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Exact electronic properties in the classically forbidden region of a metal surface

机译:在金属表面的经典禁区中的精确电子性能

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We derive exact properties of the inhomogeneous electron gas in the asymptotic classically forbidden region at a metal-vacuum interface within the framework of local effective potential energy theory. We derive a new expression for the asymptotic structure of the Kohn-Sham density functional theory (KS-DFT) exchange-correlation potential energy v(xc)(r) in terms of the irreducible electron self-energy. We also derive the exact asymptotic structure of the orbitals, density, the Dirac density matrix, the kinetic energy density, and KS exchange energy density. We further obtain the exact expression for the Fermi hole and demonstrate its structure in this asymptotic limit. The exchange-correlation potential energy is derived to be v(xc)(z -> infinity) = -alpha(KS,xc)/z, and its exchange and correlation components to be v(xc)(z -> -a(KS,x)/z and v(c)(z -> infinity) = -a(KS,c)/z, respectively. The analytical expressions for the coefficients a(KS,xc) and a(KS,x) show them to be dependent on the bulk-metal Wigner-Seitz radius and the barrier height at the surface. The coefficient alpha(KS,c) = 1/4 is determined in the plasmon-pole approximation and is independent of these metal parameters. Thus, the asymptotic structure of v(xc)(z) in the vacuum region is image-potential-like but not the commonly accepted one of -1/4z. Furthermore, this structure depends on the properties of the metal. Additionally, an analysis of these results via quantal density functional theory (Q-DFT) shows that both the Pauli W-x(z -> infinity) and lowest-order correlation-kinetic W-t((1))(z -> infinity) components of the exchange potential energy v(x)(z -> infinity) and the Coulomb W-c(z -> infinity and higher-order correlation-kinetic components of the correlation potential energy v(c)(z -> infinity), all contribute terms of O(1/z) to the structure. Hence correlations attributable to the Pauli exclusion principle, Coulomb repulsion, and correlation-kinetic effects all contribute to the asymptotic structure of the effective potential energy at a metal surface. The relevance of the results derived to the theory of image states and to KS-DFT is also discussed. (c) 2005 Wiley Periodicals, Inc.
机译:我们在局部有效势能理论的框架内,得出了金属-真空界面上渐近经典禁区中非均匀电子气的确切性质。我们用不可还原的电子自能,推导了Kohn-Sham密度泛函理论(KS-DFT)交换相关势能v(xc)(r)的渐近结构的新表达式。我们还导出了轨道,密度,狄拉克密度矩阵,动能密度和KS交换能量密度的精确渐近结构。我们进一步获得了费米孔的精确表达式,并证明了它在此渐近极限中的结构。交换相关势能导出为v(xc)(z->无穷大)= -alpha(KS,xc)/ z,其交换和相关分量为v(xc)(z-> -a( KS,x)/ z和v(c)(z-> infinity)= -a(KS,c)/ z。系数a(KS,xc)和a(KS,x)的解析表达式显示它们取决于大块金属的Wigner-Seitz半径和表面的势垒高度,在等离振子极点近似中确定系数alpha(KS,c)= 1/4,并且与这些金属参数无关。 ,真空区域中的v(xc)(z)的渐近结构是像电势似的,但不是通常公认的-1 / 4z之一,而且,这种结构还取决于金属的特性。量子密度泛函理论(Q-DFT)得出的这些结果表明交换势能的Pauli Wx(z-> infinity)和最低阶相关动力学Wt((1))(z-> infinity)分量v(x)(z-> infinity)和库仑W- c(z->无穷大和相关势能v(c)(z-> infinity)的高阶相关运动分量都对结构贡献O(1 / z)项。因此,可归因于保利排斥原理,库仑斥力和相关动力学效应的相关性都有助于金属表面有效势能的渐近结构。还讨论了结果与图像状态理论和KS-DFT的相关性。 (c)2005年Wiley Periodicals,Inc.

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