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化学复杂合金中拓扑霍尔效应的观测

Observation of Topological Hall Effect in a Chemically Complex Alloy.

作者信息

Yu Jihao, Liu Yuying, Ke Yubin, Su Jiaqi, Cao Jingshan, Li Zian, Sun Baoan, Bai Haiyang, Wang Weihua

机构信息

Institute of Physics, Chinese Academy of Sciences, Beijing, 100190, China.

Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing, 100049, China.

出版信息

Adv Mater. 2024 Apr;36(15):e2308415. doi: 10.1002/adma.202308415. Epub 2024 Feb 11.

Abstract

The topological Hall effect (THE) is the transport response of chiral spin textures and thus can serve as a powerful probe for detecting and understanding these unconventional magnetic orders. So far, the THE is only observed in either noncentrosymmetric systems where spin chirality is stabilized by Dzyaloshinskii-Moriya interactions, or triangular-lattice magnets with Ruderman-Kittel-Kasuya-Yosida-type interactions. Here, a pronounced THE is observed in a Fe-Co-Ni-Mn chemically complex alloy with a simple face-centered cubic (fcc) structure across a wide range of temperatures and magnetic fields. The alloy is shown to have a strong magnetic frustration owing to the random occupation of magnetic atoms on the close-packed fcc lattice and the direct Heisenberg exchange interaction among atoms, as evidenced by the appearance of a reentrant spin glass state in the low-temperature regime and the first principles calculations. Consequently, THE is attributed to the nonvanishing spin chirality created by strong spin frustration under the external magnetic field, which is distinct from the mechanism responsible for the skyrmion systems, as well as geometrically frustrated magnets.

摘要

拓扑霍尔效应(THE)是手性自旋织构的输运响应,因此可作为探测和理解这些非常规磁序的有力探针。到目前为止,THE仅在非中心对称系统中被观测到,在该系统中自旋手性通过Dzyaloshinskii-Moriya相互作用得以稳定,或者在具有Ruderman-Kittel-Kasuya-Yosida型相互作用的三角晶格磁体中被观测到。在此,在一种具有简单面心立方(fcc)结构的Fe-Co-Ni-Mn化学复杂合金中,在很宽的温度和磁场范围内观测到了明显的THE。由于磁性原子在密排fcc晶格上的随机占据以及原子间的直接海森堡交换相互作用,该合金表现出强烈的磁阻挫,低温区出现的重入自旋玻璃态以及第一性原理计算证明了这一点。因此,THE归因于外部磁场下强自旋阻挫产生的非零自旋手性,这与导致斯格明子系统以及几何阻挫磁体的机制不同。

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