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Theory of the spin Seebeck effect influenced by crystal-field excitations in Tb$$_3$$Fe$$_5$$O$$_{12}$$

Mori, Michiyasu  ; Tomasello, B.*; Ziman, T.*

The spin Seebeck effect (SSE) is a phenomenon of thermoelectric generation that occurs within a device consisting of a bilayer of a metal and a ferromagnet. When Tb$$_3$$Fe$$_5$$O$$_{12}$$ (TbIG) is substituted for the ferromagnet, the effect goes to zero at low temperatures, yet it increases to positive values with the application of a magnetic field. This is opposite to the expectation that the SSE should be suppressed by a magnetic field due to the increase in ${the}$ magnon gap. In this paper, the crystal-field excitations (CFE) in TbIG are calculated within a mean field theory exploiting the parameters of Terbium Gallium Garnet Tb$$_3$$Fe$$_5$$O$$_{12}$$ (TGG) from the neutron-scattering experimental literature. Like TGG, the primitive cell of TbIG hosts twelve Tb sites with six inequivalent magnetic sublattices, but due to the net $$[111]$$-molecular field from the tetrahedral and octahedral Fe ions, these can be classified into two distinct groups, the $$mathbf{C}$$ and the $$mathbf{C'}$$ sites, which account for the "double umbrella" magnetic structure. We show that when an external magnetic field is applied along the [111] direction of the crystal, the lowest CFE of the $$mathbf{C}$$ sublattices decreases. As a consequence of the magnetic field dependence of the lowest CFE, we find that at low temperatures the SSE in TbIG can result enhanced by an applied magnetic field.

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