This is not the first time that neutrino experiments have exhibited anomalous behaviour. In fact, as anyone who follows neutrinos will tell you, anomalous results are par for the course, giving
this insane rumour its suspenseful edge. In particular,
Graham notes again that the
recent MINOS results are confusing, with the introduction of large new systematic errors required to explain big shifts in the apparent $\Delta m^2$ for $\overline{\nu}$.
We can be inventive when considering such results. Some, for
instance, think that neutrinos are tachyonic while antineutrinos are not. Perhaps we should mix up the $(\nu, \overline{\nu})$ sets into tachyonic and ordinary subsets.
But given
Louise's cosmology, and a fixed local $c$, a natural thing to ponder is the
cosmic time variation of mass. It is important to understand that every observer has a cosmic time, that they observe most simply via their
CMB temperature. Since our cosmic epoch corresponds to a large universal mass $M$, we do not expect to detect a variation in $M$ over short laboratory time scales. But maybe the neutrino's tiny
rest mass, and hence small associated cosmic period, allows a mass
time variation to be observable on human laboratory time scales. Could the strange
MINOS results be explained by an oscillation of $\Delta m^2$ values between
the limiting $\pm \pi/12$ phases? Such a limitation on the measurement of $\Delta m^2$ would eventually be observable at a number of neutrino experiments. Note that the total mass scale for the triplet of states could be fixed, with the amplitudes for individual states coming from parameters that interpolate between the mixing matrices for neutrinos and their mirror counterparts. This would utterly confuse the measurements of $\theta_{13}$!
Does this have anything to do with tachyons?
Recall that the minus sign in the Koide rule occurs for one phase, but not for its mirror conjugate, possibly suggesting only a single tachyonic $\nu$ mass state. Alternatively, five of the six states could be tachyonic, with only one ordinary $\nu$ mass state. On Saturday, we will have many more ideas with which to play.