“…1. Deformed Lorentz symmetry models [17,18,19,20,21,22,23] where the dispersion relations change from the usual p 2 = m 2 form to a different form which is still covariant under the modified Lorentz transformations. In this picture the processes which are forbidden in one reference frame (like the rest frame of the massive neutrinos) will be forbidden also in the lab frame.…”