The mass and weak eigenstates are related by the Pontecorvo-Maki–Nakagawa–Sakata matrix, which is a $3\times 3$ unitary matrix. Therefore, it can be parametrized by four parameters. The usual choice is the three mixing angles $\theta_{12}$, $\theta_{13}$ and $\theta_{23}$, and a CP-violating phase $\delta_{CP}$ (or, if neutrinos are Majorana fermions, 3 different CP-violating phases). Oscillation experiments provide information about the mixing angles, but not the phase.
Note that oscillation observation is not sensitive to neutrino masses, only to the square of the difference of neutrino masses. Therefore, it could be possible that only two of the three neutrino flavours have non-zero mass.
The consequences of the existence of the CP-violating phase are
- In a difference between the oscillation $\nu_\alpha\to \nu_\beta$ and $\bar{\nu}_\alpha \to \bar{\nu}_\beta$ (and also $\nu_\beta\to \nu_\alpha$, if CPT symmetry is conserved).
- A non-zero contribution to the electric dipole of charged leptons. Nevertheless, this effect is "neglibly small and unaccesible to experiments".
- If neutrinos are Majorana fermions, the spectrum of the neutrinoless double beta decay might be sensitive to Majorana CP-violating phases.
References:
- K. Nakamura and S. T. Petcov: Neutrino mass, mixing and oscillations. Particle Data Group (Link to pdf)
- G. C. Branco, R. Gonzalez Felipe and F. R. Joaquim: Leptonic CP violation. Rev.Mod.Phys. 84 (2012) 515-565. (arXiv preprint)