Microscopic Theory of Magnon-Drag Thermoelectric Transport in Ferromagnetic Metals

Microscopic Theory of Magnon-Drag Thermoelectric Transport in Ferromagnetic Metals
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铁磁金属中磁振阻力热电输运的微观理论

DOI:
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发表时间:
2012
期刊:
影响因子:
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通讯作者:
A. Sakuma
A. Sakuma
中科院分区:
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文献类型:
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作者:
D. Miura;A. Sakuma

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本文从理论上研究了铁磁金属中的磁振子拖曳Peltier效应和Seebeck效应。一个磁振子热流描述微扰从微观角度来看,相对于电子-磁振子相互作用和电场。然后,获得磁振子阻力Peltier系数$Pi_MAG$作为磁振子热流和电荷电流之间的比率。我们证明了在低温T$下$Pi_MAG=C_MAG T^{5/2}$,系数C_MAG$与电导率的自旋极化$P$成正比,并且当$C_MAG 0$时$P>0$。从磁振子拖曳Peltier效应的实验结果,我们估计的电子-磁振子相互作用的强度约为0.3 eV$cdotAA^{3/2}$坡莫合金。
A theoretical study of the magnon-drag Peltier and Seebeck effects in ferromagnetic metals is presented. A magnon heat current is described perturbatively from the microscopic viewpoint with respect to electron--magnon interactions and the electric field. Then, the magnon-drag Peltier coefficient $Pi_MAG$ is obtained as the ratio between the magnon heat current and the electric charge current. We show that $Pi_MAG=C_MAG T^{5/2}$ at a low temperature $T$; that the coefficient $C_MAG$ is proportional to the spin polarization $P$ of the electric conductivity; and that $P>0$ for $C_MAG 0$. From experimental results for magnon-drag Peltier effects, we estimate that the strength of the electron--magnon interaction is about 0.3 eV$cdotAA^{3/2}$ for permalloy.