Abstract
In the literature on the $s$-$d$ model for the magnetization dynamics in systems without and with spin-polarized transport currents, it is generally assumed that the adiabatic part of the $s$-electron magnetization is everywhere parallel to the $d$-electron magnetization. We present model calculations within the ab initio spin-density functional theory which suggest that this assumption is not valid for systems with strongly noncollinear magnetization configurations.
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