It is known that one can find the Hall conductivity $\sigma_{xy}$ from a lattice model (in a magnetic field, say) using the TKNN formula (PRL 49 405-408 (1982)), i.e. by summing the Chern numbers for bands below the Fermi energy $E_F$: $$\sigma_{xy}=\frac{e^2}{h}\sum_{E_n<E_F}C_n$$ $C_n$ can be straightforwardly computed from the eigenstates.
If one were to cause the bands in such a model to broaden (by adding an external potential, say), could the longitudinal conductivity $\sigma_{xx}$ be computed in a straightforward way in this model?