Motivated by current interest in disordered systems of interacting electrons,
the effectiveness of the geometrically averaged density of states,
ρg(ω), as an order parameter for the Anderson transition is
examined. In the context of finite-size systems we examine complications which
arise from finite energy resolution. Furthermore we demonstrate that even in
infinite systems a decline in ρg(ω) with increasing disorder
strength is not uniquely associated with localization.Comment: 8 pages, 8 figures; revised text and figure