In this paper I describe recent work, jointly with M. Geller, treating
the dynamics of electrons in semiconducting alloys, such as AlcGa1-cA
s, whose compositions, characterized by c, is a slowly varying functio
n of position: \del(c)(r)\b<<1, where b is a characteristic lattice sp
acing. The mathematical framework is provided by the so-called general
ized Wannier functions (GWF) a(n,l(r) where n and l are band and site
labels (for composite bands an additional label v is needed). The GWFs
are generalizations to non-periodic systems of the traditional Wannie
r functions for periodic systems. We show that the eigenstates and fre
quency-dependent electric response functions can be completely describ
ed in terms of two quantities, epsilon(n)(k;C) and p(nm),(k;c), the en
ergy and momentum matrix elements of the uniform alloys of concentrati
ons c, ranging over the values of c in the non-uniform system under co
nsideration.