Papers
Topics
Authors
Recent
Detailed Answer
Quick Answer
Concise responses based on abstracts only
Detailed Answer
Well-researched responses based on abstracts and relevant paper content.
Custom Instructions Pro
Preferences or requirements that you'd like Emergent Mind to consider when generating responses
Gemini 2.5 Flash
Gemini 2.5 Flash 72 tok/s
Gemini 2.5 Pro 57 tok/s Pro
GPT-5 Medium 43 tok/s Pro
GPT-5 High 23 tok/s Pro
GPT-4o 107 tok/s Pro
Kimi K2 219 tok/s Pro
GPT OSS 120B 465 tok/s Pro
Claude Sonnet 4 39 tok/s Pro
2000 character limit reached

Ameliorating the popular lepton mixings with A4 symmetry: A see-saw model for realistic neutrino masses and mixing (1711.03510v3)

Published 9 Nov 2017 in hep-ph and hep-ex

Abstract: A model for neutrino masses and mixing is devised appointing the see-saw mechanism. The proffered model is fabricated with a combination of Type -I and Type-II see-saw contributions of which the latter dominates. The scalars and the leptons in the model are assigned $A4$ charges conducive to obtain the mass matrices viable for the scheme. The Type -II see-saw mass matrix accommodates atmospheric mass splitting and maximal mixing in the atmospheric sector ($\theta_{23}=\pi/4$). It is characterized by vanishing solar mass splitting and $\theta_{13}$ whereas the third neutrino mixing angle is free to acquire any value of $\theta_{12}0$. Particular alternatives of $\theta_{12}0$ corresponding to the popular lepton mixings viz. $\theta_{12}0=35.3\circ$ (tribimaximal), $45.0\circ$ (bimaximal), $31.7\circ$ (golden ratio) are accounted for. Another choice of $\theta_{12}0=0\circ$ (no solar mixing) is reckoned. The subdominant Type-I see-saw constituent of the model propels all the neutrino oscillation parameters into the ranges allowed by the data which in its turn get interrelated owing to their common origin. This makes the model testable in the light of future experimental data. As an example, $\theta_{23}$ emerges in the first (second) octant for normal (inverted) ordering. CP-violation is governed by phases present in the right-handed Majorana neutrino mass matrix, $M_{\nu R}$. Only normal ordering is allowed if these phases are absent. If $M_{\nu R}$ is complex the Dirac CP-violating phase $\delta$, is capable of being large, i.e., $\sim \pm \pi/2$, and inverted ordering of neutrino masses is also permitted. T2K and NOVA preliminary data favouring normal ordering and $\delta \sim -\pi/2$ predicts lightest neutrino mass to be 0.05 eV or more within the framework of this model.

List To Do Tasks Checklist Streamline Icon: https://streamlinehq.com

Collections

Sign up for free to add this paper to one or more collections.

Summary

We haven't generated a summary for this paper yet.

Dice Question Streamline Icon: https://streamlinehq.com

Follow-Up Questions

We haven't generated follow-up questions for this paper yet.

Authors (1)