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Order Versus Disorder in Chiral Tetrathiafulvalene-Oxazoline Radical-Cation Salts: Structural and Theoretical Investigations and Physical Properties

机译:手性四硫富瓦烯 - 恶唑啉自由基阳离子中的有序与无序:结构和理论研究和物理性质

摘要

Electrocrystallization experiments with the chiral ethylenedithio-tetrathiafulvalene-methyl-oxazoline (EDT-TTF-OX) donors (R)-, (S)-, and (rac)-1 have provided two series of mixed-valence salts with the PF6− and [Au(CN)2]− anions. Within each series the cell parameters are the same for the three R, S, and rac compounds, except for the space group, which is centrosymmetric triclinic P1 for the racemic forms and noncentrosymmetric P1 for the enantiopure salts. In the racemic salt [(rac)-1]2PF6 the two enantiomers crystallize disordered on the same crystallographic site with a site occupational factor of 0.6:0.4, whereas this type of disorder is not possible in the enantiopure salts. Both s-cis and s-trans conformations, when taking into account the mutual orientation of the TTF and oxazoline moieties, are present in this first series. In sharp contrast, in the series of salts [1]2[Au(CN)2], only the s-trans conformation is observed with no structural disorder. Theoretical calculations at the DFT level of theory revealed a very small energy difference between the two stable planar s-cis and s-trans conformations, which are both energy minima in either neutral or oxidized states. Single-crystal conductivity measurements showed metallic-like behavior for all the salts down to 220–250 K with a smooth increase in resistivity at lower temperatures. The conductivity at room temperature is 5 S cm−1 for [(rac)-1]2PF6, in which disorder was observed, whereas for [(R)-1]2PF6 and [(S)-1]2PF6 the average value is around 100 S cm−1. In the second series of salts the conductivity at room temperature is 125–130 S cm−1 for [(rac)-1]2[Au(CN)2] and [(R)-1]2[Au(CN)2]. Extended Hückel band structure calculations revealed identical features for the three salts of the [1]2[Au(CN)2] series and are consistent with the electronic structures of quasi-one-dimensional conductors.
机译:使用手性乙二硫基-四硫富瓦烯-甲基-恶唑啉(EDT-TTF-OX)供体(R)-,(S)-和(rac)-1进行电结晶实验,提供了两个系列的PF6-和[Au(CN)2]-阴离子。在每个系列中,除了空间组外,三个R,S和rac化合物的细胞参数均相同,对于外消旋形式为中心对称三斜P1,对映体纯盐为非中心对称P1。在外消旋盐[(rac)-1] 2PF6中,两种对映异构体在同一晶体位点上以0.6:0.4的位点职业因子结晶无序,而在对映纯盐中这种类型的无序是不可能的。当考虑到TTF和恶唑啉部分的相互取向时,s-顺式和s-反式构象都存在于该第一系列中。与之形成鲜明对比的是,在一系列盐[1] 2 [Au(CN)2]中,仅观察到s-反式构象,而没有结构异常。在DFT理论水平上的理论计算表明,两个稳定的平面s-cis和s-trans构象之间的能量差很小,它们在中性或氧化态下均为最小能量。单晶电导率测量结果显示,所有盐类(低至220–250 K)都具有类似金属的行为,并且在较低温度下电阻率平稳增加。 [[rac] -1] 2PF6在室温下的电导率为5 S cm-1,其中观察到无序,而[[R] -1] 2PF6和[(S)-1] 2PF6的平均值为大约100 S cm-1。在第二系列盐中,[(rac)-1] 2 [Au(CN)2]和[(R)-1] 2 [Au(CN)2在室温下的电导率为125-130 S cm-1 ]。扩展的Hückel能带结构计算揭示了[1] 2 [Au(CN)2]系列的三种盐的相同特征,并且与准一维导体的电子结构一致。

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