| CONDENSED MATTER: ELECTRONIC STRUCTURE, ELECTRICAL, MAGNETIC, AND OPTICAL PROPERTIES |
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Structural Determination, Unstable Antiferromagnetism and Transport Properties of Fe-Kagome Y$_{0.5}$Fe$_{3}$Sn$_{3}$ Single Crystals |
| Yang Liu1,2,3, Meng Lyu3, Junyan Liu3, Shen Zhang3,4, Jinying Yang3,4, Zhiwei Du5, Binbin Wang3, Hongxiang Wei3, and Enke Liu1,3* |
1School of Rare Earths, University of Science and Technology of China, Hefei 230026, China
2Ganjiang Innovation Academy, Chinese Academy of Sciences, Ganzhou 341000, China
3Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
4School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100049, China
5Guobiao (Beijing) Testing & Certification Co., Ltd., Beijing 100088, China
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| Cite this article: |
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Yang Liu, Meng Lyu, Junyan Liu et al 2023 Chin. Phys. Lett. 40 047102 |
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Abstract Kagome materials have been studied intensively in condensed matter physics. With rich properties, various Kagome materials emerge during this process. Here, we grew single crystals of Y$_{0.5}$Fe$_{3}$Sn$_{3}$ and confirmed an YCo$_{6}$Ge$_{6}$-type Kagome-lattice structure by detailed crystal structure characterizations. This compound bears an antiferromagnetic ordering at $T_{\rm N} = 551$ K, and shows a weak ferromagnetism at low temperatures, where an anomalous Hall effect was observed, suggesting the non-zero Berry curvature. With the unstable antiferromagnetic ground state, our systematic investigations make Y$_{0.5}$Fe$_{3}$Sn$_{3}$ a potential Kagome compound for Kagome or topological physics.
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Received: 10 February 2023
Editors' Suggestion
Published: 11 March 2023
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| PACS: |
71.20.Eh
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(Rare earth metals and alloys)
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75.30.Gw
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(Magnetic anisotropy)
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75.47.-m
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(Magnetotransport phenomena; materials for magnetotransport)
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72.15.-v
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(Electronic conduction in metals and alloys)
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