  We study ground state and finite temperature properties of disordered heavy
fermion metals by using a generalization of dynamical mean field theory which
incorporates Anderson localization effects. The emergence of a non-Fermi liquid
metallic behavior even at moderate disorder is shown to be a universal
phenomenon resulting from local density of states fluctuations. This behavior
is found to have a character of an electronic Griffiths phase, and can be
thought of as a precursor of Anderson localization in a strongly correlated
host. The temperature dependence of the conducting properties of the system
reveal a non-trivial interplay between disorder and inelastic processes, which
is reminiscent of the Mooij correlations observed in many disordered metals.
