Pointner Bernard E, Suontamo Reijo J, Schrobilgen Gary J
Department of Chemistry, McMaster University, Hamilton, Ontario, Canada.
Inorg Chem. 2006 Feb 20;45(4):1517-34. doi: 10.1021/ic0510260.
Reactions of XeO2F2 with the strong fluoride ion acceptors, AsF5 and SbF5, in anhydrous HF solvent give rise to alpha- and beta-[XeO2F][SbF6], [XeO2F][AsF6], and [FO2XeFXeO2F][AsF6]. The crystal structures of alpha-[XeO2F][SbF6] and [XeO2F][AsF6] consist of trigonal-pyramidal XeO2F+ cations, which are consistent with an AXY2E VSEPR arrangement, and distorted octahedral MF6- (M = As, Sb) anions. The beta-phase of [XeO2F][SbF6] is a tetramer in which the xenon atoms of four XeO2F+ cations and the antimony atoms of four SbF6- anions are positioned at alternate corners of a cube. The FO2XeFXeO2F+ cations of [FO(2)XeFXeO2F][AsF6] are comprised of two XeO2F units that are bridged by a fluorine atom, providing a bent Xe- - -F- - -Xe arrangement. The angle subtended by the bridging fluorine atom, a xenon atom, and the terminal fluorine atom of the XeO2F group is bent toward the valence electron lone-pair domain on xenon, so that each F- - -XeO2F moiety resembles the AX(2)Y(2)E arrangement and geometry of the parent XeO2F2 molecule. Reaction of XeF6 with [H3O][SbF6] in a 1:2 molar ratio in anhydrous HF predominantly yielded [XeF5][SbF6].XeOF4 as well as [XeO2F][Sb2F11]. The crystal structure of the former salt was also determined. The energy-minimized, gas-phase MP2 geometries for the XeO2F+ and FO2XeFXeO2F+ cations are compared with the experimental and calculated geometries of the related species IO2F, TeO2F-, XeO2(OTeF5)+, XeO2F2, and XeO2(OTeF5)2. The bonding in these species has been described by natural bond orbital and electron localization function analyses. The standard enthalpies and Gibbs free energies for reactions leading to XeO2F+ and FO2XeFXeO2F+ salts from MF5 (M = As, Sb) and XeO2F2 were obtained from Born-Haber cycles and are mildly exothermic and positive, respectively. When the reactions are carried out in anhydrous HF at low temperatures, the salts are readily formed and crystallized from the reaction medium. With the exception of [XeO2F][AsF6], the XeO2F+ and FO2XeFXeO2F+ salts are kinetically stable toward dissociation to XeO2F2 and MF5 at room temperature. The salt, [XeO2F][AsF6], readily dissociates to [FO2XeFXeO2F][AsF6] and AsF5 under dynamic vacuum at 0 degree C. The decompositions of XeO2F+ salts to the corresponding XeF+ salts and O2 are exothermic and spontaneous but slow at room temperature.
在无水氢氟酸溶剂中,二氧化氙二氟(XeO₂F₂)与强氟离子受体五氟化砷(AsF₅)和五氟化锑(SbF₅)反应,生成α - 和β - [XeO₂F][SbF₆]、[XeO₂F][AsF₆]以及[FO₂XeFXeO₂F][AsF₆]。α - [XeO₂F][SbF₆]和[XeO₂F][AsF₆]的晶体结构由三角锥型的XeO₂F⁺阳离子组成,这与AXY₂E价层电子对互斥理论(VSEPR)排布一致,还有扭曲的八面体MF₆⁻(M = As、Sb)阴离子。[XeO₂F][SbF₆]的β相是一种四聚体,其中四个XeO₂F⁺阳离子的氙原子和四个SbF₆⁻阴离子的锑原子位于立方体的交替角上。[FO₂XeFXeO₂F][AsF₆]的FO₂XeFXeO₂F⁺阳离子由两个通过氟原子桥连的XeO₂F单元组成,形成弯曲的Xe - - -F - - -Xe排列。桥连氟原子、一个氙原子以及XeO₂F基团的端基氟原子所形成的夹角向氙上的价电子孤对区域弯曲,使得每个F - - -XeO₂F部分类似于母体XeO₂F₂分子的AX₂Y₂E排列和几何形状。在无水氢氟酸中,六氟化氙(XeF₆)与[H₃O][SbF₆]以1:2的摩尔比反应,主要生成[XeF₅][SbF₆]·XeOF₄以及[XeO₂F][Sb₂F₁₁]。还测定了前一种盐的晶体结构。将XeO₂F⁺和FO₂XeFXeO₂F⁺阳离子的能量最小化气相MP2几何结构与相关物种IO₂F、TeO₂F⁻、XeO₂(OTeF₅)⁺、XeO₂F₂和XeO₂(OTeF₅)₂的实验和计算几何结构进行了比较。通过自然键轨道和电子定域函数分析描述了这些物种中的键合情况。由MF₅(M = As、Sb)和XeO₂F₂生成XeO₂F⁺和FO₂XeFXeO₂F⁺盐的反应的标准焓和吉布斯自由能通过玻恩 - 哈伯循环获得,分别为轻度放热和正值。当反应在低温无水氢氟酸中进行时,盐很容易从反应介质中形成并结晶。除了[XeO₂F][AsF₆]外,XeO₂F⁺和FO₂XeFXeO₂F⁺盐在室温下对分解为XeO₂F₂和MF₅具有动力学稳定性。盐[XeO₂F][AsF₆]在0℃动态真空下容易分解为[FO₂XeFXeO₂F][AsF₆]和AsF₅。XeO₂F⁺盐分解为相应的XeF⁺盐和O₂是放热且自发的,但在室温下较慢。