金属薄膜的自由电子理论

Philip B. Allen
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引用次数: 0

摘要

量子自由电子,即波长为 k 的平面波,其占位受保利排除原理的限制,在有关固体的所有介绍性文字中都有解释。对 "简单 "金属特性的自由电子描述效果出奇地好。我们假定金属的内部基本上是无限的,表面被认为是无关紧要的。过去 30 年来,表面可视化实验彻底改变了固态物理学,激发了新的理论和应用。因此,一个基本问题是,如何将自由电子图景应用于表面起着重要作用的固体性质?人们使用了各种版本的扩展自由电子理论,但并不总能从教学角度加以解释。本文重点讨论理想化的金属薄膜。本文给出了金属膜自由电子描述的三个版本(一个过于简化的版本和两个改进阶段)。本文以具有六层原子的铝板为例,详细说明了这些版本。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Free Electron Theory for Thin Metal Films
Quantum free electrons, i.e. plane waves, with wavevector k, and occupancy constrained by the Pauli exclusion principle, are explained in all introductory texts about solids. A free-electron description works surprisingly well for many properties of "simple" metals. It is assumed that the interior of the metal is essentially infinite, and surfaces are presumed irrelevant. Over the past 30 years, experiments that visualize surfaces have revolutionized solid state physics, stimulating new theory and applications. Therefore, a basic question is, how can the free electron picture be applied to properties of solids where surfaces play a prominent role? Various versions of an extended free-electron theory are used, but not always explained pedagogically. This paper focusses on idealized metallic films. Three versions (an oversimplified one and two stages of improvement) of a free-electron description of metal films are given. These versions are illustrated in detail for the specific example of a slab of aluminum with six layers of atoms.
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