Anomalous Hall Effect and Magnetoresistance of Ferromagnetic Metals

Abstract

The anomalous Hall effect and the magnetoresistance of ferromagnetic metals are in· vestigated on the basis of the localized d·electron (or f-electron) model. First the Hamil· tonian of the interaction between conduction electrons and localized electrons is given, which is valid when the orbital angular momenta of localized electrons are not quenched. Then we find that the scattering matrix of a conduction electron depends in a complicated way on the directions of the initial and final wave vectors and of the magnetization. The transition probability calculated to the first Born approximation by using the above matrix elements leads to the electrical resistivity of the form expressed by Eq. (1. 1) in the text. To the second Born approximation we find that the transition probability from a state k to another state k 1 is not equal to that from k 1 to k and leads to the anomalous Hall effect. The magnitude and the temperature dependence of both effects are reasonable for iron and nickel when compared with experiment. In rare-earth metals, both effects can also be obtained and, besides, the electric quadrupole moments which are associated with the orbital angular momenta cause an additional scat· tering. When we calculate the normal resistivity by adding the exchange and quadrupole scatterings, we obtain a good agreement with experiment on the magnetic contribution to the resistivity of rare-earth metals with more than half-filled 4f shells