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光解偏振多原子分子中轴向反冲极限以外的矢量相关性。

Vector correlations in photodissociation of polarized polyatomic molecules beyond the axial recoil limit.

机构信息

Ioffe Physical-Technical Institute, Russian Academy of Sciences, 194021 St. Petersburg, Russia.

出版信息

Phys Chem Chem Phys. 2011 May 14;13(18):8163-74. doi: 10.1039/c0cp01375g. Epub 2010 Dec 13.

Abstract

We present the full quantum mechanical theory of the angular momentum distributions of photofragments produced in photolysis of oriented/aligned parent polyatomic molecules beyond the axial recoil limit. This paper generalizes the results of Underwood and Powis(28,29) to the case of non-axial recoil photodissociation of an arbitrary polyatomic molecule. The spherical tensor approach is used throughout this paper. We show that the recoil angular distribution of the angular momentum polarization of each of the photofragments can be presented in a universal spherical tensor form valid for photolysis in diatomic or polyatomic molecules, irrespective of the reaction mechanism. The angular distribution can be written as an expansion over the Wigner D-functions in terms of the set of the anisotropy-transforming coefficients c(K(i)q(i))(K) (k(d), K(0)) which contain all of the information about the photodissociation dynamics and can be either determined from experiment, or computed from quantum mechanical theory. An important new conservation rule is revealed through the analysis, namely that the component q(i) of the initial reagent polarization rank K(i) and the photofragment polarization rank K onto the photofragment recoil direction k is preserved in any photolysis reaction. Both laboratory and body frame expressions for the recoil angle dependence of the photofragment angular momentum polarization are presented. The parent molecule polarization is shown to lead to new terms in the obtained photofragment angular distributions compared with the isotropic case. In particular, the terms with |q(i)| > 2 can appear which are shown to manifest angular momentum helicity non-conservation in the reaction. The expressions for the coefficients c(K(i)q(i))(K) (k(d), K(0)) have been simplified using the quasiclassical approximation in the high-J limit which allows for introducing the dynamical functions and the rotation factors which describe the decreasing of the photofragment angular momentum orientation and alignment due to the rotation of the molecular axis during photodissociation. In this case, the resultant recoil angle dependence is also presented in a form where the anisotropy of the parent molecular ensemble is expressed in terms of the molecular axis distribution, rather than in terms of the molecular density matrix.

摘要

我们提出了在超越轴向反冲极限的取向/排列的多原子母体分子光解中产生的光碎片的角动量分布的完整量子力学理论。本文将 Underwood 和 Powis(28,29)的结果推广到任意多原子分子的非轴向反冲光解的情况。在整篇论文中,我们使用了球张量方法。我们表明,每个光碎片的角动量极化的反冲角分布可以用一种通用的球张量形式表示,这种形式对于双原子或多原子分子的光解都有效,与反应机制无关。角分布可以表示为以各向异性变换系数 c(K(i)q(i))(K) (k(d), K(0))为变量的 Wigner D-函数的展开式,这些系数包含了光解动力学的所有信息,并且可以通过实验确定,也可以通过量子力学理论计算。通过分析揭示了一个重要的新守恒定律,即在任何光解反应中,初始试剂极化分量 K(i)和光碎片极化分量 K 到光碎片反冲方向 k 的 q(i)分量保持不变。给出了实验室和体坐标系中光碎片角动量极化的反冲角依赖关系的表达式。与各向同性情况相比,母体分子极化导致了所得到的光碎片角分布中出现新的项。特别是,出现了 |q(i)| > 2 的项,表明反应中角动量螺旋性不守恒。在高 J 极限下,我们简化了系数 c(K(i)q(i))(K) (k(d), K(0))的表达式,这允许引入动力学函数和旋转因子,这些函数和因子描述了在光解过程中分子轴旋转导致光碎片角动量取向和排列的减小。在这种情况下,还以一种形式给出了反冲角依赖关系,其中分子集合的各向异性用分子轴分布表示,而不是用分子密度矩阵表示。

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