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H2S和H2S+的振动光谱和电子能谱计算

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本文基于MOLPRO软件包使用从头算方法计算了星际分子H2S及其阳离子H2S+的势能面及光电子能谱。首先,在(U)CCSD/cc-pVQZ理论水平下获取了H2S沿法线坐标展开的势能面,势能面直观描述了不同振动模式耦合对分子能量变化的影响,S-H键的非对称伸缩振动和面内弯曲振动共同作用使得系统势能变化范围明显变大。振动多组态相互作用方法被用来计算非谐振动频率和振动光谱,计算结果显示,倍频和组合频之间出现了强烈的费米共振,使得相应波段处的红外强度显著增强。最后,使用拉曼波函数和收缩不变Krylov子空间方法首次计算了H2S X1A1→H2S+ X2B1的光电子能谱。此项研究有助于进一步理解星际分子的内部结构,并为实验研究及星际观测提供参考。
Vibrational spectra and photoelectron spectra calculations of H2S and H2S+
The potential energy surfaces and photoelectron spectra of the interstellar molecule H2S and its cation H2S+ were calculated using ab initio methods based on the MOLPRO software package.First,the potential ener-gy surfaces of H2S expanded along the normal coordinates were obtained at the(U)CCSD/cc-pVQZ level of theory.The potential energy surfaces visually describe the effect of different vibrational modes coupling on the molecular energy change,and the combined effect of the asymmetric stretching vibration of the S-H bond and the in-plane bending vibration makes the potential energy change range of the system significantly larger.The vibrational multi-reference configuration interaction method was used to calculate the anharmonic vibrational fre-quencies and vibrational spectrum,and the calculations showed that strong Fermi resonances appear between the overtones and combination bands,resulting in a significant enhancement of the infrared intensity at the corre-sponding bands.Finally,the photoelectron spectrum of H2S X1A1→H2S+ X2B1 was calculated for the first time using the Raman wave function and the contracted invariant Krylov subspaces method.This study will help to fur-ther understand the internal structure of interstellar molecules and provide a reference for experimental studies and interstellar observations.

Potential energy surfaceVMRCIVibrational spectroscopyPhotoelectron spectroscopy

郭甜、徐建刚、张佳美、张思雨、陈艳南、张云光

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西安邮电大学 理学院,西安 710121

势能面 VMRCI 振动光谱 光电子能谱

国家自然科学基金陕西省自然科学基金

221030612022JQ-569

2024

原子与分子物理学报
四川大学,四川省物理学会,中国物理学会原子与分子物理专业委员会

原子与分子物理学报

北大核心
影响因子:0.296
ISSN:1000-0364
年,卷(期):2024.41(4)
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