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arXiv 2211.00546cond-mat.mtrl-sci
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含自组织 MnBi$_{2}$Te$_{4}$ 七层层的磁性拓扑绝缘体 Bi$_{2}$Te$_{3}$ 和 BiSbTe$_{3}$ 中磁性和磁输运的费米能级依赖性

Fermi level dependence of magnetism and magnetotransport in the magnetic topological insulators Bi$_{2}$Te$_{3}$ and BiSbTe$_{3}$ containing self-organized MnBi$_{2}$Te$_{4}$ septuple layers

J. Sitnicka, M. Konczykowski, K. Sobczak, P. Skupiński, K. Grasza, Z. Adamus, A. Reszka, A. Wołoś

AI总结:

本研究利用电子辐照调节含MnBi$_{2}$Te$_{4}$七层层的磁性拓扑绝缘体的费米能级,发现费米能级位置不影响磁各向异性场和居里温度,排除了载流子介导的体态磁性,并证实反常霍尔效应由Berry相位驱动且可通过调节费米能级有效控制。

摘要:

磁性掺杂拓扑绝缘体中支撑铁磁性和磁输运现象的磁耦合机制,一直是实现对量子反常霍尔效应和拓扑轴子绝缘态等磁拓扑现象进行受控研究的核心问题。在此,我们关注体态载流子在磁性拓扑绝缘体族磁学性质中的作用,该系列材料的基质为 Bi$_{2}$Te$_{3}$ 或 BiSbTe$_{3}$,其中自组织形成的 Mn 构成了 MnBi$_{2}$Te$_{4}$ 七层层状结构。我们利用电子辐照技术调节费米能级,研究磁性性质如何随载流子密度的变化而改变,并讨论了辐照缺陷的作用。铁磁共振光谱和磁输运测量分别表明,费米能级位置对磁各向异性场和居里温度没有影响,从而排除了基于载流子介导过程的体态磁性。此外,磁输运测量显示,反常霍尔效应由内在且无耗散的 Berry 相位驱动机制主导,由于 Berry 曲率集中在避免能带交叉点附近,霍尔电阻率在导带底或价带顶附近得到增强。这些结果表明,通过调节费米能级,可以有效地控制、最大化或关闭反常霍尔效应。

英文摘要:

The magnetic coupling mechanisms underlying ferromagnetism and magnetotransport phenomena in magnetically doped topological insulators have been a central issue to gain controlled access to the magneto-topological phenomena such as quantum anomalous Hall effect and topological axion insulating state. Here, we focus on the role of bulk carriers in magnetism of the family of magnetic topological insulators, in which the host material is either Bi$_{2}$Te$_{3}$ or BiSbTe$_{3}$, containing Mn self-organized in MnBi$_{2}$Te$_{4}$ septuple layers. We tune the Fermi level using the electron irradiation technique and study how magnetic properties vary through the change in carrier density, the role of the irradiation defects is also discussed. Ferromagnetic resonance spectroscopy and magnetotransport measurements show no effect of the Fermi level position on the magnetic anisotropy field and the Curie temperature, respectively, excluding bulk magnetism based on a carrier-mediated process. Furthermore, the magnetotransport measurements show that the anomalous Hall effect is dominated by the intrinsic and dissipationless Berry-phase driven mechanism, with the Hall resistivity enhanced near the bottom/top of the conduction/valence band, due to the Berry curvature which is concentrated near the avoided band crossings. These results demonstrate that the anomalous Hall effect can be effectively managed, maximized, or turned off, by adjusting the Fermi level.

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