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首页> 外文期刊>Dalton transactions: An international journal of inorganic chemistry >A crystallographic, EPR and theoretical study of the Jahn-Teller distortion in [CuTp_2](Tp~- = tris{pyrazol-1-yl}hydridoborate)
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A crystallographic, EPR and theoretical study of the Jahn-Teller distortion in [CuTp_2](Tp~- = tris{pyrazol-1-yl}hydridoborate)

机译:[CuTp_2](Tp〜-=三{吡唑-1-基}氢硼酸盐)Jahn-Teller变形的晶体学,EPR和理论研究

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摘要

Crystals of the title compound (1) contain two independent, centrosymmetric half-molecules per asymmetric unit. While both of these show Jahn-Teller elongated six-coordinate geometries, the lengths of the elongated Cu-N bonds in the two molecules differ by 0.117(2) at 30 K. The structure of one of these molecules (molecule A) does not vary with temperature below 350 K. The other molecule (molecule B) shows Cu-N bond lengths that are temperature-dependent between 225 and 375 K, but do not vary further at lower temperature. This indicates a fluxional axis of Jahn-Teller elongation in this molecule at these higher temperatures. Consideration of the thermal parameters in these structures implies that the fluxionality in molecule B is frozen out near 150 K. This conclusion is supported by a Q-band powder EPR study. The d-d transition energies of molecules A and B have been calculated by several density function (DF) methods, including a time-dependent DF calculation. The crystallographic data have been reproduced using the vibronic coupling model of B is and Hitchman. This has shown that the different fluxionality regimes for molecules A and B are not a consequence of their different static molecular structures, but rather reflect their different local environments in the crystal.
机译:标题化合物(1)的晶体每个不对称单元包含两个独立的中心对称半分子。虽然这两个都显示了Jahn-Teller细长的六坐标几何形状,但两个分子中的细长Cu-N键的长度在30 K时相差0.117(2)。这些分子之一(分子A)的结构没有温度低于350 K时会发生变化。另一个分子(分子B)显示Cu-N键的长度在225至375 K之间随温度而变化,但在较低温度下不会进一步变化。这表明在这些较高温度下该分子中Jahn-Teller伸长的通量轴。考虑这些结构中的热参数意味着分子B中的流动性在150 K附近冻结。这一结论得到Q波段粉末EPR研究的支持。分子A和B的d-d跃迁能已通过几种密度函数(DF)方法进行了计算,包括随时间变化的DF计算。使用B is和Hitchman的振动耦合模型复制了晶体学数据。这表明,分子A和B的不同通量范围不是其静态分子结构不同的结果,而是反映了它们在晶体中的不同局部环境。

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