Calculation of the emission depth distribution function for electrons emitted from a crystal by the Bloch wave method

被引:2
作者
Zeng, R. G.
Ding, Z. J. [1 ]
机构
[1] Univ Sci & Technol China, Hefei Natl Lab Phys Sci Microscale, Hefei 230026, Anhui, Peoples R China
基金
中国国家自然科学基金;
关键词
Depth distribution function; Electron emission; Diffraction effects; Crystal; MONTE-CARLO-SIMULATION; BACKSCATTERING FACTOR; ESCAPE PROBABILITY; DIFFRACTION; SCATTERING; PARAMETERIZATION; SPECTROSCOPY;
D O I
10.1016/j.susc.2012.09.022
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
The quantum mechanical Bloch-wave method combined with the reciprocity principle has been used to describe electron transport in crystalline solids for determining the emission depth distribution function (EMDDF) of signal electrons in surface electron spectroscopy. The crystal structure and electron coherent scattering are explicitly taken into account; these are neglected in classical Monte Carlo methods. While electron inelastic scattering is treated with an optical potential, the EMDDF for Auger-electron emission from an Au (001) surface is calculated by the quantum method. The dependence of the EMDDF on emission angle and crystal structure has indicated that this quantum EMDDF strongly depends on the emission direction of Auger electrons and is sensitive to crystal structure. Comparisons made between the present results and classical Monte Carlo simulation results show pronounced differences due to electron-diffraction effects. The mean escape depth (MED) which describes the surface sensitivity of Auger electron spectroscopy, is also evaluated; the present calculation shows that the MED for a crystalline solid is about half that for an amorphous solid from a Monte Carlo calculation. (C) 2012 Elsevier B.V. All rights reserved.
引用
收藏
页码:102 / 108
页数:7
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