Phenomenology of Vanishing Effective Majorana Mass with a Sterile Neutrino under Cosmological and JUNO Constraints
Rushi Chambyal, Tapender, Labh Singh, Surender Verma
TLDR
This paper investigates how a sterile neutrino can lead to a vanishing effective Majorana mass, constrained by cosmology and JUNO data.
Key contributions
- Explores vanishing effective Majorana mass ($M_{ee}$) in a 3+1 neutrino framework.
- Identifies parameter space for $M_{ee}$ cancellation due to active-sterile destructive interference.
- Cosmological bounds on $\sum m_i$ restrict sterile mixing $\theta_{14}$ and lightest active neutrino mass.
- JUNO data on solar parameters may not constrain $\theta_{14}$ due to new CP-violating phase cancellations.
Why it matters
Understanding vanishing Majorana mass is crucial for neutrinoless double beta decay experiments, which seek to determine if neutrinos are their own antiparticles. This work integrates new cosmological and experimental data, offering refined constraints on neutrino properties and sterile neutrino mixing, impacting future searches for new physics.
Original Abstract
In the present work we investigate the phenomenological implications of a vanishing effective Majorana neutrino mass within a $3+1$ neutrino framework adding a eV-scale sterile neutrino beside three active neutrino states in light of latest cosmology driven bounds on sum of neutrino masses ($\sum_{i}m_i$). We explore the parameter space where the destructive interference between active and sterile states leads to vanishing amplitude, $M_{ee}$, of neutrinoless double beta ($0νββ$) decay. The allowed parameter space has been identified and predictions have been obtained taking into account the latest Planck and DESI+CMB bound on $\sum_{i}m_i$. We find that these bounds restrict the sterile mixing angle $θ_{14}$ and the lightest active neutrino mass. Furthermore, we incorporate the refined precision data from JUNO experiment regarding solar oscillation parameters ($θ_{12}, Δm_{21}^2$). We find that the sterile neutrino parameters like $θ_{14}$ may not be sensitive to the JUNO precision measurements as the constraint imposed by precise $θ_{12}$ is washed out by new cancellations driven through additional CP violating phases leading to vanishing $|M_{ee}|$.
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