Triangular antiferromagnetic order in the honeycomb layer lattice of ErCl3

被引:0
|
作者
Krämer, KW
Güdel, HU
Fischer, P
Fauth, F
Fernandez-Diaz, MT
Hauss, T
机构
[1] Univ Bern, Dept Chem & Biochem, CH-3000 Bern 9, Switzerland
[2] ETH Zurich, CH-5232 Villigen, Switzerland
[3] Paul Scherrer Inst, Neutron Scattering Lab, CH-5232 Villigen, Switzerland
[4] Inst Max Von Laue Paul Langevin, F-38042 Grenoble 9, France
[5] Hahn Meitner Inst, D-14109 Berlin, Germany
来源
EUROPEAN PHYSICAL JOURNAL B | 2000年 / 18卷 / 01期
关键词
D O I
10.1007/s100510070075
中图分类号
O469 [凝聚态物理学];
学科分类号
070205 ;
摘要
ErCl3 crystallizes in the AlCl3-type layer structure. The crystal structure was refined in the paramagnetic state by powder neutron diffraction.. The monoclinic lattice parameters at 1.5 K are a 6.8040(3) Angstrom, b = 11.7456(5) Angstrom, c = 6.3187(3) Angstrom and beta = 110.851(3)degrees. The space group is C2/m. Short range, predominantly in-plane, magnetic ordering occurs above 350 mK up to several Kelvin. Below T-N = 350(5) mK a three-dimensional antiferromagnetic order with a propagation vector of k = (2/3, 0, -1/12) sets in. The magnetic structure of ErCl3 was determined by powder and single-crystal neutron diffraction at temperatures down to 45 mK. The Er3+ ions are located on tare-dimensional honeycomb layers in the a-b plane. There are two antiferromagnetically coupled 120 degrees triangular sublattices which form right- and left-handed helices along the c-axis. The magnetic moments are oriented in the a-b plane and amount to 3.3(1) mu (B)/Er3+ at saturation. From the temperature dependence of the integrated neutron magnetic peak intensity a critical exponent beta = 0.23(2) was derived for the magnetic phase transition.
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页码:39 / 47
页数:9
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