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四方平面配位高自旋钴(II)离子:氧硫化物 Sr2CoO2Cu2S2 和 Ba2CoO2Cu2S2 及其固溶体的结构和磁性。

High-spin cobalt(II) ions in square planar coordination: structures and magnetism of the oxysulfides Sr2CoO2Cu2S2 and Ba2CoO2Cu2S2 and their solid solution.

机构信息

Department of Chemistry, University of Oxford, Oxford, UK.

出版信息

J Am Chem Soc. 2011 Mar 2;133(8):2691-705. doi: 10.1021/ja109553u. Epub 2011 Feb 8.

Abstract

The antiferromagnetic structures of the layered oxychalcogenides (Sr(1-x)Ba(x))(2)CoO(2)Cu(2)S(2) (0 ≤ x ≤ 1) have been determined by powder neutron diffraction. In these compounds Co(2+) is coordinated by four oxide ions in a square plane and two sulfide ions at the apexes of an extremely tetragonally elongated octahedron; the polyhedra share oxide vertexes. The magnetic reflections present in the diffraction patterns can in all cases be indexed using a √2a × √2a × c expansion of the nuclear cell, and nearest-neighbor Co(2+) moments couple antiferromagnetically within the CoO(2) planes. The ordered magnetic moment of Co(2+) in Sr(2)CoO(2)Cu(2)S(2) (x = 0) is 3.8(1) μ(B) at 5 K, consistent with high-spin Co(2+) ions carrying three unpaired electrons and with an additional significant unquenched orbital component. Exposure of this compound to moist air is shown to result in copper deficiency and a decrease in the size of the ordered moment to about 2.5 μ(B); there is a strong correlation between the size of the long-range ordered moment and the occupancy of the Cu site. Both the tetragonal elongation of the CoO(4)S(2) polyhedron and the ordered moment in (Sr(1-x)Ba(x))(2)CoO(2)Cu(2)S(2) increase with increasing Ba content, and in Ba(2)CoO(2)Cu(2)S(2), which has Co(2+) in an environment that is close to purely square planar, the ordered moment of 4.5(1) μ(B) at 5 K is over 0.7 μ(B) larger than that in Sr(2)CoO(2)Cu(2)S(2), so the unquenched orbital component in this case is even larger than that observed in octahedral Co(2+) systems such as CoO. The experimental observations of antiferromagnetic ground states and the changes in properties resulting from replacement of Sr by Ba are supported by ab initio calculations on Sr(2)CoO(2)Cu(2)S(2) and Ba(2)CoO(2)Cu(2)S(2). The large orbital moments in these systems apparently result from spin-orbit mixing of the unequally populated d(xz), d(yz), and d(z(2)) orbitals, which are reckoned to be almost degenerate when the CoO(4)S(2) polyhedron reaches its maximum elongation. The magnitudes of the ordered moments in high-spin Co(2+) oxide, oxychalcogenide, and oxyhalide systems are shown to correlate well with the tetragonal elongation of the coordination environment. The large orbital moments lead to an apparently magnetostrictive distortion of the crystal structures below the Neél temperature, with the symmetry lowered from tetragonal I4/mmm to orthorhombic Immm and the size of the distortion correlating well with the size of the long-range ordered moment for all compositions and for temperature-dependent data gathered on Ba(2)CoO(2)Cu(2)S(2).

摘要

(Sr(1-x)Ba(x))(2)CoO(2)Cu(2)S(2)(0 ≤ x ≤ 1)的反铁磁结构已通过粉末中子衍射确定。在这些化合物中,Co(2+) 由四个氧化物离子在正方形平面内配位,两个硫离子在极其拉长的八面体的顶点上配位;多面体共享氧化物顶点。在衍射图中出现的磁反射都可以使用核单元的 √2a × √2a × c 扩展来索引,并且最近邻的 Co(2+) 磁矩在 CoO(2) 平面内反铁磁耦合。在 Sr(2)CoO(2)Cu(2)S(2)(x = 0)中,Co(2+) 的有序磁矩为 3.8(1) μ(B),在 5 K 下,与高自旋 Co(2+) 离子携带三个未配对电子以及额外的显著未淬灭轨道分量一致。暴露于潮湿空气中的这种化合物会导致铜缺乏,有序磁矩减小到约 2.5 μ(B);有序矩的大小与 Cu 位的占有率之间存在很强的相关性。CoO(4)S(2)多面体的四方拉长和 (Sr(1-x)Ba(x))(2)CoO(2)Cu(2)S(2)中的有序磁矩都随着 Ba 含量的增加而增加,而在 Ba(2)CoO(2)Cu(2)S(2)中,Co(2+)处于接近纯平面正方形的环境中,在 5 K 时的有序磁矩为 4.5(1) μ(B),比 Sr(2)CoO(2)Cu(2)S(2)中的有序磁矩大 0.7 μ(B)以上,因此在这种情况下,未淬灭的轨道分量甚至比 CoO 等八面体 Co(2+) 系统中观察到的还要大。反铁磁基态的实验观察结果以及 Sr 被 Ba 取代导致的性质变化得到了 Sr(2)CoO(2)Cu(2)S(2)和 Ba(2)CoO(2)Cu(2)S(2)的从头算计算的支持。这些系统中较大的轨道矩显然是由于不等占据的 d(xz)、d(yz)和 d(z(2))轨道的自旋轨道混合引起的,当 CoO(4)S(2)多面体达到最大伸长时,这些轨道被认为几乎是简并的。高自旋 Co(2+)氧化物、氧卤化物和氧卤化物系统中有序磁矩的大小与配位环境的四方伸长很好地相关。较大的轨道矩导致晶体结构在奈尔温度以下发生明显的磁致伸缩畸变,对称性从四方 I4/mmm 降低到正交 Immm,并且畸变的大小与所有成分的长程有序磁矩以及 Ba(2)CoO(2)Cu(2)S(2 的温度相关数据很好地相关。

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