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首页> 外文期刊>Physical review. B, Condensed Matter And Materials Physics >First-principles calculation of charge transfer at surfaces: The case of core-excited Ar~*(2p_(3/2)~(-1)4s) on Ru(0001)
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First-principles calculation of charge transfer at surfaces: The case of core-excited Ar~*(2p_(3/2)~(-1)4s) on Ru(0001)

机译:表面电荷转移的第一性原理计算:Ru(0001)上核激发Ar〜*(2p_(3/2)〜(-1)4s)的情况

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摘要

We present an ab initio scheme for the calculation of the resonant charge transfer of electrons at surfaces. The electron initially resides in a bound resonance, i.e., appearing below the vacuum level, associated with a core-excited adsorbate. Our treatment is based on first-principles density-functional calculations of this initial situation using finite slabs. These results are combined with bulk calculations of the substrate material to obtain the Hamiltonian of the semi-infinite system in which the electron evolves. Therefore, we include a realistic description of the electronic structure of both subsystems, substrate and adsorbate, and the interaction between them. The surface Green's function is then computed using the transfer matrix method and projected onto a wave packet localized in the adsorbate. The width and energy of the resonance can be obtained from an analysis of the projected Green's function, and the charge transfer time can be estimated. The calculated width is independent of the wave packet used for the projection, at least as far as there are not several overlapping resonances at neighboring energies. Alternatively, one can directly calculate the time evolution of the population of the initial wave packet. Both alternatives are presented and compared. Our first-principles calculations are based on periodic arrangements of adsorbates on the surface. With an appropriate average of the k_‖ resolved results, one can extrapolate to the limit of an isolated adsorbate. We discuss several possibilities to do this. As an application, we focus on the case of the As bound resonance of a core-excited Ar~* (2p_(3/2)~(-1)4s) adsorbate on Ru(0001), for which there are extensive experimental studies. The calculated values and trends are in good agreement with the experimental observations.
机译:我们提出了一个从头算方案,用于计算表面电子的共振电荷转移。电子最初驻留在与核激发的吸附物相关的束缚共振中,即出现在真空能级以下。我们的处理是基于使用有限平板对这种初始情况的第一性原理密度函数计算。这些结果与衬底材料的体积计算相结合,以获得电子在其中演化的半无限系统的哈密顿量。因此,我们对这两个子系统的电子结构(衬底和被吸附物)以及它们之间的相互作用进行了实际描述。然后使用转移矩阵方法计算表面格林函数,并将其投影到位于被吸附物中的波包上。共振的宽度和能量可以从对格林函数的预测分析中获得,并且可以估计电荷转移时间。所计算的宽度至少与用于投影的波包无关,只要在相邻能量处没有多个重叠共振即可。或者,可以直接计算初始波包的时间演变。提出并比较了两种选择。我们的第一原理计算是基于表面上吸附物的周期性排列。有了k_′个解析结果的适当平均值,就可以推断出一个孤立的吸附物的极限。我们讨论了执行此操作的几种可能性。作为应用,我们重点研究了Ru(0001)上被核激发的Ar〜*(2p_(3/2)〜(-1)4s)吸附物的As结合共振的情况,对此进行了广泛的实验研究。 。计算值和趋势与实验观察结果非常吻合。

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