Magnetic structures of UNiAl in magnetic fields

被引:14
作者
Prokes, K [1 ]
Bourdarot, F
Burlet, P
Olsovec, M
Sechovsky, V
Javorsky, P
Brück, E
Goukassov, A
de Boer, FR
Menovsky, AA
机构
[1] Univ Higashi Hiroshima, ADSM, Dept Quantum Matter, Higashihiroshima 7398526, Japan
[2] Charles Univ, Dept Met Phys, CR-12116 Prague 2, Czech Republic
[3] CEN Grenoble, CEA, DRFMC SPSMS MDN, F-38054 Grenoble 9, France
[4] Univ Amsterdam, Van der Waals Zeeman Inst, NL-1018 XE Amsterdam, Netherlands
[5] CEA Saclay, Leon Brillouin Lab, F-91191 Gif Sur Yvette, France
基金
日本学术振兴会;
关键词
UNiAl; actinides; antiferromagnetic structure; neutron diffraction;
D O I
10.1016/S0921-4526(98)01054-0
中图分类号
O469 [凝聚态物理学];
学科分类号
070205 ;
摘要
UNiAl orders antiferromagnetically (AF) below T(N) = 19.3 K with a propagation vector q = (0.1, 0.1, 0.5). U moments oriented along the c-axis of the hexagonal structure are modulated sinusoidally within the basal plane with an amplitude of 1.24 mu(B)/U. The magnetic structure consists of three U moments (U(1), U(2), U(3)) coupled ferromagnetically within the basal plane. U(1) and U(2) are substantially larger than II, and invariant with held, whereas U(3) becomes enhanced in a held along c. The vector q remains intact in fields lower than the critical metamagnetic field (B(c) = 11.4 T at 1.5 K). Above B(c), UNiAl orders ferromagnetically with equal Umoments of 0.91 mu(B) in 11.8 T at 1.7 K. When decreasing field below B(c), the original propagation vector is lost and a new AF structure with q ' = (0.17, 0.03, 0.5) is established. The original q is recovered only by warming far above T(N) and subsequent zero-field cooling. (C) 1999 Elsevier Science B.V. All rights reserved.
引用
收藏
页码:246 / 247
页数:2
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