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作 者:高倩 陈俊杰 胡茜茜 谢代前[2,3] Qian Gao;Junjie Chen;Xixi Hu;Daiqian Xie(Kuang Yaming Honors School,Jiangsu Key Laboratory of Vehicle Emissions Control,Nanjing University,Nanjing 210023,China;Institute of Theoretical and Computational Chemistry,Key Laboratory of Mesoscopic Chemistry,School of Chemistry and Chemical Engineering,Nanjing University,Nanjing 210023,China;Hefei National Laboratory,Hefei 230088,China)
机构地区:[1]南京大学匡亚明学院,江苏省机动车尾气污染控制重点实验室,南京210023 [2]南京大学化学化工学院,理论与计算化学研究所,介观化学教育部重点实验室,南京210023 [3]合肥国家实验室,合肥230088
出 处:《Chinese Journal of Chemical Physics》2024年第2期221-229,I0102,共10页化学物理学报(英文)
基 金:This work was supported by the Innovation Program for Quantum Science and Technology(2021ZD0303305 to Daiqian Xie);by the National Natural Science Foundation of China(No.22073042 and No.22122302 to Xixi Hu,No.22233003 and No.22241302 to Daiqian Xie)。
摘 要:本文利用切比雪夫实波包法研究了不同初始振动态下H_(2)S第一吸收带的光解量子动力学。由于初始振动态的波函数不同,计算得到的吸收光谱以及产物的振动态分布表现出不同的动力学特性,由于角坐标波函数的变化,初始伸缩振动激发态(1,0,0)和(0,0,1)的吸收光谱宽度和峰值与振动基态不同,而(0,1,0)振动态的吸收光谱中有两个几乎同样高的峰值.(0,1,0)态的产物振动态分布对激发能量的依赖不强,并由V=0的产物主导,但在(1,0,0)和(0,0,1)振动态的较低能量处占主导的产物是SH(X,V=1)碎片,产物的转动态分布对总能量的依讨赖性较弱,且分布非常冷并在j=1处达到峰值,但(0,1,0)振动态的转动态分布表现出明显的振荡,其各向异性参数随转动量子数的振荡行为不同于其他三种振动态的各向异性参数.The photodissociation quantum dynamics for the first absorption band of H_(2)S in different initial vibrational states have been investigated using Chebyshev real wave packet method.Because of the difference of the wave functions for the initial vibrational states,the calculated absorption spectra and the distributions of vibrational and rotational state of the products display different dynamic characteristics.The width and peak position of the absorption spectra for initial stretching excited states(1,0,0)and(0,0,1)are different from that of the vibrational ground state,while the(0,1,0)vibrational state has two almost equally high peaks in its absorption spectrum because of the change of wave function in angular coordinate.The product vibrational state distribution for(0,1,0)initial state weakly depends on the excitation energy and is dominated by the products of v=0,but SH(v=1)fragment is dominant at lower energy for(1,0,0)and(0,0,1)vibrational states.The rotational state distributions of products are very cold with the peak at j=1 for these four states and weakly depend on the total energy.Besides,the rotational state distribution from(0,1,0)vibrational state displays strong oscillation,and its anisotropic parameter with rotational quantum numbers is also different from that of the other three vibrational states.
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