  We discuss the effect of disorder on the coherent propagation of the bound
state of two attracting particles. It is shown that a result analogous to the
Anderson theorem for dirty superconductors is also valid for the Cooper
problem, namely, that the pair wave function is extended beyond the
single-particle localization length if the latter is large. A physical
justification is given in terms of the Thouless block-scaling picture of
localization. These arguments are supplemented by numerical simulations. With
increasing disorder we find a transition from a regime in which the interaction
delocalizes the pair to a regime in which the interaction enhances
localization.
