Department of Chemistry, Faculty of Sciences, Okayama University, Tsushima-naka 3-1-1, Okayama City, 700 8530 Okayama, Japan.
Phys Chem Chem Phys. 2010 Mar 7;12(9):2126-38. doi: 10.1039/b919953e. Epub 2010 Jan 14.
Spin-unrestricted DFT-X3LYP/6-311++G(d,p) calculations have been performed on a series of complexes of the form Co(H(2)O)(6-n)(NH(3))(n) (n = 0-6) to examine their equilibrium gas-phase structures, energetics, and electronic properties in their quartet electronic ground states. In all cases Co(2+) in the energy-minimised structures is in a pseudo-octahedral environment. The calculations overestimate the Co-O and Co-N bond lengths by 0.04 and 0.08 A, respectively, compared to the crystallographically observed mean values. There is a very small Jahn-Teller distortion in the structure of Co(H(2)O)(6) which is in contrast to the very marked distortions observed in most (but not all) structures of this cation that have been observed experimentally. The successive replacement of ligated H(2)O by NH(3) leads to an increase in complex stability by 6 +/- 1 kcal mol(-1) per additional NH(3) ligand. Calculations using UB3LYP give stabilisation energies of the complexes about 5 kcal mol(-1) smaller and metal-ligand bond lengths about 0.005 A longer than the X3LYP values since the X3LYP level accounts for the London dispersion energy contribution to the overall stabilisation energy whilst it is largely missing at the B3LYP level. From a natural population analysis (NPA) it is shown that the formation of these complexes is accompanied by ligand-to-metal charge transfer the extent of which increases with the number of NH(3) ligands in the coordination sphere of Co(2+). From an examination of the topological properties of the electron charge density using Bader's quantum theory of atoms in molecules it is shown that the electron density rho(c) at the Co-O bond critical points is generally smaller than that at the Co-N bond critical points. Hence Co-O bonds are weaker than Co-N bonds in these complexes and the stability increases as NH(3) replaces H(2)O in the metal's coordination sphere. Several indicators, including the sign and magnitude of the Laplacian of the charge density nabla(2)rho(c), the ratio of the local potential and kinetic energy densities, |V(c)|/G(c), the sign of the total energy density H(c), and the delocalisation index delta(Co,X), X = O, N, are used to show that whilst the metal-ligand bonds are predominantly ionic in nature, they gain covalent character as NH(3) replaces H(2)O, and the Co-N bond is significantly more covalent than the Co-O bond. We have shown that the delocalisation index delta(Co,X), X = O, N, is strongly correlated with the zero-point corrected stabilisation energy E demonstrating that delta can be used as a measure of the bond stability in these complexes.
已对一系列形式为 Co(H(2)O)(6-n)(NH(3))(n) (n = 0-6) 的配合物进行了无自旋限制的 DFT-X3LYP/6-311++G(d,p) 计算,以研究它们在四重电子基态下的平衡气相结构、热力学和电子性质。在所有情况下,能量最小化结构中的 Co(2+) 都处于拟八面体环境中。与晶体观察到的平均值相比,计算结果分别高估了 Co-O 和 Co-N 键长 0.04 和 0.08 Å。Co(H(2)O)(6) 的结构存在很小的 Jahn-Teller 畸变,与实验观察到的大多数(但不是全部)此类阳离子结构中观察到的明显畸变形成对比。配位 H(2)O 的连续取代 NH(3) 导致每个额外的 NH(3)配体使配合物稳定性增加 6 ± 1 kcal mol(-1)。使用 UB3LYP 计算得到的配合物稳定能比 X3LYP 值小约 5 kcal mol(-1),金属-配体键长长约 0.005 Å,因为 X3LYP 能级考虑了伦敦色散能对整体稳定能的贡献,而在 B3LYP 能级中,这种贡献在很大程度上缺失。从自然布居分析(NPA)可以看出,这些配合物的形成伴随着配体到金属的电荷转移,其程度随着 Co(2+) 配位球中 NH(3)配体的数量增加而增加。通过使用 Bader 的分子内原子量子理论对电子电荷密度的拓扑性质进行检查,表明 Co-O 键临界点处的电子密度 rho(c)通常小于 Co-N 键临界点处的电子密度 rho(c)。因此,在这些配合物中,Co-O 键比 Co-N 键弱,并且随着 NH(3)取代金属配位球中的 H(2)O,稳定性增加。几个指标,包括电荷密度拉普拉斯算子 nabla(2)rho(c)的符号和大小、局部势能和动能密度的比值 |V(c)|/G(c)、总能量密度 H(c)的符号以及离域指数 delta(Co,X),X = O,N,用于表明尽管金属-配体键本质上主要是离子性的,但随着 NH(3)取代 H(2)O,它们具有共价特征,并且 Co-N 键比 Co-O 键具有显著更高的共价性。我们已经表明,离域指数 delta(Co,X),X = O,N,与零点校正稳定能 E 强烈相关,表明 delta 可以用作这些配合物中键稳定性的度量。