  Temperature dependent transport of disordered electronic systems is examined
in the presence of strong correlations. In contrast to what is assumed in Fermi
liquid approaches, finite temperature behavior in this regime proves largely
dominated by inelastic electron-electron scattering. This conclusion is valid
in the strong coupling limit, where the disorder, the correlations and the
Fermi energy are all comparable, as in many materials near the metal-insulator
transition.
