# Effective Majorana Neutrino Mass for ΔL = 2 Neutrino Oscillations

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^{2}

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## Abstract

**:**

## 1. Introduction

## 2. Neutrino to Antineutrino Oscillation

## 3. Neutrinoless Double-Beta Decay

## 4. Results

## 5. Conclusions

## Author Contributions

## Funding

## Institutional Review Board Statement

## Informed Consent Statement

## Data Availability Statement

## Acknowledgments

## Conflicts of Interest

## References

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**Figure 1.**The effective neutrino mass as a function of the lightest neutrino mass assuming normal ordering (${m}_{1}<{m}_{2}<{m}_{3}$). The blue shaded region depicts region II, where ${m}_{\mathrm{lightest}}$ is in the range of [2.5–6] meV and ${m}_{\beta \beta}$ is obtained as zero.

**Figure 2.**The dependence of the effective neutrino mass ${m}_{\beta \beta}^{L}$ with (dashed lines) and without (solid lines) $\nu \to \overline{\nu}$ oscillation. The red and blue lines are obtained with Majorana phases corresponding to the maximum (${\varphi}_{1}=0,{\varphi}_{2}=0$) and minimum ${m}_{\beta \beta}$ (Equation (10)). Note that y-axis ranges are different in the three panels.

**Figure 3.**Dependence of ${m}_{\beta \beta}^{L}$ on lightest mass (${m}_{1}$ for NO) with Majorana phases corresponding to maximum (${\varphi}_{1}=0,{\varphi}_{2}=0$) and minimum ${m}_{\beta \beta}$ (Equation (10)) in left and right panels, respectively, with two choices of $L/E$.

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**MDPI and ACS Style**

Khatun, A.; Šimkovic, F.
Effective Majorana Neutrino Mass for Δ*L* = 2 Neutrino Oscillations. *Symmetry* **2022**, *14*, 1383.
https://doi.org/10.3390/sym14071383

**AMA Style**

Khatun A, Šimkovic F.
Effective Majorana Neutrino Mass for Δ*L* = 2 Neutrino Oscillations. *Symmetry*. 2022; 14(7):1383.
https://doi.org/10.3390/sym14071383

**Chicago/Turabian Style**

Khatun, Amina, and Fedor Šimkovic.
2022. "Effective Majorana Neutrino Mass for Δ*L* = 2 Neutrino Oscillations" *Symmetry* 14, no. 7: 1383.
https://doi.org/10.3390/sym14071383