首页> 外文期刊>The Journal of Chemical Physics >Pulsed field ionization-photoelectorn bands for CS_2~+ in the energy range of 13.2-17.6 eV: An experimental and theoretical study
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Pulsed field ionization-photoelectorn bands for CS_2~+ in the energy range of 13.2-17.6 eV: An experimental and theoretical study

机译:13.2-17.6 eV能量范围内CS_2〜+的脉冲场电离光电子能带:实验和理论研究

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摘要

Vacuum ultraviolet pulsed field ionization-photoelectron (PFI-PE) spectra for CS_2 have been obtained in the energy range of 13.2-17.6 eV, revealing complex vibronic structures for the CS_2~+ (B ~2(sum)_u~+ and C ~2(sum)_g~+) states. The PFI-PE spectra for CS_2~+ (B ~2(sum)_u~+ and C ~2(sum)_g~+) are dominated by the v_1~+ (symmetric stretching) mode. However, PFI-PE bands due to the v_2~+ (bending) and v_3~+ (antisymmetric stetching) modes with both even and odd quanta are clearly resoled. The simulation f rotational contours resolved in the origin PFI-PE bands yields accurate ionization energies of 14.4742+-0.0005 eV (116 742+-4 cm~(-1)) and 16.1883+-0.0005 eV (130 567+-4 cm~(-1)) for the formation of CS_2~+ (B ~2(sum)_u~+ and C ~2(sum)_g~+) sates from Cs_2(X ~1(sum)_g~+), respectively. The PFI-PE bands for ~2(sum)_u~+ (3_0~2) and ~2(sum)_g~+ (3_0~3) at 14.805 and 14.965 eV, which are in near energy resonance with the 0 K dissociation thresholds for the formation of S~+(~4S) + CS(X ~1(sum)~+; v'' = 0 and 1) from CS_2, respectively, are found to be enhanced. These enhancements are rationalized by the prompt dissociation of excited CS_2 in high-n (n>=100) Rydberg states prior to PFI. Three-dimensional potential energy functions (PEFs) for CS_2~+(2 ~2#PI#_u, B ~2(sum)_u~+, and C ~2(sum)_g~+) states have been generated theoretically using the complete active space self-consistent field and internally contracted multireference configuration interaction methods. On the basis of these PEFs, the harmonic frequencies for CS_2~+(2 ~2#PI#_u, B ~2(sum)_u~+, and C ~2(sum)_g~+) and vibronic energy levels for CS_2~+(B ~2(sum)_u~+) have been calculated variationally. These theoretical predictions have made possible a satisfactory assignment of the vibraonic bands resolved in the PFI-PE spectra for CS_2~+(B ~2(sum)_u~+ and C ~2(sum)_g~+). Using the theoretical predictions obtained here, we have also assigned vibraonic bands for CS_2~+(2 ~2#PI#_u) observed in the HeI photoelectron spectrum [Baltzer et al., Chem. Phys. 202, 185 (1996)].
机译:在13.2-17.6 eV的能量范围内获得了CS_2的真空紫外脉冲场电离-光电子(PFI-PE)光谱,揭示了CS_2〜+(B〜2(sum)_u〜+和C〜 2(sum)_g〜+)个状态。 CS_2〜+(B〜2(sum)_u〜+和C〜2(sum)_g〜+)的PFI-PE光谱以v_1〜+(对称拉伸)模式为主。然而,由于具有偶数和奇数量子的v_2〜+(弯曲)和v_3〜+(反对称拉伸)模式,PFI-PE波段得到了清晰的分辨。在原始PFI-PE频带中解析的旋转轮廓的模拟产生了14.4742 + -0.0005 eV(116 742 + -4 cm〜(-1))和16.1883 + -0.0005 eV(130567 + -4 cm〜)的准确电离能(-1))分别从Cs_2(X〜1(sum)_g〜+)形成CS_2〜+(B〜2(sum)_u〜+和C〜2(sum)_g〜+)状态。 〜2(sum)_u〜+(3_0〜2)和〜2(sum)_g〜+(3_0〜3)的PFI-PE谱带分别在14.805和14.965 eV处发生,与0 K离解具有近能量共振发现分别从CS_2形成S〜+(〜4S)+ CS(X〜1(sum)〜+; v''= 0和1)的阈值得到增强。通过增强PFI之前高n(n> = 100)Rydberg态的激发CS_2的迅速离解,可以合理地实现这些增强。理论上,已经使用以下公式生成了CS_2〜+(2〜2#PI#_u,B〜2(sum)_u〜+和C〜2(sum)_g〜+)状态的三维势能函数(PEF)。完整的活动空间自洽字段和内部收缩的多引用配置交互方法。基于这些PEF,CS_2〜+(2〜2#PI#_u,B〜2(sum)_u〜+和C〜2(sum)_g〜+)的谐波频率和CS_2的振动能级〜+(B〜2(sum)_u〜+)已被不同地计算。这些理论预测使CS_2〜+(B〜2(sum)_u〜+和C〜2(sum)_g〜+)在PFI-PE光谱中解析的振动带的满意分配成为可能。使用此处获得的理论预测,我们还为HeI光电子能谱中观察到的CS_2〜+(2〜2#PI#_u)分配了振动带[Baltzer等,Chem。物理202,185(1996)]。

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