Stabilization of perpendicular magnetic anisotropy in CeO2 films deposited on Co/Pt multilayers

被引:4
|
作者
Figueiredo-Prestes, Nicholas [1 ]
Zarpellon, Juliana [1 ]
Jurca, Hugo F. [2 ]
Fernandes, Vilmar [3 ]
Varalda, Jose [1 ]
Schreiner, Wido H. [1 ]
Mosca, Dante H. [1 ]
Fichtner, Paulo F. P. [4 ]
Fabrim, Zacarias E. [4 ]
Bouzehouane, Karim [5 ]
Deranlot, Cyrile [5 ]
George, Jean-Marie [5 ]
机构
[1] Univ Fed Parana, Lab Nanoestruturas Sensores, Ctr Politecn, Caixa Postal 19044, BR-81531990 Curitiba, Parana, Brazil
[2] Inst Fed Parana, Campus Irati, BR-8450000 Irati, PR, Brazil
[3] Inst Fed Parana, Campus Curitiba, BR-80230150 Curitiba, Parana, Brazil
[4] Univ Fed Rio Grande do Sul, Escola Engn, BR-91501970 Porto Alegre, RS, Brazil
[5] Univ Paris Saclay, Univ Paris Sud, CNRS, Unite Mixte Phys, F-91767 Palaiseau, France
来源
RSC ADVANCES | 2016年 / 6卷 / 62期
关键词
NANOCRYSTALLINE CEO2; MECHANISM;
D O I
10.1039/c6ra10392h
中图分类号
O6 [化学];
学科分类号
0703 ;
摘要
Materials with perpendicular magnetic anisotropy (PMA) are of great interest as they have potential applications in high-density non-volatile memories, spin logic devices, and other spintronics applications. To attain perpendicular anisotropy, a number of material systems have been explored as ferromagnetic electrodes. Here, we use (Co/Pt)-multilayered films with PMA covered by a gold spacer-layer to induce the perpendicular magnetization in a ferromagnetic layer of cerium oxide and to control the reversible switching of its magnetization. The origin of the room-temperature ferromagnetism observed in nanocrystalline cerium oxide films remains controversial, but their wide energy band-gap and their transparency to visible light attracts attention for possible applications in magneto-optical devices. A weak magnetic stray field of 40 Oe emanates from the (Co/Pt)-multilayered film and permeates the gold spacer layer. Using a simple micromagnetic model based on the Stoner-Wohlfarth magnetization mechanism, the strength of the magnetic coupling between the ferromagnetic layers is estimated to be 18 mu J m(-2). This magnetic coupling, which is almost independent of temperature, is sufficient to promote the reversible switching of perpendicular magnetization states in the field range of a only few hundred Oersteds at room temperature.
引用
收藏
页码:S6785 / S6789
页数:5
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