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首页> 外文期刊>The Journal of Chemical Physics >PHOTODISSOCIATION OF OZONE IN THE CHAPPUIS BAND .2. TIME-DEPENDENT WAVE-PACKET CALCULATIONS AND INTERPRETATION OF DIFFUSE VIBRATIONAL STRUCTURES
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PHOTODISSOCIATION OF OZONE IN THE CHAPPUIS BAND .2. TIME-DEPENDENT WAVE-PACKET CALCULATIONS AND INTERPRETATION OF DIFFUSE VIBRATIONAL STRUCTURES

机译:光谱带中臭氧的光解离作用.2。时变波包计算和弥散振动结构的解释

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We present time-dependent wave-packet calculations describing the photodissociation of ozone in the Chappuis band, which evolves in the two lowest states of (1)A '' symmetry. The calculations are performed in the diabatic representation and include the coupling between the two relevant states. All three nuclear degrees of freedom are taken into account. The two potentiaI-energy surfaces, the coupling potential, and the two transition-dipole-moment functions with the electronic ground state have been calculated previously by ab initio methods [Woywod er nl., J. Chem. Phys. 107, 7282 (1997)]. The coupling between the two diabatic states is exceedingly strong, resulting in very fast dissociation into O+O-2 on the time scale of only one symmetric stretch period. A small portion of the initially created wave packet is temporarily trapped leading to three tiny recurrences, which reflect basically symmetric stretch motion plus same amount of bending motion. The experimentally observed diffuse vibrational structures superimposed to the broad absorption spectrum are satisfactorily reproduced and discussed both in the time-independent and the time-dependent picture of spectroscopy. In view of the very short lifetime in the excited states, the correspondingly large widths of the diffuse structures, and the participation of all three vibrational modes we conclude that an unique assignment in terms of three quantum numbers is not possible. The main structures are due to symmetric stretch excitation, but bending and even asymmetric stretch motion are also involved. A one-state model, in which only the upper (bound) adiabatic potential is employed, provides a qualitatively correct explanation of the absorption spectrum and the diffuse structures. (C) 1997 American Institute of Physics. [References: 33]
机译:我们提出了随时间变化的波包计算方法,描述了Chappuis波段中臭氧的光解离,该光解以(1)A''对称的两个最低状态演化。该计算以非绝热表示形式进行,包括两个相关状态之间的耦合。所有三个核自由度都被考虑在内。先前已经通过从头开始的方法[Woywod er nl。,J.Chem.Soc.Sci。,Vol.26,No.5,pp.1,1986]来计算出两个电势能表面,耦合电势以及两个具有电子基态的跃迁偶极矩函数。物理107,7282(1997)]。两种非绝热状态之间的耦合非常强,导致仅在一个对称伸展期的时间尺度上即可非常快速地解离为O + O-2。最初创建的波包的一小部分被暂时捕获,导致三个微小的重复,这反映了基本对称的拉伸运动加上相同量的弯曲运动。在与时间无关的光谱和与时间有关的光谱图中,可以令人满意地重现和讨论叠加到宽吸收光谱上的实验观察到的漫振动结构。鉴于激发态的寿命非常短,扩散结构的宽度相应较大以及所有三个振动模式的参与,我们得出结论,就三个量子数而言,唯一的分配是不可能的。主要结构归因于对称的拉伸激励,但也涉及弯曲甚至不对称的拉伸运动。一种仅使用上限(结合)绝热势能的单态模型,从质量上正确地解释了吸收光谱和扩散结构。 (C)1997美国物理研究所。 [参考:33]

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