K3Cu8Se6的合成、晶体结构及低温x射线研究

C. Näther , D. Röhnert , W. Bensch
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引用次数: 8

摘要

以单质铜与K2Se3、外加硒(摩尔比为1:3:1)在623 K下反应制备了新型三元混价硒化铜K3Cu8Se6。该化合物在C2/m单斜空间群中结晶,与K3Cu8S6、RbCu8S6、Rb3Cu8Se6和Cs3Cu8Se6等型。该结构由1∞[Cu8Se6]层组成,这些层被钾离子分开。铜原子或呈四面体畸变,或与硒原子呈三角形配位。在晶体结构中,三角形平面配位铜原子形成平行于b轴的双链。这些双链通过扭曲的CuSe4四面体连接成层,这些四面体与Cu周围的Se3三角形共享边缘和角落。在这部分结构中,Cu-Cu距离很短,只有2.497 (2)Å,比单质铜中的Cu-Cu距离短。由于四面体配位铜离子在室温下表现出异常大的各向异性位移参数,因此进行了低温结构测定。在低温下,所有原子的各向异性位移系数都明显较小,但即使在150 K时,四面体配位铜原子的一些系数也比三角形平面配位铜中心的系数大两倍。然而,实验表明,这种无序的性质似乎主要是由于铜离子在室温下的流动性扩大,而铜离子在冷却时被冻结。我们没有给出像K3Cu8S6那样形成上层结构的线索。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Synthesis, crystal structure and low-temperature X-ray investigations of K3Cu8Se6

The new ternary mixed-valent copper selenide K3Cu8Se6 has been prepared by the reaction of elemental copper with K2Se3 and additional selenium (molar ratio 1: 3: 1) at 623 K. The compound crystallizes in the monoclinic space group C2/m and is isotypic to K3Cu8S6, RbCu8S6, Rb3Cu8Se6 and Cs3Cu8Se6. The structure consists of 1[Cu8Se6] layers which are separated by the potassium cations. The copper atoms are either tetrahedrally distorted or trigonal planar coordinated by the selenium atoms. In the crystal structure the trigonal planar coordinated Cu atoms form double chains which are running parallel to the b-axis. These double chains are connected into layers via the distorted CuSe4 tetrahedra which share edges and corners with the Se3 triangles around Cu. In this part of the structure a very short Cu-Cu distances of only 2.497 (2) Å appears which is shorter than the Cu-Cu distance in elemental copper. Because the tetrahedrally coordinated copper ions exhibit unusual large anisotropic displacement parameters at room temperature, a low-temperature structure determination was performed. At low temperatures the anisotropic displacement coefficients are significantly smaller for all atoms, but even at 150 K some coefficients for the tetrahedrally coordinated Cu atoms are twice as large as for the trigonal planar coordinated Cu centers. However, the experiment shows that the nature of the disorder seems to be predominantly due to an enlarged mobility of the copper ions at room-temperature which is freezed on cooling. Our give no hints for the formation of a superstructure like in K3Cu8S6.

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