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.
Categories: hep-ph