Albert-Ludwigs-Universität Freiburg, Institut für Anorganische und Allgemeine Chemie and Freiburger Materialforschungszentrum (FMF), Albertstr. 21, 79104 Freiburg, Germany.
Chemistry. 2009 Sep 21;15(37):9505-20. doi: 10.1002/chem.200900100.
Compounds including the free or coordinated gas-phase cations Ag(eta(2)-C(2)H(4))(n) (n = 1-3) were stabilized with very weakly coordinating anions A (A = Al{OC(CH(3))(CF(3))(2)}(4), n = 1 (1); Al{OC(H)(CF(3))(2)}(4), n = 2 (3); Al{OC(CF(3))(3)}(4), n = 3 (5); {(F(3)C)(3)CO}(3)Al-F-Al{OC(CF(3))(3)}(3), n = 3 (6)). They were prepared by reaction of the respective silver(I) salts with stoichiometric amounts of ethene in CH(2)Cl(2) solution. As a reference we also prepared the isobutene complex [(Me(2)C=CH(2))Ag(Al{OC(CH(3))(CF(3))(2)}(4))] (2). The compounds were characterized by multinuclear solution-NMR, solid-state MAS-NMR, IR and Raman spectroscopy as well as by their single crystal X-ray structures. MAS-NMR spectroscopy shows that the Ag(eta(2)-C(2)H(4))(3) cation in its Al{OC(CF(3))(3)}(4) salt exhibits time-averaged D(3h)-symmetry and freely rotates around its principal z-axis in the solid state. All routine X-ray structures (2theta(max.) < 55 degrees) converged within the 3sigma limit at C=C double bond lengths that were shorter or similar to that of free ethene. In contrast, the respective Raman active C=C stretching modes indicated red-shifts of 38 to 45 cm(-1), suggesting a slight C=C bond elongation. This mismatch is owed to residual librational motion at 100 K, the temperature of the data collection, as well as the lack of high angular data owing to the anisotropic electron distribution in the ethene molecule. Therefore, a method for the extraction of the C=C distance in [M(C(2)H(4))] complexes from experimental Raman data was developed and meaningful C=C distances were obtained. These spectroscopic C=C distances compare well to newly collected X-ray data obtained at high resolution (2theta(max.) = 100 degrees) and low temperature (100 K). To complement the experimental data as well as to obtain further insight into bond formation, the complexes with up to three ligands were studied theoretically. The calculations were performed with DFT (BP86/TZVPP, PBE0/TZVPP), MP2/TZVPP and partly CCSD(T)/AUG-cc-pVTZ methods. In most cases several isomers were considered. Additionally, [M(C(2)H(4))(3)] (M = Cu(+), Ag(+), Au(+), Ni(0), Pd(0), Pt(0), Na(+)) were investigated with AIM theory to substantiate the preference for a planar conformation and to estimate the importance of sigma donation and pi back donation. Comparing the group 10 and 11 analogues, we find that the lack of pi back bonding in the group 11 cations is almost compensated by increased sigma donation.
包括游离或配位气相阳离子Ag(eta(2)-C(2)H(4))(n)(n = 1-3)的化合物与非常弱配位阴离子A(A = Al{OC(CH(3))(CF(3))(2)}(4),n = 1(1);Al{OC(H)(CF(3))(2)}(4),n = 2(3);Al{OC(CF(3))(3)}(4),n = 3(5);{(F(3)C)(3)CO}(3)Al-F-Al{OC(CF(3))(3)}(3),n = 3(6)))稳定。它们是通过将各自的银(I)盐与等摩尔量的乙烯在 CH(2)Cl(2)溶液中反应制备的。作为参考,我们还制备了异丁烯配合物[(Me(2)C=CH(2))Ag(Al{OC(CH(3))(CF(3))(2)}(4))](2)。这些化合物通过多核溶液-NMR、固态 MAS-NMR、IR 和拉曼光谱以及它们的单晶 X 射线结构进行了表征。MAS-NMR 光谱表明,其Al{OC(CF(3))(3)}(4)盐中的Ag(eta(2)-C(2)H(4))(3)阳离子在固态中具有时间平均的 D(3h)对称性,并可自由绕其主 z 轴旋转。所有常规 X 射线结构(2theta(max.) < 55 度)在 C=C 双键长度收敛到 3sigma 极限内,该长度与游离乙烯相似或更短。相比之下,各自的拉曼活性 C=C 伸缩模式表明红移 38 至 45 cm(-1),表明 C=C 键略有伸长。这种不匹配归因于 100 K 温度下的残余旋转运动,以及由于乙烯分子中的各向异性电子分布而缺乏高角度数据。因此,开发了一种从实验拉曼数据中提取[M(C(2)H(4))]配合物中 C=C 距离的方法,并获得了有意义的 C=C 距离。这些光谱 C=C 距离与新收集的在高分辨率(2theta(max.) = 100 度)和低温(100 K)下获得的 X 射线数据很好地吻合。为了补充实验数据并进一步了解键的形成,对具有多达三个配体的配合物进行了理论研究。计算使用 DFT(BP86/TZVPP、PBE0/TZVPP)、MP2/TZVPP 和部分 CCSD(T)/AUG-cc-pVTZ 方法进行。在大多数情况下,考虑了几种异构体。此外,还用 AIM 理论研究了[M(C(2)H(4))(3)](M = Cu(+)、Ag(+)、Au(+)、Ni(0)、Pd(0)、Pt(0)、Na(+)),以证实平面构象的偏好,并估计 sigma 供体和 pi 反供体的重要性。比较第 10 和 11 族类似物,我们发现第 11 族阳离子中缺乏 pi 反键作用几乎被增加的 sigma 供体所补偿。