The conductivity of a magnetic nanocontact with a spin inhomogeneity in the
form of a Ginzburg-Bulaevskii domain wall at the center between oppositely
magnetized edges is considered. The conductivity of the nanocontact is cal
culated in the ballistic approximation for Fe, Co, and Ni in the low-temper
ature limit, with allowance made for the spatial major-minor change in the
electron spin energy due to exchange splitting in the edges. The calculatio
ns are carried out for the limiting cases of long and short nanocontacts. I
t is shown that the domain wall formed in a nanocontact causes considerable
quantitative and qualitative changes in the dependence of the conductivity
on the channel width. (C) 2000 MAIK "Nauka/Interperiodica".