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arXiv 2201.11568cond-mat.mes-hallcond-mat.mtrl-scicond-mat.str-el
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磁性Weyl半金属中动量空间Berry相引起的自旋动电力

Spin motive force by the momentum-space Berry phase in magnetic Weyl semimetals

Akira Harada, Hiroaki Ishizuka

AI总结:

本文揭示磁性Weyl半金属中磁进动通过动量空间Berry相产生无磁化梯度的自旋动电力,展示拓扑电子态与磁动力学的非平凡耦合。

摘要:

我们证明,在非中心对称磁性Weyl半金属中,铁磁矩的磁进动通过一种类似于绝热电荷泵浦的机制感应出电流。该电流是进动引起Weyl节点圆周运动所产生的动量空间Berry相的结果。此机制类似于法拉第效应,即环形电流感应出磁场。Weyl节点的圆周运动在动量空间中感应出磁荷流,从而产生描述绝热泵浦的Berry相。实验上,这一现象类似于自旋动电力,即在存在磁化空间梯度时由磁进动感应出的电流。然而,与传统自旋动电力不同,这种电流在无磁化梯度的情况下也会出现。该结果展示了拓扑电子态与磁动力学之间非平凡的相互作用。

英文摘要:

We show that the magnetic precession of ferromagnetic moments in a noncentrosymmetric magnetic Weyl semimetal induces an electric current through a mechanism analogous to the adiabatic charge pumping. The current is a consequence of a Berry phase in the momentum space resulting from the circular motion of Weyl nodes induced by the precession. This mechanism resembles the Faraday effect, namely, induced magnetic field by circular electric current. The circular motion of Weyl nodes induces magnetic charge current in the momentum space, which results in a Berry phase that describes the adiabatic pump. Experimentally, this phenomenon is similar to spin motive force, which is an electric current induced by magnetic precision in the presence of the spatial gradient of magnetization. However, unlike the conventional spin motive force, this current occurs without a magnetization gradient. The result demonstrates a nontrivial interplay between the topological electronic state and magnetic dynamics.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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