Laboratoire des Collisions, Agrégats, Réactivité, IRSAMC, UMR 5589, CNRS et Université Paul Sabatier-Toulouse 3, 118 route de Narbonne, F-31062 Toulouse Cedex 09, France.
J Chem Phys. 2012 Nov 14;137(18):184311. doi: 10.1063/1.4762837.
The stability of the ground or excited state calcium atom in an argon-doped helium droplet has been investigated using an extension of the helium density functional method to treat clusters. This work was motivated by the experimental study presented in a companion paper, hereafter called Paper I [A. Masson, M. Briant, J. M. Mestdagh, M. A. Gaveau, A. Hernando, and N. Halberstadt, J. Chem. Phys. 137, 184310 (2012)], which investigated Ca(2) photodissociation in an argon-doped helium droplet and the nature of the fluorescent species. It is found that one single argon atom is sufficient to bring the calcium atom inside the droplet, for droplets of over 200 helium atoms. The absorption and emission spectra of CaAr(M) (M = 0-7) clusters have been simulated using the recently developed density sampling method to describe the influence of the helium environment. Absorption spectra exhibit broad, double bands that are significantly blueshifted with respect to the calcium atomic line. The emission spectra are less broad and redshifted with respect to the calcium resonance line. The shifts are found to be additive only for M ≤ 2, because only the first two argon atoms are located in equivalent positions around the calcium p orbital. This finding gives a justification for the fit presented in the companion paper, which uses the observed shifts in the emission spectra as a function of argon pressure to deduce the shifts as a function of the number of argon atoms present in the cluster. An analysis of this fit is presented here, based on the calculated shifts. It is concluded that the emitting species following Ca(2) photodissociation in an argon-doped droplet in Paper I could be Ca∗Ar(M) in a partly evaporated droplet where less than 200 helium atoms remain.
使用氦团簇密度泛函方法的扩展来处理,研究了掺氩氦滴中基态和激发态钙原子的稳定性。这项工作的动机来自于一篇伴生论文中的实验研究,以下称为论文 I [A. Masson, M. Briant, J. M. Mestdagh, M. A. Gaveau, A. Hernando, and N. Halberstadt, J. Chem. Phys. 137, 184310 (2012)],该论文研究了掺氩氦滴中 Ca(2)光解和荧光物种的性质。结果表明,对于超过 200 个氦原子的液滴,只需一个单个氩原子就能将钙原子带入液滴内部。使用最近开发的密度抽样方法模拟了 CaAr(M)(M = 0-7)团簇的吸收和发射光谱,以描述氦环境的影响。吸收光谱呈现出宽的、双峰,与钙原子线相比明显蓝移。发射光谱的展宽较小,且相对于钙共振线红移。只有当 M ≤ 2 时,这些位移才是相加的,因为只有前两个氩原子位于钙 p 轨道周围的等效位置。这一发现为伴生论文中提出的拟合提供了合理性,该拟合使用发射光谱中观察到的位移作为氩气压的函数,推导出作为团簇中存在的氩原子数的函数的位移。这里基于计算出的位移,对该拟合进行了分析。得出的结论是,在论文 I 中掺氩液滴中 Ca(2)光解后产生的发射物种可能是部分蒸发液滴中的 Ca∗Ar(M),其中少于 200 个氦原子仍然存在。