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Modified Tri-bimaximal neutrino mixing confronted by JUNO $θ_{12}$ measurement

Xiao-Gang He

Abstract

The JUNO collaboration has released its first measurement of reactor neutrino oscillations results, obtaining $\sin^2θ_{12} = 0.3092\pm 0.0087$, an improvement in precision by a factor of 1.6 over previous combined results. We confront the minimally modified tri-bimaximal mixing pattern with the new data. Before the measurement of a non-zero $θ_{13}$ mixing angle, the tri-bimximal mixing pattern is one of the most popular simple mixing scheme for neutrinos. Modifications have been proposed to keep some features of tri-bimaximal mixing and make it to be consistent with data. Minimal modifications preserving one column of the tri-bimaximal mixing matrix, yielding three patterns: a) unchanged third, b) unchanged second and c) unchanged first column. Pattern a) is excluded since it keeps $θ_{13}=0$. Pattern b) predicts $V_{e2} = 1/\sqrt{3}$ and specific CP phase correlations, but JUNO's smaller $|V_{e2}|$ disfavors it at more than 3.5$σ$. Pattern c), predicting $V_{e2} = \cosτ/\sqrt{3}$, can be in agreement with current data within 1$σ$, and implies $\sin^2θ_{12} = (1-3\sin^2θ_{13})/3(1-\sin^2θ_{13})$ and CP violating quantity $\sin θ= \pm 0.998$. The negative sign favors the inverted neutrino mass hierarchy. Upcoming experiments can further test this scenario.

Modified Tri-bimaximal neutrino mixing confronted by JUNO $θ_{12}$ measurement

Abstract

The JUNO collaboration has released its first measurement of reactor neutrino oscillations results, obtaining , an improvement in precision by a factor of 1.6 over previous combined results. We confront the minimally modified tri-bimaximal mixing pattern with the new data. Before the measurement of a non-zero mixing angle, the tri-bimximal mixing pattern is one of the most popular simple mixing scheme for neutrinos. Modifications have been proposed to keep some features of tri-bimaximal mixing and make it to be consistent with data. Minimal modifications preserving one column of the tri-bimaximal mixing matrix, yielding three patterns: a) unchanged third, b) unchanged second and c) unchanged first column. Pattern a) is excluded since it keeps . Pattern b) predicts and specific CP phase correlations, but JUNO's smaller disfavors it at more than 3.5. Pattern c), predicting , can be in agreement with current data within 1, and implies and CP violating quantity . The negative sign favors the inverted neutrino mass hierarchy. Upcoming experiments can further test this scenario.

Paper Structure

This paper contains 1 section, 9 equations.

Table of Contents

  1. Acknowledgments