Switching field distribution and magnetization reversal process of FePt dot patterns

被引:6
作者
Ishio, S. [1 ]
Takahashi, S. [1 ]
Hasegawa, T. [1 ]
Arakawa, A. [1 ]
Sasaki, H. [1 ]
Yan, Z. [2 ]
Liu, X. [2 ]
Kondo, Y. [3 ]
Yamane, H. [3 ]
Ariake, J. [3 ]
Suzuki, M. [4 ]
Kawamura, N. [4 ]
Mizumaki, M. [4 ]
机构
[1] Akita Univ, Dept Mat Sci & Engn, Akita 0108502, Japan
[2] Akita Univ, Venture Business Lab, Akita 0108502, Japan
[3] Akita Prefectural Res & Dev Ctr, Akita 0101623, Japan
[4] Japan Synchrotron Radiat Res Inst, Sayo, Hyogo 6795198, Japan
基金
日本科学技术振兴机构;
关键词
Fe Pt; Dot pattern; Magnetization reversal; Switching field; Coercivity; ANISOTROPY; DEPENDENCE; FILMS;
D O I
10.1016/j.jmmm.2014.02.049
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The fabrication of FePt nanodots with a high structural quality and the control of their switching fields are key issues in realizing high density bit pattern recording. We have prepared FePt dot patterns for dots with 15-300 nm diameters by electron beam lithography and re-annealing, and studied the relation between magnetization reversal process and structure of FePt nanodots. The switching field (H) of dot patterns re-annealed at 710 degrees C for 240 min showed a bimodal distribution, where a higher peak was found at 5-6 T, and a lower peak was found at similar to 2 T. It was revealed by cross-sectional TOM analysis that the structure of dots in the pattern can be classified into two groups. One group has a high degree of order with well-defined 100 11 crystalline growth, and the other group includes structurally-disturbed dots like [1 1 11 growth and twin crystals. This structural inhomogeneity causes the magnetic switching field distribution observed. (C) 2014 Elsevier By. All rights reserved.
引用
收藏
页码:205 / 210
页数:6
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