论文标题

$ \ bf {mnbi_4te_7} $和$ \ bf {mnbi_6te_ {10}} $中的铁磁 - 抗磁性共存的基态和交换偏见效应

Ferromagnetic-antiferromagnetic coexisting ground states and exchange bias effects in $\bf{MnBi_4Te_7}$ and $\bf{MnBi_6Te_{10}}$

论文作者

Xu, Xiaolong, Yang, Shiqi, Wang, Huan, Guzman, Roger, Zhu, Yaozheng, Peng, Yuxuan, Zang, Zhihao, Xi, Ming, Tian, Shangjie, Li, Yanping, Lei, Hechang, Luo, Zhaochu, Yang, Jinbo, Xia, Tianlong, Zhou, Wu, Huang, Yuan, Ye, Yu

论文摘要

Natural superlattice structures $\rm{(MnBi_2Te_4)(Bi_2Te_3)}$$_n$ ($n$ = 1, 2,...), in which magnetic $\rm{MnBi_2Te_4}$ layers are separated by nonmagnetic $\rm{Bi_2Te_3}$ layers, hold band topology, magnetism and reduced层间耦合,为实现外来拓扑量子状态提供了一个有希望的平台。然而,它们在二维极限中的磁性对于进一步探索量子现象至关重要,仍然难以捉摸。 Here, complex ferromagnetic (FM)-antiferromagnetic (AFM) coexisting ground states that persist up to the 2-septuple layers (SLs) limit are observed and comprehensively investigated in $\rm{MnBi_4Te_7}$ ($n$ = 1) and $\rm{MnBi_6Te_{10}}$ ($n$ = 2).无处不在的MN-BI位点混合改变甚至会改变微妙的SL磁相互作用的符号,从而产生空间不均匀的层间偶联。此外,在$ \ rm {(MNBI_2TE_4)(BI_2TE_3)} $$ _ n $($ n $ = 1,2)中观察到可调交换偏差效应,这是由于FM和AFM组件之间的耦合而产生的。我们的工作重点介绍了一种新的方法来进行磁性微调,并为进一步研究$ \ rm {(MNBI_2TE_4)(BI_2TE_3)} $$ _ N $($ n $ = 1,2,...)以及其磁性应用以及其磁性应用铺平了道路。

Natural superlattice structures $\rm{(MnBi_2Te_4)(Bi_2Te_3)}$$_n$ ($n$ = 1, 2,...), in which magnetic $\rm{MnBi_2Te_4}$ layers are separated by nonmagnetic $\rm{Bi_2Te_3}$ layers, hold band topology, magnetism and reduced interlayer coupling, providing a promising platform for the realization of exotic topological quantum states. However, their magnetism in the two-dimensional limit, which is crucial for further exploration of quantum phenomena, remains elusive. Here, complex ferromagnetic (FM)-antiferromagnetic (AFM) coexisting ground states that persist up to the 2-septuple layers (SLs) limit are observed and comprehensively investigated in $\rm{MnBi_4Te_7}$ ($n$ = 1) and $\rm{MnBi_6Te_{10}}$ ($n$ = 2). The ubiquitous Mn-Bi site mixing modifies or even changes the sign of the subtle inter-SL magnetic interactions, yielding a spatially inhomogeneous interlayer coupling. Further, a tunable exchange bias effect is observed in $\rm{(MnBi_2Te_4)(Bi_2Te_3)}$$_n$ ($n$ = 1, 2), arising from the coupling between the FM and AFM components in the ground state. Our work highlights a new approach toward the fine-tuning of magnetism and paves the way for further study of quantum phenomena in $\rm{(MnBi_2Te_4)(Bi_2Te_3)}$$_n$ ($n$ = 1, 2,...) as well as their magnetic applications.

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