Braunschweig Holger, Kaupp Martin, Adams Christopher J, Kupfer Thomas, Radacki Krzysztof, Schinzel Sandra
Institut für Anorganische Chemie, Julius-Maximilians-Universität Würzburg, Am Hubland, D-97074 Würzburg, Germany.
J Am Chem Soc. 2008 Aug 27;130(34):11376-93. doi: 10.1021/ja802034p. Epub 2008 Aug 2.
An optimized procedure for the selective dimetalation of [V(eta (6)-C 6H 6) 2] by BuLi/tmeda allowed for the isolation and characterization of [V(eta (6)-C 6H 5Li) 2].tmeda. X-ray diffraction of its thf solvate [V(eta (6)-C 6H 5Li) 2].(thf) 7 revealed an unsymmetrical, dimeric composition in the solid state, in which both subunits are connected by three bridging lithium atoms. Treatment with several element dihalides facilitated the isolation of [ n]vanadoarenophanes ( n = 1, 2) with boron and silicon in the bridging positions. In agreement with the number and covalent radii of the bridging elements, these derivatives exhibit molecular ring strain to a greater or lesser extent. The B-B bond of the [2]bora species [V(eta (6)-C 6H 5) 2B 2(NMe 2) 2] was readily cleaved by [Pt(PEt 3) 3] to afford the corresponding oxidative addition product. Subsequently, [V(eta (6)-C 6H 5) 2B 2(NMe 2) 2] was employed as a diborane(4) precursor in the diboration of 2-butyne under stoichiometric, homogeneous, and heterogeneous catalysis conditions. This transformation is facilitated by the reduction of molecular ring strain, which was confirmed by a decrease of the tilt angle alpha observed in the corresponding solid-state structures. EPR spectroscopy was used to probe the electronic structure of strained [ n]vanadoarenophanes and revealed an obvious correlation between the degree of molecular distortion and the observed hyperfine coupling constant a iso. State-of-the-art DFT calculations were able to reproduce the measured isotropic vanadium hyperfine couplings and the coupling anisotropies. The calculations confirmed the decrease of the absolute isotropic hyperfine couplings with increasing tilt angle. Closer analysis showed that this is mainly due to increased positive contributions to the spin density at the vanadium nucleus from the spin polarization of doubly occupied valence orbitals of vanadium-ligand sigma-antibonding character. The latter are destabilized and thus made more polarizable in the bent structures.
通过丁基锂/四甲基乙二胺对[V(η⁶-C₆H₆)₂]进行选择性双金属化的优化程序,使得[V(η⁶-C₆H₅Li)₂].tmeda得以分离和表征。其四氢呋喃溶剂化物[V(η⁶-C₆H₅Li)₂].(thf)₇的X射线衍射表明,固态下其组成为不对称二聚体,其中两个亚基通过三个桥连锂原子相连。用几种元素二卤化物处理有助于分离出桥连位置含有硼和硅的[ n]钒杂芳烃(n = 1, 2)。与桥连元素的数量和共价半径一致,这些衍生物在不同程度上表现出分子环张力。[2]硼物种[V(η⁶-C₆H₅)₂B₂(NMe₂)₂]的B-B键很容易被[Pt(PEt₃)₃]裂解,得到相应的氧化加成产物。随后,[V(η⁶-C₆H₅)₂B₂(NMe₂)₂]在化学计量、均相和多相催化条件下被用作2-丁炔双硼化反应中的乙硼烷(4)前体。这种转化因分子环张力的降低而得以促进,这一点在相应固态结构中观察到的倾斜角α的减小得到了证实。电子顺磁共振光谱用于探测应变[ n]钒杂芳烃的电子结构,并揭示了分子畸变程度与观测到的各向同性超精细耦合常数a iso之间存在明显的相关性。最先进的密度泛函理论计算能够重现测量到的各向同性钒超精细耦合和耦合各向异性。计算结果证实,随着倾斜角的增加,绝对各向同性超精细耦合减小。进一步分析表明,这主要是由于钒-配体σ反键特征的双占据价轨道的自旋极化对钒核自旋密度的正贡献增加所致。后者在弯曲结构中变得不稳定,因此更具极化性。