Department of Chemistry, Arak Branch, Islamic Azad University, Arak, Iran.
J Phys Chem A. 2013 Feb 21;117(7):1621-31. doi: 10.1021/jp310389q. Epub 2013 Feb 5.
The structural properties of ethene (1) and tetrahydridodimetallenes M(2)H(4) [M = Si (2), Ge (3), and Sn (4)] have been examined by means of CCSD(T)/Def2-TZVPP, MP4(SDTQ)/Def2-TZVPP, and B3LYP/Def2-TZVPP levels of theory and natural bond orbital analysis (NBO) interpretations. The results obtained showed the expected planar ground state structure for compound 1 (D(2h) symmetry) but trans-bent ground state structures for compounds 2-4 (C(2h) symmetry). The distortions of the high-symmetry configurations of compounds 2-4 are due to the pseudo Jahn-Teller effect (PJTE), which is the only source of instability of high-symmetry configurations in nondegenerate states. The distortions are due to the mixing of the ground A(g) and excited B(2g) states [i.e., HOMO(B(3u)) → LUMO + 3(B(1u)) for compound 1, HOMO(B(3u)) → LUMO + 2(B(1u)) for compound 2, and HOMO(B(3u)) → LUMO + 1(B(1u)) for compounds 3 and 4]. Importantly, the higher-lying B(1g), B(2u), and B(2g) states are not involved in the PJT interactions. The energy gaps between reference states (Δ) in the undistorted configurations decrease from compound 1 to compound 4, and the PJT stabilization energies increase. Therefore, the primary force constant of the ground state in the Q((b2g)) direction (K(0)) decreases from compound 1 to compound 4. This fact can be justified by the valence isoelectronic systems of these compounds (having similar vibronic coupling constants, F). For the purpose of more chemical transparency, the NBO results were analyzed, and their relation to the PJT interactions has been revealed. The NBO analysis showed that stabilization energy associated with π(M-H) (b(u)) → σ*(M═M) (b(u)) electron delocalization (i.e., the mixing of the distorted b(u) molecular orbitals along the b(2g) bending distortions) increases from compound 1 to compound 4. Also, by using the hybridized orbitals obtained, an n parameter is defined. The NBO results revealed that the n values in the mean hybrid orbitals (sp(n)) increase from compound 1 to 4. The correlations between the PJT stabilization energies, bond orders, n values, π(M-M) → σ*(M═M) electron delocalizations, and structural parameters of compounds 1-4 have been investigated.
通过 CCSD(T)/Def2-TZVPP、MP4(SDTQ)/Def2-TZVPP 和 B3LYP/Def2-TZVPP 理论水平和自然键轨道分析(NBO)解释,研究了乙烯(1)和四氢化二金属烯 M(2)H(4) [M = Si(2)、Ge(3)和 Sn(4)] 的结构性质。结果表明,化合物 1 具有预期的平面基态结构(D(2h) 对称性),而化合物 2-4 具有反式弯曲基态结构(C(2h) 对称性)。化合物 2-4 的高对称构型的变形是由于赝 Jahn-Teller 效应(PJTE),这是简并态中高对称构型不稳定性的唯一来源。变形是由于基态 A(g)和激发态 B(2g)态的混合引起的[例如,化合物 1 中 HOMO(B(3u))→LUMO + 3(B(1u)),化合物 2 中 HOMO(B(3u))→LUMO + 2(B(1u)),化合物 3 和 4 中 HOMO(B(3u))→LUMO + 1(B(1u))]。重要的是,较高的 B(1g)、B(2u)和 B(2g)态不参与 PJT 相互作用。未变形构型中参考态(Δ)之间的能隙从化合物 1 到化合物 4 减小,PJT 稳定能增加。因此,在 Q((b2g))方向的基态主要力常数(K(0))从化合物 1 到化合物 4 减小。这一事实可以用这些化合物的价等电子体系(具有相似的振子耦合常数,F)来解释。为了更具化学透明度,分析了 NBO 结果,并揭示了它们与 PJT 相互作用的关系。NBO 分析表明,与 π(M-H)(b(u))→σ*(M═M)(b(u))电子离域相关的稳定能(即沿 b(2g)弯曲变形的扭曲 b(u)分子轨道的混合)从化合物 1 增加到化合物 4。此外,通过使用获得的杂化轨道,定义了一个 n 参数。NBO 结果表明,化合物 1-4 的平均杂化轨道(sp(n))中的 n 值增加。研究了化合物 1-4 的 PJT 稳定能、键序、n 值、π(M-M)→σ*(M═M)电子离域以及结构参数之间的相关性。