A Model of Neutrino Masses and Mixing from Hierarchy and Symmetry

Abstract

We construct a model that allows us to determine the three neutrino masses directly from the experimental mass squared differences, ${\Delta }_{\mathrm{atm}}$ and ${\Delta }_{\mathrm{sol}}$, together with the assumption that $\Lambda =\surd (1/6)=\surd (m_2/m_3)$. The parameter, $\Lambda$, basically a Clebsch-Gordan coefficient with the value of about 0.4 stems from the group $S_3$, and is NOT an expansion parameter, in contrast with the Wolfenstein parameter, $0.22<\lambda <0.25$ needed to explain quark masses. For a variety of initial values of ${\Delta }_{\mathrm{atm}}$, we find that the lowest mass, $m_1$, varies from $1.4-3.610^{-3}eV$, the next lowest mass, $m_2$ varies only slightly from $8.4-9.010^{-3}eV$, and the heaviest mass, $m_3$, ranges from $5.0-5.410^{-2}eV$. The elements of the mixing matrix, $U$, and of the mass matrix, $M$, are examined with particular emphasis on the role of small angle ${\theta }_{13}$. The phase, $\delta$, of the mixing matrix $U$ has a serious effect in the mass matrix only for the matrix elements $M_{e\mu }$ and $M_{e\tau }$, because these are the only ones for which the real part vanishes in the allowed range for ${\theta }_{13}$. Their dependence on $s_{13}$ for various values of $\delta$ is given explicitly. We study the elements of the mass matrix, $M$, for our solution 1, that of the perfect rational hierarchy, for the case $\delta =0$, and find that all of them are smaller than $0.03eV$. The only candidates for double texture zero models are $M_{ee}$ and $M_{e\mu }=M_{\mu e}$.

Added explanatory paragraph - page8, removed several sentences, added acknowledgment, corrected typos