We investigate the effects of a finite chemical potential FL in QCD vi
ewed as a disordered medium. In the quenched approximation, A(4) = i m
u induces a complex electric Aharonov-Bohm effect that causes the diag
onal contribution to the quark return probability to vanish at mu = m(
pi)/2 (half the pion mass). In two-color QCD, the weak-localization co
ntribution to the quark return probability remains unaffected causing
a mutation in the spectral statistics. In full QCD, the complex electr
ic flux is screened and the light quarks are shown to diffuse asymmetr
ically with a substantial decrease in the conductivity along the 'spat
ial' directions. Mean-field arguments suggest that a d = 1 percolation
transition may take place in the range 1.5 rho(o) < rho < 3 rho(o), w
here rho(o) is nuclear matter density. (C) 1998 Elsevier Science B.V.
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