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使用高温同步辐射衍射法测定在密封石英毛细管中加热的纯、掺杂和共掺杂锐钛矿纳米颗粒的热膨胀系数。

Thermal expansion coefficient determination of pure, doped, and co-doped anatase nanoparticles heated in sealed quartz capillaries using high-temperature synchrotron radiation diffraction.

作者信息

Albetran Hani Manssor

机构信息

Department of Basic Sciences, College of Education, Imam Abdulrahman Bin Faisal University, Dammam 31451, Saudi Arabia.

出版信息

Heliyon. 2020 Jul 30;6(7):e04501. doi: 10.1016/j.heliyon.2020.e04501. eCollection 2020 Jul.

DOI:10.1016/j.heliyon.2020.e04501
PMID:32775715
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC7394871/
Abstract

Synchrotron radiation diffraction was conducted and at high temperature to establish the lattice parameters of pure/undoped, doped, and co-doped anatase nanoparticles. The nanoparticles were heated from room temperature to 950 °C in sealed quartz capillaries. The effect of pressure, doping (aluminium or indium), and co-doping (indium-chromium or silver-chromium) on the thermal expansion coefficients of nanocrystalline anatase was established. Synchrotron radiation diffraction high temperature , transmission electron microscopy, and the Rietveld refinement method were used to characterise the anatase nanoparticles. The anisotropy of the thermal expansion, α/α, for pressurised anatase nanoparticles was smaller than that for anatase heated in unpressurised air or argon, and it was much smaller in a vacuum.

摘要

在高温下进行同步辐射衍射,以确定纯/未掺杂、掺杂和共掺杂锐钛矿纳米颗粒的晶格参数。纳米颗粒在密封石英毛细管中从室温加热到950℃。确定了压力、掺杂(铝或铟)和共掺杂(铟 - 铬或银 - 铬)对纳米晶锐钛矿热膨胀系数的影响。利用同步辐射衍射高温、透射电子显微镜和Rietveld精修方法对锐钛矿纳米颗粒进行表征。加压锐钛矿纳米颗粒的热膨胀各向异性α/α比在非加压空气或氩气中加热的锐钛矿小,而在真空中则小得多。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2384/7394871/aa22ac7fe6d1/gr10.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2384/7394871/6a8c69a1cede/gr1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2384/7394871/d3f088517866/gr2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2384/7394871/4d36d1efa738/gr3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2384/7394871/56811c5b3707/gr4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2384/7394871/454d82382393/gr5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2384/7394871/99ad6ad8c2d2/gr6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2384/7394871/a2ab81b9e244/gr7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2384/7394871/8ca364f2b2ed/gr8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2384/7394871/59181cb03cc8/gr9.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2384/7394871/aa22ac7fe6d1/gr10.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2384/7394871/6a8c69a1cede/gr1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2384/7394871/d3f088517866/gr2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2384/7394871/4d36d1efa738/gr3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2384/7394871/56811c5b3707/gr4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2384/7394871/454d82382393/gr5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2384/7394871/99ad6ad8c2d2/gr6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2384/7394871/a2ab81b9e244/gr7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2384/7394871/8ca364f2b2ed/gr8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2384/7394871/59181cb03cc8/gr9.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2384/7394871/aa22ac7fe6d1/gr10.jpg

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