Field-induced magnetic structures in UNiGe

被引:0
|
作者
K. Prokeš
H. Nakotte
E. Brück
P.F. de Châtel
V. Sechovský
机构
[1] Hahn–Meitner-Institute,
[2] SF 2,undefined
[3] 14109 Berlin,undefined
[4] Germany,undefined
[5] Department of Electronic Structures,undefined
[6] Charles University,undefined
[7] 121 16 Prague 2,undefined
[8] The Czech Republic,undefined
[9] Physics Department,undefined
[10] MSC3D,undefined
[11] New Mexico State University,undefined
[12] Las Cruces,undefined
[13] NM 88003,undefined
[14] USA,undefined
[15] Van der Waals–Zeeman Instituut,undefined
[16] Universiteit van Amsterdam,undefined
[17] 1018 XE Amsterdam,undefined
[18] The Netherlands,undefined
来源
Applied Physics A | 2002年 / 74卷
关键词
PACS: 75.25.+z; 75.30.-m; 61.12.-q;
D O I
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中图分类号
学科分类号
摘要
Below TN=50 K, UNiGe exhibits incommensurate (INC) antiferromagnetic (AF) order with an additional order–order (AF) phase transition at TM=42.5 K. The ground-state AF structure is characterized by a propagation vector (0,1/2,1/2). At 4.2 K, there are two field-induced transitions at 17 and 25 T for the b-axis and at 3 and 10 T for fields along c. No transitions are observed for the a∥B orientation up to 38 T. While the intermediate field-induced phases for both b∥B and c∥B geometries have propagation vector (0,1/3,1/3), the INC structure is characterized by a propagation vector (0,δ1, δ2). All phases have a non-collinear arrangement of U moments with all three components, i.e. also along the a-axis, which is the hard-magnetization direction. The field-forced ferromagnetic phase, which is established for c∥B above 10 T still exhibits a significant a-axis component. This suggests that the magnetic ordering in UNiGe is governed by anisotropic exchange interactions.
引用
收藏
页码:s757 / s759
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