I'm hesitant to mention this, especially since I don't think this is the scope that is relevant here, and also because this is in the classical physics forum. But since people have already brought up "hypercharge" and QED, I suppose then it is fair game now.
If you look at the Luttinger Liquid theory for 1D conductors, even under the smallest many-body coupling, a very interesting phenomenon has been predicted. The Landau Fermi Liquid quasiparticle (in an ordinary conductor, this quasiparticle is our renormalized electron) undergoes a "fractionalization", whereby the spin and charge are no longer "good quantum numbers". In fact, spin-charge separation is predicted[1]. This is where the spin and charge transport moves almost independently of each other. If you look at the dispersion curve for each one of them, they have no longer on top of each other, but disperses differently. For many, this signifies that the unit "carrier" in such a system has fractionalize - the spin and charge moves separately.
There are several indications that this may have been observed. The violation of the Wiedemann-Franz law in several different systems[2] has been attributed to such spin-charge separation.
Edit: I just realized that the point that I'm making with regards to the topic of this thread (mass and charge) didn't get made. (That'll teach me to post something in a hurry.) The point here is that these "observables", such as mass, spin, and charge, may, under certain circumstances, be "separated". Since we have seen spin and charge separation, I wouldn't be surprised that mass and charge might be separable as well. We haven't seen the latter yet, of course, since in most of these condensed matter systems, mass isn't that interesting yet. But if we can renormalize such masses, especially with the Fermi liquid system, via the effective mass from band structure, there's nothing here to indicate that such fractionialization can't occur with mass and charge.
Zz.
[1] T. Lorenz et al. Nature v.418, p.614 (2002).
[2] G.Z. Liu and G. Cheng, PRB v.66, p.100505.1 (2002).