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首页> 外文期刊>The Journal of Chemical Physics >ELECTRONICALLY DIABATIC QUANTUM DYNAMICS OF MOLECULAR DESORPTION [Review]
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ELECTRONICALLY DIABATIC QUANTUM DYNAMICS OF MOLECULAR DESORPTION [Review]

机译:分子吸附的电子绝热量子动力学[综述]

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The photodesorption of a diatomic from a metal surface, following absorption of visible or UV light, involves electronic transitions of the desorbing species coupled to the lattice vibrations and electron-hole excitations of the substrate. We present a general treatment of these phenomena, based on the Liouville-Von Neuman equation for the density operator, and a stochastic theory of localized perturbations in an extended system. The Hamiltonian of the extended molecular system is divided into a term for the localized primary degrees of freedom (DFs) affected by the desorption, coupled to secondary DFs that acts as a time-evolving bath. A self-consistent field treatment gives an effective (non-Hermitian) Hamiltonian for the primary DFs that accounts for energy fluctuation and dissipation in terms of the properties of adsorbate and substrate. A diabatic electronic representation is used to eliminate momentum couplings between adsorbate electronic states. The bath dynamics is studied for lattice vibrations and for electronic excitations. Electron-hole excitations of the substrate are considered for intraband and interband transitions. The assumption of Brownian motion leads to expressions for the dissipative potentials in terms of the time-correlation functions of lattice displacements and of electron density fluctuations. The dissipation depends on time, allowing for time-dependent substrate temperatures and generalizing the Langevin description. Dissipation contributes to the time evolution of both ground and excited electronic states of the desorbing species. The model is discussed for the special case of Ni(001)(ads)CO. (C) 1995 American Institute of Physics. [References: 111]
机译:在吸收可见光或紫外光之后,金属原子上的双原子光解吸涉及与基体的晶格振动和电子空穴激发耦合的解吸物质的电子跃迁。我们基于密度算符的Liouville-Von Neuman方程和扩展系统中局部扰动的随机理论,给出了对这些现象的一般处理。扩展分子系统的哈密顿量分为受解吸影响的局部初级自由度(DFs)术语,该次级自由度与充当时间演化浴的次级DFs耦合。自洽场处理为主要DF提供了有效的(非Hermitian)哈密顿量,从而根据吸附物和基质的性质考虑了能量波动和耗散。非绝热电子表示用于消除被吸附物电子态之间的动量耦合。研究了熔池动力学的晶格振动和电子激发。对于带内和带间过渡,考虑了衬底的电子空穴激发。布朗运动的假设根据晶格位移和电子密度波动的时间相关函数得出了耗散势的表达式。耗散取决于时间,从而允许随时间变化的基板温度并推广Langevin描述。耗散有助于解吸物质的基态和激发电子态的时间演化。针对Ni(001)(ads)CO的特殊情况讨论了该模型。 (C)1995年美国物理研究所。 [参考:111]

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