首页> 外文OA文献 >Full dimensional Franck-Condon factors for the acetylene [~ over A] [superscript 1]A[subscript u] — [~ over X] [superscript 1Σ[+ over g] transition. II. Vibrational overlap factors for levels involving excitation in ungerade modes
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Full dimensional Franck-Condon factors for the acetylene [~ over A] [superscript 1]A[subscript u] — [~ over X] [superscript 1Σ[+ over g] transition. II. Vibrational overlap factors for levels involving excitation in ungerade modes

机译:乙炔[〜over a] [上标1] a [下标u] - [〜over X] [上标1Σ[+ over g]跃迁的全维Franck-Condon因子。 II。在ungerade模式下涉及激励的水平的振动重叠因子

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摘要

A full-dimensional Franck-Condon calculation has been applied to the [~ over A] [superscript 1]A[subscript u] — [~ over X] [superscript 1]Σ[+ over g] transition in acetylene in the harmonic normal mode basis. Details of the calculation are discussed in Part I of this series. To our knowledge, this is the first full-dimensional Franck-Condon calculation on a tetra-atomic molecule undergoing a linear-to-bent geometry change. In the current work, the vibrational intensity factors for levels involving excitation in ungerade vibrational modes are evaluated. Because the Franck-Condon integral accumulates away from the linear geometry, we have been able to treat the out-of-plane component of trans bend (ν['' over 4]) in the linear [~ over X] state in the rotational part of the problem, restoring the χ Euler angle and the a-axis Eckart conditions. A consequence of the Eckart conditions is that the out-of-plane component of ν['' over 4] does not participate in the vibrational overlap integral. This affects the structure of the coordinate transformation and the symmetry of the vibrational wavefunctions used in the overlap integral, and results in propensity rules involving the bending modes of the [~ over X] state that were not previously understood. We explain the origin of some of the unexpected propensities observed in IR-UV laser-induced fluorescence spectra, and we calculate emission intensities from bending levels of the [~ over A] state into bending levels of the [~ over X] state, using normal bending mode and local bending mode basis sets. Our calculations also reveal Franck-Condon propensities for the Cartesian components of the cis bend (ν['' over 5]), and we predict that the best [~ over A]-state vibrational levels for populating [~ over X]-state levels with large amplitude bending motion localized in a single C–H bond (the acetylene↔vinylidene isomerization coordinate) involve a high degree of excitation in ν[′ over 6] (cis-bend). Mode ν[′ over 4] (torsion) populates levels with large amplitude counter-rotational motion of the two hydrogen atoms.
机译:在谐波法线中乙炔中的[〜over A] [上标1] A [下标u] — [〜over X] [上标1]Σ[+ over g]跃迁上已进行了全尺寸Franck-Condon计算。模式基础。计算的详细信息将在本系列的第一部分中讨论。据我们所知,这是对发生线性到弯曲几何变化的四原子分子的第一个全尺寸Franck-Condon计算。在当前的工作中,评估了在不激振振动模式下涉及激励的振动强度因子。由于弗朗克-康登积分的累积远离线性几何,因此我们已经能够在旋转的线性[〜over X]状态下处理反弯弯曲的平面外分量(ν[''over 4])部分问题,恢复χEuler角和a轴Eckart条件。 Eckart条件的结果是ν[''超过4]的平面外分量不参与振动重叠积分。这影响了在重叠积分中使用的坐标变换的结构和振动波函数的对称性,并导致涉及[〜over X]状态的弯曲模式的倾向规则,这是以前无法理解的。我们解释了在IR-UV激光诱导的荧光光谱中观察到的一些意想不到的倾向的起源,并使用以下公式计算了发射强度:从[〜A之上]状态的弯曲能级到[〜X之上]状态的弯曲能级。正常弯曲模式和局部弯曲模式基集。我们的计算还揭示了顺式弯曲的笛卡尔分量的弗兰克-康登倾向(ν[''超过5]),并且我们预测填充[〜超过X]态的最佳[〜超过A]状态的振动能级在单个C–H键(乙炔↔亚乙烯基异构化坐标)中发生大幅度弯曲运动的水平涉及ν['超过6]的高度激发(顺式弯曲)。模式ν['大于4](扭转)填充两个氢原子的大振幅反向旋转运动的能级。

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