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Current-driven magnetization switching in ferromagnetic bulk Rashba semiconductor (GeMn)Te

机译:铁磁体Rashba半导体(GeMn)Te中的电流驱动磁化切换

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摘要

Multiferroic materials with both ferroelectric and ferromagnetic orders provide a promising arena for the electrical manipulation of magnetization through the mutual correlation between those ferroic orders. Such a concept of multiferroics may expand to semiconductor with both broken symmetries of spatial inversion and time reversal, that is, polar ferromagnetic semiconductors. Here, we report the observation of current-driven magnetization switching in one such example, (Ge,Mn)Te thin films. The ferromagnetism caused by Mn doping opens an exchange gap in original massless Dirac band of the polar semiconductor GeTe with Rashba-type spin-split bands. The anomalous Hall conductivity is enhanced with increasing hole carrier density, indicating that the contribution of the Berry phase is maximized as the Fermi level approaches the exchange gap. By means of pulse-current injection, the electrical switching of the magnetization is observed in the (Ge,Mn)Te thin films as thick as 200 nm, pointing to the Rashba-Edelstein effect of bulk origin. The efficiency of this effect strongly depends on the Fermi-level position owing to the efficient spin accumulation at around the gap. The magnetic bulk Rashba system will be a promising platform for exploring the functional correlations among electric polarization, magnetization, and current.
机译:具有铁电序和铁磁序的多铁性材料通过这些铁序之间的相互关系,为磁化的电操纵提供了广阔的舞台。这种多铁性的概念可以扩展到具有空间反转和时间反转的对称性破损的半导体,即极性铁磁半导体。在这里,我们报告了在一个这样的示例(Ge,Mn)Te薄膜中电流驱动的磁化切换的观察结果。 Mn掺杂引起的铁磁性在具有Rashba型自旋分裂带的极性半导体GeTe的原始无质量Dirac带中打开了一个交换间隙。随着空穴载流子密度的增加,霍尔电导率异常增加,表明当费米能级接近交换间隙时,贝里相的贡献最大。通过脉冲电流注入,在厚达200 nm的(Ge,Mn)Te薄膜中观察到了磁化强度的电转换,这表明了大量起源的Rashba-Edelstein效应。由于在间隙周围的有效自旋积累,该效应的效率在很大程度上取决于费米能级位置。磁散装Rashba系统将是探索极化,磁化和电流之间功能关系的有前途的平台。

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