Magnetic properties of the layered magnetic topological insulator EuSn2As2

被引:15
|
作者
Li, Huijie [1 ,2 ]
Gao, Wenshuai [1 ]
Chen, Zheng [2 ,3 ]
Chu, Weiwei [2 ,3 ]
Nie, Yong [2 ,3 ]
Ma, Shuaiqi [1 ]
Han, Yuyan [2 ]
Wu, Min [2 ]
Li, Tian [2 ]
Niu, Qun [2 ]
Ning, Wei [2 ]
Zhu, Xiangde [2 ]
Tian, Mingliang [1 ,2 ,4 ]
机构
[1] Anhui Univ, Inst Phys Sci & Informat Technol, Hefei 230601, Peoples R China
[2] Chinese Acad Sci, HFIPS, High Field Magnet Lab, Anhui Key Lab Condensed Matter Phys Extreme Condi, Hefei 230031, Anhui, Peoples R China
[3] Univ Sci & Technol China, Dept Phys, Hefei 230031, Anhui, Peoples R China
[4] Anhui Univ, Sch Phys & Mat Sci, Hefei 230601, Peoples R China
关键词
This paper was supported by the National Key Research and Development Program of China; Grant No. 2016YFA0401003 and No. 2017YFA0403502; the Natural Science Foundation of China (No. U19A2093; No; U2032214; U2032163; U1732274; and No. 11904002); the Collaborative Innovation Program of Hefei Science Center; Chinese Academy of Sciences (CAS; Grant No. 2019HSC-CIP 001); the Youth Innovation Promotion Association of CAS (Grant No. 2017483); and the Natural Science Foundation of Anhui Province (No. 1908085QA15);
D O I
10.1103/PhysRevB.104.054435
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
EuSn2As2 with a layered rhombohedral crystal structure is proposed to be a candidate for an intrinsic antiferromagnetic (AFM) topological insulator. Here, we have investigated systematic magnetoresistance (MR) and magnetization measurements on the high-quality EuSn2As2 single crystal with the magnetic field both parallel and perpendicular to the (001) plane. Both the kink of magnetic susceptibility and longitudinal resistivity reveal that EuSn2As2 undergoes an AFM transition at T-N = 21 K. At T = 2 K, the magnetization exhibits two successive plateaus of similar to 5.6 and similar to 6.6 mu(B)/Eu at the corresponding critical magnetic fields. Combined with the negative longitudinal MR and abnormal Hall resistance, we demonstrate that EuSn2As2 undergoes complicated magnetic transitions from an AFM state to a canted ferromagnetic (FM) state at H-c and then to a polarized FM state at H-s as the magnetic field increases.
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页数:5
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