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首页> 外文期刊>Journal of Electron Spectroscopy and Related Phenomena >Effective attenuation lengths for photoelectrons emitted by high-energy laboratory X-ray sources
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Effective attenuation lengths for photoelectrons emitted by high-energy laboratory X-ray sources

机译:高能实验室X射线源发出的光电子的有效衰减长度

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摘要

We report calculations of effective attenuation lengths (EALs) for Si 2s(1/2), Cu 2p(3/2), Ag 3d(5/2), and Au 4f(7/2) photoelectrons excited by Mg K alpha, Al K alpha, Zr L alpha, and Ti K alpha X-rays, where the photoelectron energies ranged from 321 eV to 4.426 keV. These EALs, appropriate for determining overlayer-film thicknesses, were calculated from the transport-approximation formalism and from Monte Carlo simulations using photoionization cross sections from the dipole and non-dipole approximations. Satisfactory consistency was found between EALs determined from the TA formalism and from MC simulations, while differences between EALs for Au 4f(7/2) photoelectrons from the dipole and non-dipole approximations were between 1% (for Mg and Al K alpha X-rays) and 2.5% (for Ti K alpha X-rays) for photoelectron emission angles less than 50 degrees. As in past work for electron energies less than 2 key, we found a simple linear relation between the ratio of the average EAL (for emission angles less than 50 degrees) to the inelastic mean free path (IMFP) and the single-scattering albedo, a function of the IMFP and the transport mean free path. The root-mean-square difference between our average EALs and those from the linear expression was 1.44%. This expression should be useful in determinations of film thicknesses by XPS with unpolarized X-rays for photoelectron energies up to about 5 key. (C) 2015 Elsevier B.V. All rights reserved.
机译:我们报告了由Mg K alpha激发的Si 2s(1/2),Cu 2p(3/2),Ag 3d(5/2)和Au 4f(7/2)光电子的有效衰减长度(EAL)的计算, Al K alpha,Zr L alpha和Ti K alpha X射线,其中光电子能量范围为321 eV至4.426 keV。这些EAL适用于确定覆盖层的膜厚,是根据传输近似形式和蒙特卡罗模拟(使用来自偶极和非偶极近似的光电离横截面)计算得出的。从TA形式主义和MC模拟确定的EAL之间发现令人满意的一致性,而偶极和非偶极近似的Au 4f(7/2)光电子的EAL之间的差异在1%之间(对于Mg和Al K alpha X-射线)和2.5%(对于Ti KαX射线)小于50度的光电子发射角。与过去的电子能量小于2键的工​​作一样,我们发现平均EAL(对于小于50度的发射角)与非弹性平均自由程(IMFP)的比与单散射反照率之间存在简单的线性关系, IMFP和运输平均自由程的函数。我们的平均EAL与来自线性表达式的EAL的均方根差为1.44%。该表达式在通过XPS用非偏振X射线测定高达约5键的光电子能量的膜厚中应该是有用的。 (C)2015 Elsevier B.V.保留所有权利。

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