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手性四硫富瓦烯-恶唑啉自由基阳离子盐中的有序与无序:结构与理论研究及物理性质。

Order versus disorder in chiral tetrathiafulvalene-oxazoline radical-cation salts: structural and theoretical investigations and physical properties.

机构信息

Université d'Angers, CNRS, Laboratoire de Chimie et Ingénierie Moléculaire, CIMA UMR 6200, UFR Sciences, Bât. K, 2 Bd. Lavoisier, 49045 Angers, France.

出版信息

Chemistry. 2010 Jan 11;16(2):528-37. doi: 10.1002/chem.200901980.

Abstract

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 PF(6) (-) 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 P$\bar 1$ for the racemic forms and noncentrosymmetric P1 for the enantiopure salts. In the racemic salt (rac)-1PF(6) 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[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)-1PF(6), in which disorder was observed, whereas for (R)-1PF(6) and (S)-1PF(6) 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[Au(CN)(2)] and (R)-1[Au(CN)(2)]. Extended Hückel band structure calculations revealed identical features for the three salts of the 1[Au(CN)(2)] series and are consistent with the electronic structures of quasi-one-dimensional conductors.

摘要

用电化学结晶实验,我们合成了手性乙基二硫代四硫富瓦烯-甲基恶唑啉(EDT-TTF-OX)给体(R)-、(S)-和(rac)-1,并得到了两个系列的混合价盐,其中阴离子分别为 PF(6) (-) 和 [Au(CN)(2)] (-)。在每个系列中,三个 R、S 和 rac 化合物的晶胞参数相同,除了空间群,外消旋盐(rac)-1 的空间群为中心对称的三斜 P$\bar 1$,而对映纯盐的空间群为非中心对称的 P1。在外消旋盐(rac)-1PF(6)中,两种对映异构体无序地占据同一晶体学位点,占据因子为 0.6:0.4,而这种无序在对映纯盐中是不可能的。当考虑 TTF 和恶唑啉部分的相互取向时,这一系列中同时存在 s-cis 和 s-trans 构象。与此形成鲜明对比的是,在盐系列1[Au(CN)(2)]中,仅观察到 s-trans 构象,没有结构无序。DFT 理论计算表明,在中性或氧化态下,两种稳定的平面 s-cis 和 s-trans 构象之间的能量差异非常小,它们都是能量最小值。单晶电导率测量表明,所有盐在 220-250 K 以下表现出金属样行为,低温下电阻率呈平滑增加。在观察到无序的(rac)-1](2)PF(6)中,室温电导率为 5 S cm(-1),而(R)-1](2)PF(6)和(S)-1](2)PF(6)的平均电导率约为 100 S cm(-1)。在第二个盐系列中,室温电导率在 125-130 S cm(-1)范围内,对于(rac)-1](2)[Au(CN)(2)]和(R)-1](2)[Au(CN)(2)]。扩展的 Hückel 能带结构计算揭示了1[Au(CN)(2)]系列中三种盐的相同特征,与准一维导体的电子结构一致。

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