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半经典初值表示:从莫勒到米勒。第二部分。

Semiclassical initial value representation: From Møller to Miller. II.

作者信息

Bonnet Laurent

机构信息

Univ. Bordeaux, CNRS, Bordeaux INP, ISM, UMR 5255, F-33400 Talence, France.

出版信息

J Chem Phys. 2023 Mar 21;158(11):114112. doi: 10.1063/5.0137725.

DOI:10.1063/5.0137725
PMID:36948824
Abstract

As shown by W. H. Miller in a seminal article [J. Chem. Phys. 53, 3578 (1970)], the most convenient and accurate semiclassical (SC) theory of molecular scattering in action-angle coordinates is based on the initial value representation (IVR) and the use of shifted angles, which are different from the natural angles usually used in the quantum and classical treatments. Here, we show for an inelastic molecular collision that the initial and final shifted angles define three-segment classical paths that are exactly those involved in the classical-limit of Tannor-Weeks quantum scattering theory [J. Chem. Phys. 98, 3884 (1993)], provided that the translational wave packets |g⟩ and |g⟩ into play in this theory are both taken at |0⟩. Assuming this to be the case, using van Vleck propagators, and applying the stationary phase approximation, Miller's SCIVR expression of S-matrix elements is found, with an additional cut-off factor canceling the energetically forbidden transition probabilities. This factor, however, is close to unity in most practical cases. Furthermore, these developments show that the Møller operators underlie Miller's formulation, thus confirming, for molecular collisions, the results recently established in the simpler case of light-induced rotational transitions [L. Bonnet, J. Chem. Phys. 153, 174102 (2020)]. Last but not least, we show, based on the previous results, that for processes involving long-range anisotropic forces, implementing the Skinner-Miller method [Chem. Phys. Lett. 300, 20 (1999)] in shifted coordinates makes its predictions both easier and more accurate than in natural coordinates.

摘要

正如W. H. 米勒在一篇开创性文章[《化学物理杂志》53, 3578 (1970)]中所表明的那样,在作用角坐标下最方便且准确的分子散射半经典(SC)理论是基于初值表示(IVR)以及使用位移角,位移角与量子和经典处理中通常使用的自然角不同。在此,我们针对非弹性分子碰撞表明,初始和最终位移角定义了三段经典路径,这些路径恰好就是坦诺尔 - 威克斯量子散射理论[《化学物理杂志》98, 3884 (1993)]经典极限中所涉及的路径,前提是该理论中起作用的平移波包|g⟩和|g⟩都取为|0⟩。假设情况如此,使用范弗莱克传播子并应用驻相近似,可得到S矩阵元的米勒SCIVR表达式,还有一个额外的截止因子可消除能量上禁止的跃迁概率。然而,在大多数实际情况下,这个因子接近于1。此外,这些进展表明,莫勒算符是米勒公式的基础,从而对于分子碰撞,证实了最近在光致转动跃迁这个更简单情形中所确立的结果[L. 博内,《化学物理杂志》153, 174102 (2020)]。最后但同样重要的是,基于先前的结果我们表明,对于涉及长程各向异性力的过程,在位移坐标中实施斯金纳 - 米勒方法[《化学物理快报》300, 20 (1999)]会使其预测比在自然坐标中更容易且更准确。

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