Your questions here showed your continued misunderstanding of the concept of "quasiparticles", because you are still thinking that these are actual "objects". this is incorrect, and other than suggesting that you look again at Landau's Fermi Liquid model, I don't know what else to do.
Spin-charge separation, or in general,
fractionalization, occurs in "exotic" situation, such as 1D quantum wires or when quasiparticles have to go through a constriction, where there is a confinement. We don't measure or detect such individual quasiparticles, the way you are implying in many of your questions. That would be silly, because the whole concept of quasiparticles does not exist when we pull individual particles out of its many-body interactions.
Instead, we detect the evidence of fractionalization via several different signatures. We could, for example, detect a violation of the Wiedermann-Franz law that indicates that the thermal conductivity is different than the electrical conductivity. Or we could map out the dispersion of the spin currents and the charge currents, which was done for 1D Luttinger liquids.
Never in any of these were there any consideration of "an electron" or "a particle". In basic QM, one can say the analogue statement that in such a system, an "electron" is no longer a good quantum number.
I stumbled upon this document when I was looking for something to cite. It appears to be a term paper of some sort, but it has the necessary description and references. You should have discovered this if you did a similar search on spin-charge separation.
http://guava.physics.uiuc.edu/~nigel/courses/569/Essays_Fall2010/Files/Schubel.pdf
Zz.