Spin-transfer-torque induced spatially nonuniform switching in ferrimagnets

被引:4
|
作者
Zhang, Xue [1 ,2 ,3 ]
Xu, Zhengde [1 ,2 ,3 ]
Ren, Jie [1 ]
Qiao, Yixiao [1 ]
Fan, Weijia [4 ,5 ]
Zhu, Zhifeng [1 ,6 ]
机构
[1] ShanghaiTech Univ, Sch Informat Sci & Technol, Shanghai 201210, Peoples R China
[2] Chinese Acad Sci, Shanghai Inst Microsyst & Informat Technol, Shanghai 200050, Peoples R China
[3] Univ Chinese Acad Sci, Beijing 100049, Peoples R China
[4] Tongji Univ, Shanghai Key Lab Special Artificial Microstruct M, Shanghai 200092, Peoples R China
[5] Tongji Univ, Sch Phys Sci & Engn, Shanghai 200092, Peoples R China
[6] Shanghai Engn Res Ctr Energy Efficient & Custom A, Shanghai 201210, Peoples R China
基金
中国国家自然科学基金; 国家重点研发计划;
关键词
ANGULAR-MOMENTUM COMPENSATION; MAGNETIZATION REVERSAL; DRIVEN;
D O I
10.1063/5.0179040
中图分类号
O59 [应用物理学];
学科分类号
摘要
Ferrimagnet (FiM), (FeCo)(1-)Gd-x(x), attracts research attention due to its ultrafast magnetic dynamics and finite net magnetization. Incorporating FiM into the magnetic tunnel junction will be beneficial to further improve the writing speed of magnetic random access memory. It is commonly assumed that the FeCo and Gd atoms are switched together due to the strong exchange coupling, which remains valid even if one performs the two-sublattice macrospin simulation. Interestingly, using the atomistic model developed by our group, it is clearly seen that different atoms are not switched together. In addition, our study reveals that the nature of switching is spatially nonuniform even in the small sample with the dimension of 20 x 20 nm(2). Furthermore, the characteristics of nonuniformity are completely different for samples with different Gd compositions (x). When x is close to the magnetization compensation point, successful switching cannot be obtained, but is accompanied by the stable oscillation. The atom type that dominates the oscillation is different from that predicted by the two-sublattice macrospin model. In addition, the size of a singular region is a non-monotonic function of current density. All these results can only be understood by considering the spatial nonuniform magnetization dynamics.
引用
收藏
页数:6
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