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Use of complex configuration interaction calculations and the stationary principle for the description of metastable electronic states of HCl-

机译:使用复杂的配置相互作用计算和平稳原理描述HCl-

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The complex multireference single- and double-excitation configuration interaction method has been employed to compute potential curves for the anion of the hydrogen chloride molecule. First, conventional CI calculations with real basis functions have been carried out to determine the potential curves of both HCl and its anion over a large range of internuclear distance. It is shown that adding basis functions with very small exponents leads to sharply avoided crossings for the HCl- potentials that greatly complicate the search for resonance states thought to be responsible for features observed in electron collision experiments. By limiting the number of such diffuse-type functions it is possible to describe resonance states at a highly correlated level and still account for their interaction with the continuum in which they are embedded. In the present study of the HCl- anion the complex basis function technique of Moiseyev-Corcoran and McCurdy-Resigno is employed to calculate the energy positions and line-widths of the resonance states. Two states of ~2σ~+ symmetry are calculated which have potentials that have significantly different shapes than that of the neutral ground state and thus contribute to the cross section for vibrational excitation of the neutral HCl molecule induced by low-energy electron collisions. The lower of these (1 ~2σ~+) correlates smoothly with the bound anionic ground state at large internuclear distances and is seen to be responsible for the sharp peaks observed in the low-energy region of the spectrum. The upper state (3~2σ~+) has a much larger bond length and is assigned to the broad bands observed with a maximum in the 2.5-3.0 eV range. The present calculations thus stand in contradiction to earlier claims that the above peaks are caused by so-called virtual states without a definite autoionization lifetime.
机译:复杂的多参考单激发和双激发构型相互作用方法已用于计算氯化氢分子阴离子的电势曲线。首先,已经进行了具有实基函数的常规CI计算,以确定在较大的核间距范围内HCl及其阴离子的电势曲线。结果表明,增加具有非常小的指数的基函数会导致避免避免HCl电位的交叉,这使寻找共振态的搜索复杂化,认为共振态是电子碰撞实验中观察到的特征所致。通过限制这种扩散型函数的数量,可以在高度相关的水平上描述共振状态,并且仍然可以考虑它们与嵌入它们的连续体的相互作用。在目前对HCl阴离子的研究中,采用了Moiseyev-Corcoran和McCurdy-Resigno的复数基函数技术来计算共振态的能量位置和线宽。计算出〜2σ〜+对称的两个状态,其电势的形状与中性基态的形状显着不同,从而有助于由低能电子碰撞引起的中性HCl分子的振动激发的截面。这些中的较低者(1〜2σ〜+)在大的核间距离处与结合的阴离子基态平滑相关,并且被认为是在低能谱区域观察到的尖峰的原因。较高的态(3〜2σ〜+)具有更长的键长,并分配给观察到的宽带,最大值在2.5-3.0 eV范围内。因此,本计算与先前的权利要求相矛盾,即上述峰值是由所谓的虚拟状态引起的,而没有确定的自电离寿命。

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