Magnetic properties and magnetic structures of synthetic natrochalcites, NaMII2(D3O2)(MoO4)2, M = Co or Ni

被引:24
|
作者
Vilminot, Serge [1 ]
Andre, Gilles [2 ]
Bouree-Vigneron, Francoise [2 ]
Baker, Peter J. [3 ]
Blundell, Stephen J. [3 ]
Kurmoo, Mohamedally [4 ]
机构
[1] ULP, CNRS, IPCMS, Grp Mat Inorgan,UMR 7504, F-67034 Strasbourg 2, France
[2] CEA Saclay, CNRS, Lab Leon Brillouin, F-91191 Gif Sur Yvette, France
[3] Univ Oxford, Clarendon Lab, Oxford OX1 3PU, England
[4] Univ Strasbourg, CNRS, Inst Le Bel, Chim Coordinat Organ Lab,UMR7140, F-67000 Strasbourg 01, France
基金
英国工程与自然科学研究理事会;
关键词
D O I
10.1021/ja804685u
中图分类号
O6 [化学];
学科分类号
0703 ;
摘要
The magnetic properties and magnetic structures from neutron diffraction of two synthetic natrochalcites, NaM2II(H3O2)(MoO4)(2), M = CO (1Co) or Ni (2Ni), are reported. They are isostructural (monoclinic C2/m) and consist of chains of edge-shared MO6 octahedra connected by mu-O from H3O2- and MoO42-. These chains form a three-dimensional network with O-H-O, O-Mo-O, and O-Na-O bridging 4, 3, and 4 metal ions, respectively. Both compounds behave as canted antiferromagnets but differ in their behaviors, 1Co showing a broad maximum (28 K) above the Neel transition (21 K) and the canting taking place at 13 K, some 8 K below T-N, while for 2Ni the canting takes place at T-N (28 K). Analyses of the neutron powder diffraction data shed some light on the geometry of D3O2- and suggest antiferromagnetism with a propagation vector k = (0,0,0) with the moments within each chain being parallel but antiparallel to those in neighboring chains. The difference between 1Co and 2Ni is in the orientation of the moments; they are parallel to the chain axis (b-axis) for 1Co and perpendicular to it for 2Ni with a major component along the c-axis and a small one along the a-axis. The heat capacity data peak at 20.9(3) K (1Co) and 25.1 (1) K (2Ni). The derived magnetic entropies, following correction of the lattice contribution using the measured data for the nonmagnetic Zn analogue, suggest S = 1/2 for 1Co but is lower than that expected for 2Ni (S = 1). In both cases, only ca. 60% of the entropy is found below the magnetic ordering temperature, suggesting considerable short-range correlations at higher temperatures. While the temperature at which the magnetic diffraction becomes observable coincides with that of at the peak in heat capacity, it is lower than TN observed by magnetization measurements in both cases, and there is evidence of short-range ordering in a narrow range of temperature (T-N +/- 5 K).
引用
收藏
页码:13490 / 13499
页数:10
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