The resistivity data of Fe-based ternary alloys has been reevaluated t
aking into account that the conduction electrons in Fe are predominant
ly highly polarized (approximately 95%) d-like electrons. This drastic
ally changes the previously derived values of solute cross sections an
d scattering rate ratios of the majority and minority conduction elect
rons. It further removes the perplexing result of previous analyses th
at the spin-up and spin-down cross sections of sp solute atoms were no
t equal but varied by about a factor of 7. These cross sections should
be equal since the nonmagnetic sp electrons cause only a charge pertu
rbation. The vastly different cross-section ratios from those previous
ly obtained cast doubt on the proposed explanation of the giant magnet
oresistance effect as being due to spin-dependent scattering from solu
te or interface atoms. A more plausible explanation of the large magne
toresistance at low fields for both pure Fe and its layered structures
is that it is caused by the large scattering at antiparallel magnetic
boundaries due to the high polarization of the conduction electrons.
Moreover, since past analyses of scattering, transport effects, etc. i
n 3d ferromagnetics have assumed that the conduction electrons are sp-
like, all of these results should also be critically reexamined to det
ermine their validity.