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Scattering and dissociative adsorption of H_(2) on the armchair and zigzag edges of graphite

机译:H_(2)在石墨的扶手椅和锯齿形边缘上的散射和解离吸附

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摘要

We performed quantum dynamics calculations on the scattering and dissociative adsorption of hydrogen molecules incident on the armchair and zigzag edges of graphite layers, using relevant potential-energy surfaces (PESs) recently obtained by Dino et al. [e-J. Surf. Sci. Nanotech. 2, 77 (2003), and references therein]. By employing the coupled channel method to determine the reflection and sticking probabilities, we compared the hydrogen scattering and dissociative adsorption dynamics on the two graphite surfaces. Our findings show the different scattering behaviors of H_(2) for the armchair edge and for the zigzag edge, which enable the identification of an unknown graphite edge from its interaction with H_(2). The scattering on the zigzag edge is due to the highly curved region of the PES reaction path for H_(2) interacting with the zigzag edge, whereas the scattering for the armchair edge is caused by a potential barrier. The reflection probability initially decreases with increasing the kinetic energy in both cases but gradually increases for the zigzag edge. Our findings also indicate that the zigzag edge can adsorb hydrogen better than the armchair edge, mainly due to the absence (presence) of an activation barrier in the zigzag (armchair) edge. There is a very weak dependence of the sticking probability on the initial vibrational state of H_(2) for both graphite edges. The difference in the vibrational effect is due to the relative position of the curved region with respect to the potential barrier (well).
机译:我们使用Dino等人最近获得的相关势能表面(PES),对入射在石墨层的扶手椅和锯齿形边缘上的氢分子的散射和解离吸附进行了量子动力学计算。 [e-J。冲浪。科学纳米技术。 2,77(2003),及其中的参考文献]。通过使用耦合通道方法确定反射和粘附的可能性,我们比较了两个石墨表面上的氢散射和解离吸附动力学。我们的发现表明,扶手椅边缘和锯齿形边缘的H_(2)散射行为不同,这使得能够根据与H_(2)的相互作用识别未知的石墨边缘。锯齿形边缘的散射是由于PE_H2(2)与锯齿形边缘相互作用的PES反应路径的高度弯曲区域引起的,而扶手椅扶手椅边缘的散射是由势垒引起的。在这两种情况下,反射概率最初都随着动能的增加而减小,但对于之字形边缘,反射概率逐渐增大。我们的发现还表明,之字形边缘比扶手椅形边缘能更好地吸收氢,这主要是由于之字形(扶手椅形)边缘中不存在(存在)激活屏障。对于两个石墨边缘,粘附概率对H_(2)的初始振动状态的依赖性都非常弱。振动效果的差异归因于弯曲区域相对于势垒(阱)的相对位置。

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