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Magnon-assisted transport and thermopower in ferromagnet-normal metal tunnel junctions

arXiv:cond-mat/0302485 · doi:10.1103/PhysRevB.68.172404

Abstract

We develop a theoretical model of magnon-assisted transport in a mesoscopic tunnel junction between a ferromagnetic metal and a normal (non-magnetic) metal. The current response to a bias voltage is dominated by the contribution of elastic processes rather than magnon-assisted processes and the degree of spin polarization of the current, parameterized by a function $P (Π_{\uparrow (\downarrow)},Π_{N})$, $0 \leq P \leq 1$, depends on the relative sizes of the majority $Π_{\uparrow}$ and minority $Π_{\downarrow}$ band Fermi surface in the ferromagnet and of the Fermi surface of the normal metal $Π_{N}$. On the other hand, magnon-assisted tunneling gives the dominant contribution to the current response to a temperature difference across the junction. The resulting thermopower is large, $S \sim - (k_B/e) (k_BT/ω_{D})^{3/2} P (Π_{\uparrow (\downarrow)},Π_{N})$, where the temperature dependent factor $(k_{B}T/ω_{D})^{3/2}$ reflects the fractional change in the net magnetization of the ferromagnet due to thermal magnons at temperature $T$ (Bloch's $T^{3/2}$ law) and $ω_{D}$ is the magnon Debye energy.

7 pages, 2 eps figures