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使用实验室X射线源确定薄膜的对分布函数。

Determining pair distribution functions of thin films using laboratory-based X-ray sources.

作者信息

Bylin Johan, Kapaklis Vassilios, Pálsson Gunnar K

机构信息

Division of Materials Physics, Department of Physics and Astronomy, Uppsala University, Box 516, 75 121Uppsala, Sweden.

出版信息

J Appl Crystallogr. 2024 Aug 30;57(Pt 5):1373-1383. doi: 10.1107/S1600576724006368. eCollection 2024 Oct 1.

DOI:10.1107/S1600576724006368
PMID:39387074
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11460393/
Abstract

This article demonstrates the feasibility of obtaining accurate pair distribution functions of thin amorphous films down to 80 nm, using modern laboratory-based X-ray sources. The pair distribution functions are obtained using a single diffraction scan without the requirement of additional scans of the substrate or of the air. By using a crystalline substrate combined with an oblique scattering geometry, most of the Bragg scattering of the substrate is avoided, rendering the substrate Compton scattering the primary contribution. By utilizing a discriminating energy filter, available in the latest generation of modern detectors, it is demonstrated that the Compton intensity can further be reduced to negligible levels at higher wavevector values. Scattering from the sample holder and the air is minimized by the systematic selection of pixels in the detector image based on the projected detection footprint of the sample and the use of a 3D-printed sample holder. Finally, X-ray optical effects in the absorption factors and the ratios between the Compton intensity of the substrate and film are taken into account by using a theoretical tool that simulates the electric field inside the film and the substrate, which aids in planning both the sample design and the measurement protocol.

摘要

本文展示了使用基于现代实验室的X射线源获取低至80纳米的非晶薄膜精确对分布函数的可行性。对分布函数通过单次衍射扫描获得,无需对衬底或空气进行额外扫描。通过使用晶体衬底结合倾斜散射几何结构,避免了衬底的大部分布拉格散射,使衬底康普顿散射成为主要贡献。利用最新一代现代探测器中可用的鉴别能量滤波器,结果表明在更高波矢值下,康普顿强度可进一步降低到可忽略不计的水平。通过基于样品的投影检测足迹在探测器图像中系统地选择像素以及使用3D打印样品架,将来自样品架和空气的散射降至最低。最后,通过使用一种理论工具来模拟薄膜和衬底内部的电场,考虑吸收因子中的X射线光学效应以及衬底与薄膜的康普顿强度之比,这有助于规划样品设计和测量方案。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/82c7/11460393/4892264af909/j-57-01373-fig9.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/82c7/11460393/38523aaae280/j-57-01373-fig1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/82c7/11460393/112f25b3cdb3/j-57-01373-fig2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/82c7/11460393/308ef53be10e/j-57-01373-fig3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/82c7/11460393/83c6e357886d/j-57-01373-fig4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/82c7/11460393/bd4d862bf8ac/j-57-01373-fig5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/82c7/11460393/6176d8a53068/j-57-01373-fig6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/82c7/11460393/e8fd24bca7d2/j-57-01373-fig7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/82c7/11460393/86d005f480fa/j-57-01373-fig8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/82c7/11460393/4892264af909/j-57-01373-fig9.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/82c7/11460393/38523aaae280/j-57-01373-fig1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/82c7/11460393/112f25b3cdb3/j-57-01373-fig2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/82c7/11460393/308ef53be10e/j-57-01373-fig3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/82c7/11460393/83c6e357886d/j-57-01373-fig4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/82c7/11460393/bd4d862bf8ac/j-57-01373-fig5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/82c7/11460393/6176d8a53068/j-57-01373-fig6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/82c7/11460393/e8fd24bca7d2/j-57-01373-fig7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/82c7/11460393/86d005f480fa/j-57-01373-fig8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/82c7/11460393/4892264af909/j-57-01373-fig9.jpg

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