Department of Chemistry, McMaster University, Hamilton, Ontario, L8S 4M1, Canada.
Inorg Chem. 2010 Jul 19;49(14):6673-89. doi: 10.1021/ic100712y.
The syntheses and structural characterizations of the [XOF(2)][AsF(6)] (X = Cl, Br) salts and the XeF(2) adduct-salts, [BrOF(2)][AsF(6)].nXeF(2) (n = 1, 2), are described. Although the [XOF(2)][AsF(6)] salts have been known for some time, their crystal structures had not been reported until the present study. The crystal structure of [BrOF(2)][AsF(6)] shows a positional disorder among the oxygen atom and the fluorine atoms. Both ClOF(2)(+) and BrOF(2)(+) have pseudo-octahedral coordination with a primary tripodal coordination sphere consisting of an oxygen atom and two fluorine atoms and a secondary coordination sphere consisting of three long contacts to fluorine atoms of different AsF(6)(-) anions. The low-temperature Raman spectra of [XOF(2)][AsF(6)] have been assigned on the basis of the crystal structures and with the aid of quantum-chemical calculations using [XOF(2)]AsF(6)(2-) as a model for the crystallographic environment of XOF(2)(+). Several examples of XeF(2) coordinated through fluorine to transition metal centers are known, but no crystallographically characterized examples of XeF(2) coordinated to a nonmetal center other than xenon are known. The complex cation salts, [BrOF(2)][AsF(6)].nXeF(2) (n = 1, 2), were synthesized, and their Raman spectra have been assigned with the aid of quantum-chemical calculations. Although the structure of [BrOF(2)][AsF(6)].2XeF(2) is similar to that of the recently reported krypton analogue, notable differences occur. The contact distances between bromine and the fluorine atoms of NgF(2) (Ng = Kr, Xe) are shorter in [BrOF(2)][AsF(6)].2XeF(2) than in the KrF(2) analogue, which is attributed to the more polar natures of the Xe-F bonds. Unlike [BrOF(2)][AsF(6)].2KrF(2), which has been shown in the prior study to be stable in HF solution at room temperature, [BrOF(2)][AsF(6)].2XeF(2) enters into a dissociative equilibrium in which fluoride ion abstraction by BrOF(2)(+) occurs to give Xe(2)F(3)(+) and BrOF(3). The ELF and QTAIM analyses of [BrOF(2)]AsF(6)(2-) and [BrOF(2)][AsF(6)].2XeF(2) were carried out and are compared with those of [BrOF(2)][AsF(6)].2KrF(2) and for free BrOF(2)(+) to better understand the effect of Br(V) coordination number on the localization domain of the Br(V) valence electron lone pair.
本文描述了 [XOF(2)][AsF(6)](X = Cl,Br)盐和 XeF(2)加合物-盐 [BrOF(2)][AsF(6)]。nXeF(2)(n = 1,2)的合成和结构特征。尽管 [XOF(2)][AsF(6)]盐已经存在了一段时间,但直到本研究才报道了它们的晶体结构。[BrOF(2)][AsF(6)]的晶体结构显示出氧原子和氟原子之间的位置无序。ClOF(2)(+)和 BrOF(2)(+)都具有伪八面体配位,其初级三脚架配位球由一个氧原子和两个氟原子组成,二级配位球由三个与不同 AsF(6)(-)阴离子的氟原子的长接触组成。[XOF(2)][AsF(6)]的低温拉曼光谱是基于晶体结构并借助量子化学计算来分配的,其中使用 [XOF(2)]AsF(6)(2-)作为 XOF(2)(+)晶体环境的模型。已知几个 XeF(2)通过氟原子配位到过渡金属中心的例子,但已知 XeF(2)配位到除氙以外的非金属中心的晶体化学例子尚不清楚。合成了阳离子盐[BrOF(2)][AsF(6)].nXeF(2)(n = 1,2),并借助量子化学计算对其拉曼光谱进行了分配。尽管[BrOF(2)][AsF(6)].2XeF(2)的结构与最近报道的氪类似物相似,但仍存在明显差异。NgF(2)(Ng = Kr,Xe)中溴与氟原子之间的接触距离在[BrOF(2)][AsF(6)].2XeF(2)中比在 KrF(2)类似物中更短,这归因于 Xe-F 键的极性更强。与先前研究中表明在室温下在 HF 溶液中稳定的[BrOF(2)][AsF(6)].2KrF(2)不同,[BrOF(2)][AsF(6)].2XeF(2)进入解离平衡,其中 BrOF(2)(+)通过夺取氟离子形成 Xe(2)F(3)(+)和 BrOF(3)。对[BrOF(2)]AsF(6)(2-)和[BrOF(2)][AsF(6)].2XeF(2)进行了 ELF 和 QTAIM 分析,并与[BrOF(2)][AsF(6)].2KrF(2)和游离 BrOF(2)(+)进行了比较,以更好地理解 Br(V)配位数对 Br(V)价电子孤对定域域的影响。