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利用PSICHÉ的白光站结合X射线断层扫描、X射线衍射和X射线吸收对高压下的液体进行原位表征。

In situ characterization of liquids at high pressure combining X-ray tomography, X-ray diffraction and X-ray absorption using the white beam station at PSICHÉ.

作者信息

Henry L, Guignot N, King A, Giovenco E, Deslandes J P, Itié J P

机构信息

Synchrotron SOLEIL, L'Orme des Merisiers, Saint-Aubin, 91192 Gif-sur-Yvette, France.

Univ Lyon, UCBL, ENSL, UJM, CNRS, LGL-TPE, F-69622 Villeurbanne, France.

出版信息

J Synchrotron Radiat. 2022 May 1;29(Pt 3):853-861. doi: 10.1107/S1600577522003411. Epub 2022 Apr 25.

DOI:10.1107/S1600577522003411
PMID:35511017
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC9070723/
Abstract

A novel experimental setup dedicated to the study of liquid and amorphous materials, on the white beam station of the PSICHÉ beamline at SOLEIL, is described. The Beer-Lambert absorption method has been developed using a broad-spectrum (white) incident beam for in situ density measurements at extreme conditions of pressure and temperature. This technique has been combined with other existing X-ray techniques (radiographic imaging, tomography and combined angle energy dispersive X-ray diffraction). Such a multi-technical approach offers new possibilities for the characterization of liquid and amorphous materials at high pressure and high temperature. The strength of this approach is illustrated by density measurements of liquid gallium at pressures up to 4 GPa, combining the three independent X-ray techniques (the Beer-Lambert absorption method, tomography and X-ray diffraction).

摘要

本文描述了一种用于研究液体和非晶态材料的新型实验装置,该装置位于索莱伊(SOLEIL)的PSICHÉ光束线的白光站。已开发出利用宽谱(白色)入射光束的比尔-朗伯吸收法,用于在极端压力和温度条件下进行原位密度测量。该技术已与其他现有的X射线技术(射线成像、断层扫描和组合角度能量色散X射线衍射)相结合。这种多技术方法为高压和高温下液体和非晶态材料的表征提供了新的可能性。通过结合三种独立的X射线技术(比尔-朗伯吸收法、断层扫描和X射线衍射)对高达4 GPa压力下的液态镓进行密度测量,说明了这种方法的优势。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d50b/9070723/d7d014c4f6e8/s-29-00853-fig8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d50b/9070723/6c21fbece06f/s-29-00853-fig1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d50b/9070723/0f0b1a9fa1fc/s-29-00853-fig2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d50b/9070723/d75242c3bbd3/s-29-00853-fig3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d50b/9070723/7bf80d8a7760/s-29-00853-fig4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d50b/9070723/403fea3c7399/s-29-00853-fig5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d50b/9070723/d592b9ef8b7d/s-29-00853-fig6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d50b/9070723/3007dedd0ae2/s-29-00853-fig7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d50b/9070723/d7d014c4f6e8/s-29-00853-fig8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d50b/9070723/6c21fbece06f/s-29-00853-fig1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d50b/9070723/0f0b1a9fa1fc/s-29-00853-fig2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d50b/9070723/d75242c3bbd3/s-29-00853-fig3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d50b/9070723/7bf80d8a7760/s-29-00853-fig4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d50b/9070723/403fea3c7399/s-29-00853-fig5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d50b/9070723/d592b9ef8b7d/s-29-00853-fig6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d50b/9070723/3007dedd0ae2/s-29-00853-fig7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d50b/9070723/d7d014c4f6e8/s-29-00853-fig8.jpg

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