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首页> 外文期刊>Acta Crystallographica Section B >Temperature-dependent analysis of thermal motion, disorder and structures of tris(ethylenediamine)zinc(II) sulfate and tris(ethylenediamine)copper(II) sulfate
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Temperature-dependent analysis of thermal motion, disorder and structures of tris(ethylenediamine)zinc(II) sulfate and tris(ethylenediamine)copper(II) sulfate

机译:硫酸三(乙二胺)锌(II)和硫酸三(乙二胺)铜(II)的热运动,无序和结构的温度依赖性分析

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摘要

The crystal structures of the title compounds have been determined in the temperature range 140–290?K for the zinc complex, and 190–270?K for the copper complex. The two structures are isostructural in the trigonal space group with the sulfate anion severely disordered on a site with 32 (D3) symmetry. This sulfate disorder leads to a disordered three-dimensional hydrogen-bond network, with the N—H atoms acting as donors and the sulfate O atoms as acceptors. The displacement parameters of the N and C atoms in both compounds contain disorder contributions in the out-of-ligand plane direction owing to ring puckering and/or disorder in hydrogen bonding. In the Zn compound the vibrational amplitudes in the bond directions are closely similar. Their differences show no significant deviations from rigid-bond behaviour. In the Cu compound, a (presumably) dynamic Jahn–Teller effect is identified from a temperature-independent contribution to the displacement ellipsoids of the N atom along the N—Cu bond. These conclusions derive from analyses of the atomic displacement parameters with the Hirshfeld test, with rigid-body models at different temperatures, and with a normal coordinate analysis. This analysis considers the atomic displacement parameters (ADPs) from all different temperatures simultaneously and provides a detailed description of both the thermal motion and the disorder in the cation. The Jahn–Teller radii of the Cu compound derived on the basis of the ADP analysis and from the bond distances in the statically distorted low-temperature phase [Lutz (2010). Acta Cryst. C66, m330–m335] are found to be the same.
机译:锌配合物的温度范围为140-290?K,铜配合物的温度范围为190-270?K,确定了标题化合物的晶体结构。在三角形空间群中,这两个结构是同构的,硫酸根阴离子在具有32(D 3 )对称性的位点上严重无序。这种硫酸盐紊乱导致一个无序的三维氢键网络,其中NH原子为施主,而硫酸盐O原子为受主。两种化合物中N和C原子的位移参数由于环起皱和/或氢键合无序而在配体平面外方向上具有无序贡献。在Zn化合物中,键方向的振动幅度非常相似。它们的差异表明与刚性键合行为无明显差异。在Cu化合物中,根据对N原子沿N-Cu键的位移椭球的温度无关贡献,可以确定(大概)动态Jahn-Teller效应。这些结论来自于使用Hirshfeld检验,不同温度下的刚体模型以及法向坐标分析对原子位移参数的分析。该分析同时考虑了来自所有不同温度的原子位移参数(ADP),并提供了热运动和阳离子中无序的详细描述。 Cu化合物的Jahn–Teller半径是根据ADP分析得出的,并且是由静态变形的低温相中的键距得出的[Lutz(2010)。 Acta Cryst。 C66,m330–m335]被发现是相同的。

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