A Ward-Takahashi identity, as a consequence of gauge invariance and in
a form that relates self-energy to the two-particle Bethe-Salpeter sc
attering kernel, was first derived by Vollhardt and Wolfle for a syste
m of independent particles moving in a random medium. This is generali
zed to a class of interacting electronic systems in materials with or
without random impurities, following a procedure previously used for c
lassical wave transport in disordered media. This class of systems als
o possesses other symmetry properties such as invariance under time tr
anslations and local spin rotations, which imply local conservation la
ws for energy and spin current. They imply additional Vollhardt-Wolfle
type identities. We present non-perturbative derivations of these ide
ntities, and consider the constraints they impose on the relationship
between the self-energy and the two-particle scattering kernel. (C) 19
98 Published by Elsevier Science B.V.