首页> 外文期刊>The Journal of Chemical Physics >Isotope effects in the dissociation of the (B)over-tilde(1)A(1) state of SiH2, SiHD, and SiD2 using three-dimensional wave packet propagation
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Isotope effects in the dissociation of the (B)over-tilde(1)A(1) state of SiH2, SiHD, and SiD2 using three-dimensional wave packet propagation

机译:使用三维波包传播,SiH2,SiHD和SiD2的(B)over-tilde(1)A(1)状态解离中的同位素效应

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Dissociations after the A B-1(1)-> B (1)A(1) photoexcitation of SiH2, SiHD, and SiD2 were studied to investigate excited-state dynamics and effects of the initial vibrational state. The cross section (sigma) for the photodissociation relative to SiH2(B)-> Si(D-1)+H-2 and the rovibrational population of the H-2 fragment were computed using the wave packet propagation technique based on the three-dimensional potential energy surfaces (PESs) of the A and B electronic states and the transition dipole surfaces, which were reported in our previous paper [J. Chem. Phys. 122, 144307 (2005)]. The photodissociation spectrum consists of a broadband and a number of sharp peaks. For SiH2 and SiD2, the sharp peaks correspond to the resonance structure of the vibrational levels of the B state and the broadbands are nearly independent of the photon energy. The broadband for SiHD increases steeply with the photon energy above 30 000 cm(-1). The flux leaving the computational grid for SiH2 and SiD2 consists of at least two components, whereas that for SiHD consists of only a faster component. These large isotope effects were discussed based on the valley to the dissociation channel on PES and the difference in the position of the initial wave packet for three isotopomers. (c) 2006 American Institute of Physics.
机译:研究了SiH2,SiHD和SiD2的A B-1(1)-> B(1)A(1)光激发后的解离,以研究激发态动力学和初始振动态的影响。相对于SiH2(B)-> Si(D-1)+ H-2的光解离的横截面(sigma)和H-2片段的旋振种群是使用波包传播技术基于以下三种方法计算的: A和B电子态的尺寸势能面(PESs)和跃迁偶极面,在我们以前的论文中已有报道[J.化学物理122,144307(2005)]。光解离光谱由宽带和许多尖峰组成。对于SiH2和SiD2,尖峰对应于B状态振动能级的共振结构,而宽带几乎与光子能量无关。随着光子能量超过30000 cm(-1),SiHD的宽带急剧增加。离开计算网格的SiH2和SiD2的通量至少包含两个分量,而SiHD的通量仅包含较快的分量。讨论了这些大的同位素效应,是基于PES上解离通道的波谷以及三种同位素异构体的初始波包位置的差异。 (c)2006年美国物理研究所。

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