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THEORETICAL STUDY ON THE PHOTOSTIMULATED DESORPTION OF CO FROM A PT SURFACE

机译:PT表面光解CO的理论研究

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Photostimulated desorptions (PSD's) of CO, CO+, and CO- from a Pt surface are studied theoretically using Pt-2-CO model cluster including image force correction. Calculations are performed by the single excitation configuration interaction and the symmetry adapted cluster (SAC)/SAC-CI methods. The PSD's of the ground state CO occur as the Menzel-Gomer-Redhead (MGR) process and those of CO+ (n cation) and excited (n-->pi*) CO* through the modified MGR process in which the upper repulsive potential curves are nonadiabatic; the process proceeds through a sequence of nonadiabatic transitions between the similar pertinent states embedded in the metal excited bands. The excited states as the desorption channels are characterized by the excitations from the Pt-CO bonding orbitals to the antibonding MO's: metal-adsorbate chemical bond cleavage by photons which leads to a repulsive potential is essential for the PSD. The electrostatic image force interaction plays only a minor role and the present result does not support the Antoniewicz model. The calculated excitation-energy thresholds for the CO, CO+, and CO* desorptions are 1.6 similar to 2.6, 11.3, and 11.3-12.7 eV, respectively, which explains the energy thresholds and the fluence dependencies of the incident laser in the PSD experiments. On the other hand, the PSD giving CO- would occur with the energy range of 6.2-8.2 eV, one to two photon energy of the 193 nm (6.4 eV) laser. Since the upper nonadiabatic potential curves have shallow minima, in this case, the lifetime of the CO- species would be larger than those of the CO+ and CO* species. The present study clarifies the electronic structures of the desorbed CO+, CO-, and CO* species, which have not been identified experimentally. (C) 1996 American Institute of Physics. [References: 46]
机译:使用包括图像力校正在内的Pt-2-CO模型集群,从理论上研究了Pt表面上CO,CO +和CO-的光刺激解吸(PSD)。计算是通过单个激发配置相互作用和对称适应性群集(SAC)/ SAC-CI方法进行的。基态CO的PSD发生为Menzel-Gomer-Redhead(MGR)过程,而CO +(n阳离子)和激发(n-> pi *)CO *的PSD通过改进的MGR过程产生,其中上排斥力曲线是非绝热的;该过程通过嵌入在金属激发能带中的相似相关态之间的一系列非绝热跃迁进行。作为解吸通道的激发态的特征是从Pt-CO键轨道到反键MO的激发:光子对金属-吸附物的化学键裂解,导致PSD的排斥势必不可少。静电像力相互作用仅起次要作用,目前的结果不支持Antoniewicz模型。计算出的CO,CO +和CO *解吸的激发能量阈值分别为1.6、2.6、11.3和11.3-12.7 eV,这说明了PSD实验中的能量阈值和入射激光的注量依赖性。另一方面,产生CO-的PSD的能量范围为6.2-8.2 eV,这是193 nm(6.4 eV)激光的一到两个光子能量。由于较高的非绝热势曲线具有极小的最小值,因此在这种情况下,CO-物种的寿命将大于CO +和CO *物种的寿命。本研究阐明了解吸的CO +,CO-和CO *物种的电子结构,目前尚未通过实验确定。 (C)1996年美国物理研究所。 [参考:46]

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