中国物理B ›› 2021, Vol. 30 ›› Issue (7): 77502-077502.doi: 10.1088/1674-1056/ac0786
Magnetocrystalline anisotropy and dynamic spin reorientation of half-doped Nd0.5Pr0.5FeO3 single crystal
Haotian Zhai(翟浩天)1, Tian Gao(高湉)1,2,3,†, Xu Zheng(郑旭)1, Jiali Li(李佳丽)1, Bin Chen(陈斌)2, Hongliang Dong(董洪亮)2, Zhiqiang Chen(陈志强)2, Gang Zhao(赵钢)3, Shixun Cao(曹世勋)3, Chuanbing Cai(蔡传兵)3,‡, and Vyacheslav V. Marchenkov4,5
- 1 Department of Physics, Shanghai University of Electric Power, Shanghai 200090, China;
2 Center for High Pressure Science and Technology Advanced Research, Shanghai 201203, China;
3 Shanghai Key Laboratory of High Temperature Superconductors, Shanghai University, Shanghai 200444, China;
4 M. N. Mikheev Institute of Metal Physics, Ekaterinburg 620108, Russia;
5 Ural Federal University, Ekaterinburg 620002, Russia
Magnetocrystalline anisotropy and dynamic spin reorientation of half-doped Nd0.5Pr0.5FeO3 single crystal
Haotian Zhai(翟浩天)1, Tian Gao(高湉)1,2,3,†, Xu Zheng(郑旭)1, Jiali Li(李佳丽)1, Bin Chen(陈斌)2, Hongliang Dong(董洪亮)2, Zhiqiang Chen(陈志强)2, Gang Zhao(赵钢)3, Shixun Cao(曹世勋)3, Chuanbing Cai(蔡传兵)3,‡, and Vyacheslav V. Marchenkov4,5
- 1 Department of Physics, Shanghai University of Electric Power, Shanghai 200090, China;
2 Center for High Pressure Science and Technology Advanced Research, Shanghai 201203, China;
3 Shanghai Key Laboratory of High Temperature Superconductors, Shanghai University, Shanghai 200444, China;
4 M. N. Mikheev Institute of Metal Physics, Ekaterinburg 620108, Russia;
5 Ural Federal University, Ekaterinburg 620002, Russia
摘要： The single crystals of Nd$_{0.5}$Pr$_{0.5}$FeO$_{3}$ were successfully grown by optical floating zone method. Room temperature x-ray diffraction and Laue photograph declared the homogeneity and high quality of the crystal. The significant magnetic anisotropy and multiple magnetic transitions illustrate the complex magnetic structure. At high temperatures ($T > 66 $ K), it shows the typical characteristics of $\varGamma _{4}$(G$_{x}$, A$_{y}$, F$_{z}$) state. With the decrease of the temperature, it undergoes a first-order spin reorientation transition from $\varGamma _{4}$(G$_{x}$, A$_{y}$, F$_{z}$) to $\varGamma _{2}$(F$_{x}$, C$_{y}$, G$_{z}$) state in the temperature window of 45-66 K under an applied magnetic field of 0.01 T. As the temperature drops to $\sim 17 $ K, a new magnetic interaction mechanism works, which results in a further enhancement of magnetization. The ${T}$-$H$ phase diagram of Nd$_{0.5}$Pr$_{0.5}$FeO$_{3}$ single crystal was finally constructed.
中图分类号: (Magnetic oxides)
- 75.47.Lx