The residual resistivity in Co/Ni superlattices is shown to oscillate
as a function of superlattice period for fixed Co to Ni thickness rati
o. Additional experimental evidence shows that this behavior is enhanc
ed when randomness is artificially introduced in the individual layer
thickness. We analyze this in terms of a scattering mechanism associat
ed with the presence of localized electron eigenstates near the Fermi
level in the metallic superlattices. A one-dimensional tight-binding c
alculation shows that localized states appear close to superlattice pe
riods for which the resistivity exhibits maxima.