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An optimal adiabatic-to-diabatic transformation of the 1 ~2A' and 2~2A' states of H_3

机译:H_3的1〜2A'和2〜2A'状态的绝热绝热转换

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Molecular reaction dynamics iin the adiabatic representation is complicated by the existence of conical intersections and the associated geometric phase effect. The first-derivative coupling vector between the corresponding electronically adiabatic states can, in general, be decomposed into longitudinal (removable) and transverse (nonremovable) parts. At intersection geometries, the longitudinal part is singular, whereas the transverse part is not. In a two-electronic-state Born-Huang expansion, an adiabatic-to-diabatic transformation completely eliminates the contribution of the longitudinal part to the nuclear motion Schrodinger equation, leaving however the transverse part contribution. We report here the results of an accurate calculation of this transverse part for the 1~2A' and 2~2A' electronic states of H_3 obtained by solving a three-dimensional Poisson equation over the entire domain U of internal nuclear configuration space Q of importance to reactive scattering. In addition to requiring a knowledge of the first-derivative coupling vector everywhere in U, the solution depends on an arbitrary choice of boundary conditions. These have been picked so as to minimize the averge value over U of the magnitude of the transverse part, resulting in an optimal diabatization angle. The dynamical importance of the transverse term in the diabatic nuclear motion Schrodinger equation is discussed on the basis of its magnitude not only in the vicinity of the conical intersection, but also over all of the energetically accessible regions of the full U domain. We also present and discusss the diabatic potential energy surfaces obtained by this optimal diabatization procedure.
机译:绝热表示中的分子反应动力学因圆锥形相交的存在和相关的几何相位效应而变得复杂。通常,可以将相应的电子绝热状态之间的一阶导数耦合向量分解为纵向(可移动)部分和横向(不可移动)部分。在相交几何中,纵向部分是奇异的,而横向部分不是。在两个电子状态的Born-Huang展开中,绝热到绝热的转换完全消除了纵向部分对核运动Schrodinger方程的贡献,而留下了横向部分的贡献。我们在这里报告通过求解在内部核构型空间Q的整个域U上的三维泊松方程获得的H_3的1〜2A'和2〜2A'电子态的横向部分的精确计算结果反应性散射。除了需要了解U中各处的一阶导数耦合向量外,该解决方案还取决于边界条件的任意选择。选择这些是为了使横截面的大小的U上的平均值最小,从而产生最佳的绝热角。在绝热核运动Schrodinger方程中,不仅根据圆锥交点附近的幅度,而且还对整个U域的所有能量可访问区域的幅度进行讨论,讨论横向项在绝热核运动Schrodinger方程中的动力学重要性。我们还介绍并讨论了通过该最佳绝热过程获得的绝热势能面。

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