Laboratoire de Spectroscopie Atomique, Moléculaire et Applications-LSAMA, Université de Tunis, Tunis, Tunisia.
J Chem Phys. 2012 Jun 28;136(24):244309. doi: 10.1063/1.4730303.
Highly correlated ab initio methods were used in order to generate the potential energy curves and spin-orbit couplings of electronic ground and excited states of PS and PS(+). We also computed those of the bound parts of the electronic states of the PS(-) anion. We used standard coupled cluster CCSD(T) level with augmented correlation-consistent basis sets, internally contacted multi-reference configuration interaction, and the newly developed CCSD(T)-F12 methods in connection with the explicitly correlated basis sets. Core-valence correction and scalar relativistic effects were examined. Our data consist of a set of spectroscopic parameters (equilibrium geometries, harmonic vibrational frequencies, rotational constants, spin-orbit, and spin-spin constants), adiabatic ionization energies, and electron affinities. For the low laying electronic states, our calculations are consistent with previous works whereas the high excited states present rather different shapes. Based on these new computations, the earlier ultraviolet bands of PS and PS(+) were reassigned. For PS(-) and in addition to the already known anionic three bound electronic states (i.e., X(3)Σ(-), (1)Δ, and 1(1)Σ(+)), our calculations show that the (1)Σ(-), (3)Σ(+), and the (3)Δ states are energetically below their quartet parent neutral state (a(4)Π). The depletion of the J = 3 component of PS(-)((3)Δ) will mainly occur via weak interactions with the electron continuum wave.
我们使用高度相关的从头算方法生成了 PS 和 PS(+)的电子基态和激发态的势能曲线和自旋轨道耦合。我们还计算了 PS(-)阴离子电子态的束缚部分。我们使用了带有增强相关性一致基组的标准耦合簇 CCSD(T)水平、内部接触多参考组态相互作用和新开发的 CCSD(T)-F12 方法,并结合了显式相关基组。我们检查了核价修正和标量相对论效应。我们的数据包括一组光谱参数(平衡几何形状、简谐振动频率、转动常数、自旋轨道和自旋自旋常数)、绝热电离能和电子亲和能。对于低能电子态,我们的计算与以前的工作一致,而高能激发态则呈现出不同的形状。基于这些新的计算,我们重新分配了 PS 和 PS(+)的早期紫外带。对于 PS(-),除了已经知道的三个阴离子束缚电子态(即 X(3)Σ(-)、(1)Δ 和 1(1)Σ(+))之外,我们的计算表明(1)Σ(-)、(3)Σ(+)和(3)Δ 态在能量上低于其四重 parent 中性态(a(4)Π)。PS(-)((3)Δ)的 J = 3 分量的耗尽将主要通过与电子连续波的弱相互作用发生。