >$. A merit in considering U(3)$\times$O(3) lies in that we can lower the cutoff scale $\Lambda$ in the yukawaon model.