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Magnetic Structure and Metamagnetic Transitions in the van der Waals Antiferromagnet CrPS<sub>4</sub>

Yuxuan PengState Key Laboratory for Artificial Microstructure &amp; Mesoscopic Physics School of Physics Peking University Beijing 100871 P. R. ChinaShilei DingState Key Laboratory for Artificial Microstructure &amp; Mesoscopic Physics School of Physics Peking University Beijing 100871 P. R. ChinaMan ChengZhejiang Province Key Laboratory of Quantum Technology and Device Department of Physics Zhejiang University Hangzhou 310027 P. R. ChinaQifeng HuZhejiang Province Key Laboratory of Quantum Technology and Device Department of Physics Zhejiang University Hangzhou 310027 P. R. ChinaJie YangBeijing Key Laboratory for Magnetoelectric Materials and Devices Beijing 100871 P. R. ChinaFanggui WangState Key Laboratory for Artificial Microstructure &amp; Mesoscopic Physics School of Physics Peking University Beijing 100871 P. R. ChinaMingzhu XueState Key Laboratory for Artificial Microstructure &amp; Mesoscopic Physics School of Physics Peking University Beijing 100871 P. R. ChinaZhou LiuState Key Laboratory for Artificial Microstructure &amp; Mesoscopic Physics School of Physics Peking University Beijing 100871 P. R. ChinaZhongchong LinState Key Laboratory for Artificial Microstructure &amp; Mesoscopic Physics School of Physics Peking University Beijing 100871 P. R. ChinaMaxim AvdeevAustralian Nuclear Science and Technology Organisation (ANSTO) New Illawarra Road, Lucas Heights Sydney NSW 2234 AustraliaYanglong HouBeijing Key Laboratory for Magnetoelectric Materials and Devices Beijing 100871 P. R. ChinaWenyun YangState Key Laboratory for Artificial Microstructure &amp; Mesoscopic Physics School of Physics Peking University Beijing 100871 P. R. ChinaYi ZhengZhejiang Province Key Laboratory of Quantum Technology and Device Department of Physics Zhejiang University Hangzhou 310027 P. R. ChinaJinbo YangBeijing Key Laboratory for Magnetoelectric Materials and Devices Beijing 100871 P. R. China
2020en
ABI

Annotatsiya

Abstract In 2D magnets, interlayer exchange coupling is generally weak due to the van der Waals layered structure but it still plays a vital role in stabilizing the long‐range magnetic ordering and determining the magnetic properties. Using complementary neutron diffraction, magnetic, and torque measurements, the complete magnetic phase diagram of CrPS 4 crystals is determined. CrPS 4 shows an antiferromagnetic ground state (A‐type) formed by out‐of‐plane ferromagnetic monolayers with interlayer antiferromagnetic coupling along the c axis below T N = 38 K. Due to small magnetic anisotropy energy and weak interlayer coupling, the low‐field metamagnetic transitions in CrPS 4, that is, a spin‐flop transition at ≈0.7 T and a spin‐flip transition from antiferromagnetic to ferromagnetic under a relatively low field of 8 T, can be realized for H ∥ c . Intriguingly, with an inherent in‐plane lattice anisotropy, spin‐flop‐induced moment realignment in CrPS 4 for H ∥ c is parallel to the quasi‐1D chains of CrS 6 octahedra. The peculiar metamagnetic transitions and in‐plane anisotropy make few‐layer CrPS 4 flakes a fascinating platform for studying 2D magnetism and for exploring prototype device applications in spintronics and optoelectronics.

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