Lingjun Zhu, Qijing Zheng, Yingqi Wang, Kerstin Krüger, Alec M. Wodtke, Oliver Bünermann, Jin Zhao*, Hua Guo* and Bin Jiang*,
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引用次数: 0
Abstract
To understand the recently observed enigmatic nonadiabatic energy transfer for hyperthermal H atom scattering from a semiconductor surface, Ge(111)c(2 × 8), we present a mixed quantum-classical nonadiabatic molecular dynamics model based on the time-dependent evolution of Kohn–Sham orbitals and a classical path approximation. Our results suggest that facile nonadiabatic electronic transitions from the valence band to the conduction band occur selectively at the rest atom site, where surface states are doubly occupied, but not at the adatom site, where empty surface states are localized. This drastic site specificity can be attributed to the changes of the local band structure upon energetic H collisions at different surface sites, leading to transient near degeneracies and significant couplings between occupied and unoccupied orbitals at the rest atom but not at the adatom. These insights shed valuable light on the collision-induced nonadiabatic dynamics at semiconductor surfaces.
为了理解最近观测到的半导体表面 Ge(111)c(2×8)超热 H 原子散射的神秘非绝热能量转移,我们提出了一个基于 Kohn-Sham 轨道随时间演变和经典路径近似的混合量子经典非绝热分子动力学模型。我们的研究结果表明,从价带到导带的简便非绝热电子跃迁选择性地发生在原子静止位点,在那里表面态被双重占据,而不是在原子位点,在那里空的表面态被局部化。这种剧烈的位点特异性可归因于在不同的表面位点发生高能 H 碰撞时局部能带结构的变化,从而导致瞬时的近变性以及在原子位点(而非原子位点)有占据轨道和无占据轨道之间的显著耦合。这些见解为研究半导体表面碰撞诱导的非绝热动力学提供了宝贵的启示。