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通讯:氦纳米液滴光电离的碱金属原子的角动量取向和荧光偏振。

Communication: angular momentum alignment and fluorescence polarization of alkali atoms photodetached from helium nanodroplets.

机构信息

LCAR-IRSAMC, Université Toulouse 3 - Paul Sabatier and CNRS, 31062 Toulouse, France.

出版信息

J Chem Phys. 2013 Dec 14;139(22):221102. doi: 10.1063/1.4843235.

DOI:10.1063/1.4843235
PMID:24329048
Abstract

The theory of photofragments angular momentum polarization is applied to the photodetachment of an electronically excited alkali atom from a helium nanocluster (N = 200). The alignment of the electronic angular momentum of the bare excited alkali atoms produced is calculated quantum mechanically by solving the excited states coupled equations with potentials determined by density functional theory (DFT). Pronounced oscillations as a function of excitation energy are predicted for the case of Na@(He)200, in marked contrast with the absorption cross-section and angular distribution of the ejected atoms which are smooth functions of the energy. These oscillations are due to quantum interference between different coherently excited photodetachment pathways. Experimentally, these oscillations should be reflected in the fluorescence polarization and polarization-resolved photoelectron yield of the ejected atoms, which are proportional to the electronic angular momentum alignment. In addition, this result is much more general than the test case of NaHe200 studied here. It should be observable for larger droplets, for higher excited electronic states, and for other alkali as well as for alkali-earth atoms. Detection of these oscillations would show that the widely used pseudo-diatomic model can be valid beyond the prediction of absorption spectra and could help in interpreting parts of the dynamics, as already hinted by some experimental results on angular anisotropy of bare alkali fragments.

摘要

光碎片角动量极化理论被应用于氦团簇(N = 200)中电子激发的碱金属原子的光致脱附。通过求解密度泛函理论(DFT)确定的势能耦合的激发态方程,从量子力学上计算了产生的裸露激发碱金属原子的电子角动量的取向。对于 Na@(He)200 情况,预测了明显的随激发能量的振荡,与射出原子的吸收截面和角分布形成鲜明对比,后者是能量的光滑函数。这些振荡是由于不同相干激发的光致脱附途径之间的量子干涉引起的。在实验中,这些振荡应该反映在射出原子的荧光偏振和偏振分辨光电子产额中,它们与电子角动量取向成正比。此外,这一结果比这里研究的 NaHe200 测试案例更为普遍。它应该可以在更大的液滴、更高的激发电子态以及其他碱金属和碱土金属原子中观察到。检测到这些振荡将表明广泛使用的伪双原子模型可以超出吸收光谱的预测而有效,并有助于解释部分动力学,正如一些关于裸露碱金属碎片的各向异性的实验结果所暗示的那样。

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