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- W1970725101 abstract "We recently showed that an electron wave packet undergoes an abrupt, sideways jump $ensuremath{Delta}y$ during scattering in the presence of spin-orbit interaction. This causes the Hall effect in ferromagnets around room temperature (${R}_{s}ensuremath{propto}{ensuremath{rho}}^{2}$). The value of the side jump per collision ($ensuremath{Delta}yensuremath{approx}{10}^{ensuremath{-}10}$ m) seems the same for impurity and phonon scattering. A more complete justification of the side-jump model is given here. This model is used to derive the isothermal Nernst coefficient ${Q}_{s}^{mathrm{is}}$, giving ${Q}_{s}^{mathrm{is}}ensuremath{propto}ensuremath{rho}T$, where $ensuremath{rho}$ is the resistivity. If spin-disorder scattering is also introduced, then the Hall conductivity ${ensuremath{gamma}}_{mathrm{Hs}}$ is not affected, but the Nernst coefficient becomes ${Q}_{s}^{mathrm{is}}=ensuremath{-}T(ensuremath{alpha}+ensuremath{beta}ensuremath{rho})$. This formula agrees with the data of Kondorskii and Vasileva on Fe, Ni, Co, Gd, and Fe-Ni. The side jump is assumed to have the same value for spin disorder as for impurity or phonon scattering. The constant $ensuremath{alpha}$ is predicted to exist even in pure metals, in agreement with the above data but not with the Kondorskii theory." @default.
- W1970725101 created "2016-06-24" @default.
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- W1970725101 date "1972-03-01" @default.
- W1970725101 modified "2023-10-14" @default.
- W1970725101 title "Application of the Side-Jump Model to the Hall Effect and Nernst Effect in Ferromagnets" @default.
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- W1970725101 doi "https://doi.org/10.1103/physrevb.5.1862" @default.
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