Giant magnetoresistance (GMR) effects are observed in several classes
of bulk magnetic materials. The resistance changes at metamagnetic tra
nsitions connected with reorientation of 4f moments are only moderate
due to the relatively weak coupling of the 4f and conduction electrons
. Much larger GMR effects can be achieved by mechanisms involving the
d states (RhFe, RCo(2)), though the most spectacular resistance variat
ions are connected with metamagnetic transitions in U-intermetallic an
tiferromagnets. This phenomenon can be interpreted as due to Fermi sur
face gapping (due to magnetic superzones) and/or due to spin-dependent
scattering in analogy with magnetic multilayers.