Abstract
We investigate effects of non-zero Dirac and Majorana CP violating phases on neutrino-antineutrino oscillations in a magnetic field of astrophysical environments. It is shown that in the presence of strong magnetic fields and dense matter, non-zero CP phases can induce new resonances in the oscillations channels $\nu_e \leftrightarrow \bar{\nu}_e$, $\nu_e \leftrightarrow \bar{\nu}_\mu$ and $\nu_e \leftrightarrow \bar{\nu}_{\tau}$. We also consider all other possible oscillation channels with $\nu_\mu$ and $\nu_\tau$ in the initial state. The resonances can potentially lead to significant phenomena in neutrino oscillations accessible for observation in experiments. In particular, we show that neutrino-antineutrino oscillations combined with Majorana-type CP violation can affect the $\bar{\nu}_e$/$\nu_e$ ratio for neutrinos coming from the supernovae explosion. This effect is more prominent for the normal neutrino mass ordering. The detection of supernovae neutrino fluxes in the future experiments, such as JUNO, DUNE and Hyper-Kamiokande, can give an insight into the nature of CP violation and, consequently, provides a tool for distinguishing the Dirac or Majorana nature of neutrinos.
Highlights
CP symmetry implies that the equations of motion of a system remain invariant under the CP transformation, that is a combination of charge conjugation (C) and parity inversion (P)
We study neutrino-antineutrino oscillations engendered by the interaction with a magnetic field in astrophysical environments and search for possible manifestations of the Majorana CP-violating phases in neutrino fluxes from supernovae
We qualitatively show below how the appearance of the new resonances affects observable neutrino fluxes
Summary
CP symmetry implies that the equations of motion of a system remain invariant under the CP transformation, that is a combination of charge conjugation (C) and parity inversion (P). 0 01 where δ is the Dirac CP-violating phase, the additional phases α1 and α2 are the so-called Majorana CP-violating phases, which can be nonzero only for the case of Majorana neutrinos, and cik 1⁄4 cos θik and sik 1⁄4 sin θik As it was shown in [12,13], it is impossible to observe the Majorana CP phases in the neutrino flavor oscillations (see [14,15] for a recent discussion). In [16] the authors stated that in principle it is possible to measure Majorana CP phases in neutrino-antineutrino oscillations due to tiny effects of nonzero neutrino masses. We study neutrino-antineutrino oscillations engendered by the interaction with a magnetic field in astrophysical environments and search for possible manifestations of the Majorana CP-violating phases in neutrino fluxes from supernovae.
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