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首页> 外文期刊>The Journal of Chemical Physics >Spin-orbit coupling effects in dihydrides of third-row transition elements.II. Interplay of nonadiabatic coupling in the dissociation path ofrhenium dihydride
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Spin-orbit coupling effects in dihydrides of third-row transition elements.II. Interplay of nonadiabatic coupling in the dissociation path ofrhenium dihydride

机译:第三行过渡元素二酐中的自旋轨道耦合效应。二氢化hen离解路径中非绝热偶联的相互作用

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摘要

This is the second paper in a series of investigations on spin-orbit coupling (SOC) effects indihydrides of third-row transition elements. The dissociation path of rhenium dihydride wasexplored using the multiconfiguration self-consistent-field method followed by diagonalization ofSOC matrices, in which the Stevens-Basch-Krauss-Jasien-Cundari (SBKJC) basis sets wereemployed after adding one set of polarization functions for each atom. The most stable rheniumdihydride has a linear structure and its ground state is ~6Σ_g~+.BothC2vand Csdissociation paths intoa Re atom and a hydrogen molecule (Re(~6S) +H_2(~1Σ_g~+)) were explored on the potential energycurves of low-lying states. A relatively high energy barrier was obtained along the C2v path and twoconical intersections were found at the H–Re–H angles of 29.8° and 96.1° along the C2v path. Sinceit was revealed that the geometrical deformation to Cs symmetry at the H–Re–H angle of 29.8° doesnot provide explicit lowering of the energy barrier for the dissociation, even after consideringnonadiabatic couplings (NACs) in the neighborhood of the conical intersections, it can be concludedthat the most feasible path is hopping from the lowest 6A1 state to the lowest 6B2 state at theH-Re-H angle of 96.1° followed by hopping from the lowest 6B2 state back to the lowest 6A1 stateat the H-Re-H angle of 29.8°, where the latter crossing point is the highest in energy along this path.Thus, when the molecular system can reach the areas of these crossing points, the molecular systemhops from one of the states to another owing to NAC or SOC effects; especially, SOC effectsbecome important at the crossing point with C_(2v)symmetry.
机译:这是对第三行过渡元素的自旋轨道耦合(SOC)效应二酐的一系列研究的第二篇论文。利用多构型自洽场方法,然后对SOC矩阵进行对角化,探索了二氢化rh的解离路径,其中,在为每个原子添加一组极化函数之后,使用Stevens-Basch-Krauss-Jasien-Cundari(SBKJC)基组。最稳定的二氢化rh具有线性结构,其基态为〜6Σ_g〜+ .C2vand Cs的Cs离解路径均进入Re原子和氢分子(Re(〜6S)+ H_2(〜1Σ_g〜+))。低洼国家。沿C2v路径获得了相对较高的能垒,并且沿C2v路径在29.8°和96.1°的H–Re–H角处发现了两个圆锥形交叉点。既然已经揭示出,即使在考虑圆锥形交叉点附近的非绝热耦合(NAC)之后,在29.8°的H–Re–H角处Cs对称性的几何变形也不能显着降低解离的能垒。结论是,最可行的路径是在96.1°的H-Re-H角从最低6A1状态跳到最低6B2状态,然后在H-Re-H角从最低6B2状态跳回到最低6A1状态。 29.8°,其中后一个交叉点是沿着该路径能量最高的位置。因此,当分子系统可以到达这些交叉点的​​区域时,由于NAC或SOC效应,分子系统从一种状态跃迁到另一种状态;特别是,在C_(2v)对称的交叉点,SOC效应变得重要。

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