TY - JOUR
T1 - Magnetization reversal in epitaxial exchange-biased IrMn/FeGa bilayers with anisotropy geometries controlled by oblique deposition
AU - Zhang, Yao
AU - Zhan, Qingfeng
AU - Zuo, Zhenghu
AU - Yang, Huali
AU - Zhang, Xiaoshan
AU - Dai, Guohong
AU - Liu, Yiwei
AU - Yu, Ying
AU - Wang, Jun
AU - Wang, Baomin
AU - Li, Run Wei
N1 - Publisher Copyright:
© 2015 American Physical Society.
PY - 2015/5/12
Y1 - 2015/5/12
N2 - We fabricated epitaxial exchange biased (EB) IrMn/FeGa bilayers by oblique deposition and systematically investigated their magnetization reversal. Two different configurations with the uniaxial magnetic anisotropy Ku parallel and perpendicular to the unidirectional anisotropy Keb were obtained by controlling the orientation of the incident FeGa beam during deposition. A large ratio of Ku/Keb was obtained by obliquely depositing the FeGa layer to achieve a large Ku while reducing the IrMn thickness to obtain a small Keb. Besides the previously reported square loops, conventional asymmetrically shaped loops, and one-sided and two-sided two-step loops, unusual asymmetrically shaped loops with a three-step magnetic transition for the descending branch and a two-step transition for the ascending branch and biased three-step loops were observed at various field orientations in the films of both IrMn (tIrMn=1.5 to 20 nm)/FeGa (10 nm) with KuKeb and IrMn (tIrMn≤2 nm)/FeGa (10 nm) with Ku||Keb. Considering the geometries of anisotropies, a model based on domain wall nucleation and propagation was employed to quantitatively describe the angular dependent behaviors of IrMn/FeGa bilayers. The biased three-step magnetic switching was predicted to take place when |Ku|>90+Keb, where 90 is the 90° domain wall nucleation energy, and the EB leads to the appearance of the unusual asymmetrically shaped hysteresis loops.
AB - We fabricated epitaxial exchange biased (EB) IrMn/FeGa bilayers by oblique deposition and systematically investigated their magnetization reversal. Two different configurations with the uniaxial magnetic anisotropy Ku parallel and perpendicular to the unidirectional anisotropy Keb were obtained by controlling the orientation of the incident FeGa beam during deposition. A large ratio of Ku/Keb was obtained by obliquely depositing the FeGa layer to achieve a large Ku while reducing the IrMn thickness to obtain a small Keb. Besides the previously reported square loops, conventional asymmetrically shaped loops, and one-sided and two-sided two-step loops, unusual asymmetrically shaped loops with a three-step magnetic transition for the descending branch and a two-step transition for the ascending branch and biased three-step loops were observed at various field orientations in the films of both IrMn (tIrMn=1.5 to 20 nm)/FeGa (10 nm) with KuKeb and IrMn (tIrMn≤2 nm)/FeGa (10 nm) with Ku||Keb. Considering the geometries of anisotropies, a model based on domain wall nucleation and propagation was employed to quantitatively describe the angular dependent behaviors of IrMn/FeGa bilayers. The biased three-step magnetic switching was predicted to take place when |Ku|>90+Keb, where 90 is the 90° domain wall nucleation energy, and the EB leads to the appearance of the unusual asymmetrically shaped hysteresis loops.
UR - https://www.scopus.com/pages/publications/84929590150
U2 - 10.1103/PhysRevB.91.174411
DO - 10.1103/PhysRevB.91.174411
M3 - 文章
AN - SCOPUS:84929590150
SN - 1098-0121
VL - 91
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 17
M1 - 174411
ER -