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用于高能量分辨率非弹性X射线散射分析仪的高质量石英单晶。

High-quality quartz single crystals for high-energy-resolution inelastic X-ray scattering analyzers.

作者信息

Hönnicke Marcelo Goncalves, Huang Xianrong, Cusatis Cesar, Koditwuakku Chaminda Nalaka, Cai Yong Q

机构信息

Universidade Federal da Integração Latino-Americana , Caixa Postal 2044, Foz do Iguacu, Parana 85867-970, Brazil.

出版信息

J Appl Crystallogr. 2013 Aug 1;46(Pt 4):939-944. doi: 10.1107/S0021889813004731. Epub 2013 Jun 7.

DOI:10.1107/S0021889813004731
PMID:24046502
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC3769068/
Abstract

Spherical analyzers are well known instruments for inelastic X-ray scattering (IXS) experiments. High-resolution IXS experiments almost always use Si single crystals as monochromators and spherical analyzers. At higher energies (>20 keV) Si shows a high energy resolution (<10 meV), at an exact symmetric back-diffraction condition, since the energy resolution is given by the real part of the susceptibility or polarizability. However, at low energies (<10 keV), high energy resolution is difficult to achieve with Si. α-SiO (quartz) can be an option, since it offers high energy resolution at low energies. In this work, the characterization of high-quality α-SiO is presented. Such characterization is made by high-resolution rocking curve, topography and lattice parameter mapping in different samples from a single block. X-ray optics with α-SiO for IXS at lower energies (from 2.5 to 12.6 keV) with medium to high energy resolution (from 90 to 11 meV) are proposed and theoretically exploited.

摘要

球形分析仪是用于非弹性X射线散射(IXS)实验的知名仪器。高分辨率IXS实验几乎总是使用硅单晶作为单色仪和球形分析仪。在较高能量(>20 keV)下,在精确的对称背散射条件下,硅显示出高能量分辨率(<10 meV),因为能量分辨率由磁化率或极化率的实部给出。然而,在低能量(<10 keV)下,用硅很难实现高能量分辨率。α-二氧化硅(石英)可以是一种选择,因为它在低能量下提供高能量分辨率。在这项工作中,展示了高质量α-二氧化硅的表征。这种表征是通过对来自单个块体的不同样品进行高分辨率摇摆曲线、形貌和晶格参数映射来完成的。提出并从理论上研究了用于较低能量(2.5至12.6 keV)、具有中等到高能量分辨率(90至11 meV)的IXS的带有α-二氧化硅的X射线光学器件。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0bf5/3769068/826f6bc21053/j-46-00939-fig8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0bf5/3769068/0ed74ef4d2db/j-46-00939-fig1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0bf5/3769068/65e5c43c5698/j-46-00939-fig2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0bf5/3769068/bd595861cf1e/j-46-00939-fig3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0bf5/3769068/d6c497f2de04/j-46-00939-fig4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0bf5/3769068/807c29bb975a/j-46-00939-fig5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0bf5/3769068/bf147adb50fe/j-46-00939-fig6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0bf5/3769068/c6a881db1345/j-46-00939-fig7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0bf5/3769068/826f6bc21053/j-46-00939-fig8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0bf5/3769068/0ed74ef4d2db/j-46-00939-fig1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0bf5/3769068/65e5c43c5698/j-46-00939-fig2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0bf5/3769068/bd595861cf1e/j-46-00939-fig3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0bf5/3769068/d6c497f2de04/j-46-00939-fig4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0bf5/3769068/807c29bb975a/j-46-00939-fig5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0bf5/3769068/bf147adb50fe/j-46-00939-fig6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0bf5/3769068/c6a881db1345/j-46-00939-fig7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/0bf5/3769068/826f6bc21053/j-46-00939-fig8.jpg

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