中国物理B ›› 2008, Vol. 17 ›› Issue (3): 1130-1134.doi: 10.1088/1674-1056/17/3/063
龚依民1, 蓝志环1, 闫羽1, 杜晓波1, 王文全1, 王学凤1, 苏峰1, 卢磊1, 张之胜1, 金汉民1, 温戈辉2
Gong Yi-Min(龚依民)a), Lan Zhi-Huan(蓝志环)a), Yan Yu(闫羽)a),Du Xiao-Bo(杜晓波)a)†, Wang Wen-Quan(王文全)a), Wang Xue-Feng(王学凤)a), Su Feng(苏峰)a), Lu Lei(卢磊)a), Zhang Zhi-Sheng(张之胜)a),Jin Han-Min(金汉民)a), and Wen Ge-Hui(温戈辉)b)
摘要: In this paper magnetization remanence curves were studied for nanocrystalline Pr8Fe87B5, Pr12Fe82B6 and Pr15Fe77B8. Initially the sample was at remanence following saturation along $z$-axis. After rotating the magnet by $5n$ degrees (n=0, 1, ..., 18) a field H was applied along $z$-axis and then decreased to zero, and the remanence Jr^{n} $ was measured as a function of $H$. The curves were compared with those calculated based on the nucleation of reverse domain model and domain wall pinning model. The latter model succeeds in simulation much better than the former, and it is concluded that the magnetization reversal is dominated by domain wall pinning for all the samples. The nucleation mechanism contribution, while remains small, increases with the increase of Pr content.
中图分类号: (Magnetization curves, hysteresis, Barkhausen and related effects)