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一维势垒中电子输运的比较研究与场发射问题相关。

A comparative study of the electron transmission through one-dimensional barriers relevant to field-emission problems.

机构信息

FUNDP-University of Namur, Rue de Bruxelles 61, B-5000 Namur, Belgium.

出版信息

J Phys Condens Matter. 2010 May 5;22(17):175007. doi: 10.1088/0953-8984/22/17/175007. Epub 2010 Apr 7.

DOI:10.1088/0953-8984/22/17/175007
PMID:21393665
Abstract

We study the transmission coefficient of one-dimensional barriers that are relevant to field-emission problems. We compare, in particular, the results provided by the simple Jeffreys-Wentzel-Kramers-Brillouin (JWKB) approximation, the continued-fraction technique and the transfer-matrix methodology for the electronic transmission through square, triangular and Schottky-Nordheim barriers (the Schottky-Nordheim barrier is often used in models of field emission from flat metals). For conditions that are typical of field emission (Fermi energy of 10 eV, work function of 4.5 eV and field strength of 5 V nm(-1)), it is shown that the simple JWKB approximation must be completed by an effective prefactor P(eff) in order to match the exact quantum-mechanical result. This prefactor takes typical values around 3.4 for square barriers, 1.8 for triangular barriers and 0.84 for the Schottky-Nordheim barrier. For fields F between 1 and 10 V nm(-1) and for work functions φ between 1 and 5 eV, the prefactor P(eff) to consider in the case of the Schottky-Nordheim barrier actually ranges between 0.28 and 0.98. This study hence demonstrates that the Fowler-Nordheim equation (in its standard form that accounts for the image interaction and that actually relies on the simple JWKB approximation) overestimates the current emitted from a flat metal by a factor that may be of the order of 2-3 for the conditions considered in this work. The study thus confirms Forbes's opinion that this prefactor should be reintegrated in field-emission theories.

摘要

我们研究了与场发射问题相关的一维势垒的透射系数。我们特别比较了简单的杰弗里-温策尔-克拉默斯-布里渊(JWKB)近似、连分式技术和转移矩阵方法在通过方形势垒、三角形势垒和肖特基-诺德海姆势垒(肖特基-诺德海姆势垒常用于平面金属的场发射模型)的电子透射中的结果。对于典型的场发射条件(费米能为 10 eV,功函数为 4.5 eV,场强为 5 V nm(-1)),我们发现简单的 JWKB 近似必须通过有效预因子 P(eff)来完成,以便与精确的量子力学结果匹配。这个预因子对于方形势垒的典型值约为 3.4,三角形势垒的为 1.8,肖特基-诺德海姆势垒的为 0.84。对于 1 到 10 V nm(-1)之间的场强 F 和 1 到 5 eV 之间的功函数 φ,肖特基-诺德海姆势垒中要考虑的预因子 P(eff)实际上在 0.28 到 0.98 之间。因此,这项研究表明,在考虑到本工作条件的情况下,福勒-诺德海姆方程(其考虑了镜像相互作用并实际上依赖于简单 JWKB 近似的标准形式)高估了从平面金属发射的电流,其因子可能在 2-3 左右。因此,这项研究证实了福布斯的观点,即应该在场发射理论中重新整合这个预因子。

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