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2021 ◽  
Vol 0 (0) ◽  
Author(s):  
Bohdana Belan ◽  
Marek Daszkiewicz ◽  
Mariya Dzevenko ◽  
Beata Rożdżyńska-Kiełbik ◽  
Volodymyr Pavlyuk ◽  
...  

Abstract The crystal structures of Eu5Si3 and EuSi were studied in detail by X-ray single-crystal diffraction. The single crystals were selected from arc-melted and annealed samples. X-ray diffraction was performed at room temperature on an Oxford Diffraction X’calibur Atlas four-circle diffractometer (MoKα radiation). Eu5Si3 adopts the tetragonal Cr5B3-type: space group I4/mcm (# 140), Pearson code tI32, Z = 4, a = 7.9339(6), c = 15.308(2) Å. The compounds with equiatomic composition EuSi crystallize in the structure type TlI: space group Cmcm (# 63), Pearson code oS8, Z = 4, a = 4.6955(6), b = 11.1528(13), c = 3.9845(4) Å. The silicides Eu5Si3 and Li2Si form during electrochemical lithiation (charge process) of EuSi. The electrochemical process 5EuSi + 4Li+ + 4e − ↔ Eu5Si3 + 2Li2Si is reversible, and the discharge specific capacity at 1C rate reached 140 mAhg−1 and the Coulombic efficiency is 93%.


2019 ◽  
Vol 75 (a1) ◽  
pp. a163-a163
Author(s):  
Pierre Le Magueres ◽  
Marl DelCampo ◽  
Keisuke Saito ◽  
Joseph D. Ferrara ◽  
Jakub Wojciechowski ◽  
...  

2018 ◽  
Vol 74 (a1) ◽  
pp. a468-a468
Author(s):  
Pierre Le Magueres ◽  
Eric W. Reinheimer ◽  
Mathias Meyer ◽  
Adrian Jones ◽  
Damian Kucharczyk
Keyword(s):  

2010 ◽  
Vol 43 (6) ◽  
pp. 1440-1451 ◽  
Author(s):  
Alexander Dudka

New methods have been developed for scaling the intensities of diffraction reflections measured on a diffractometer with a CCD detector. The algorithm involves cyclic alternation of the refinement of a structure model from experimental data corrected for anisotropic effects with the refinement of anisotropic parameters from initial data for a fixed structure model. The first method consists of refining scale factors for the intensities after they have first been corrected for anisotropic effects of known physical nature (thermal diffuse scattering, absorption, extinctionetc.). It has been shown that the majority of the observed biases of intensities are caused by the characteristics of the CCD detector and the technique used for data collection on the diffractometer, rather than by the properties of the sample. The second (alternative) method of fixed scaling has been implemented here. This method does not require refinement of empirical scale factors but uses intensity correction maps obtained by averaging the results derived from several experiments with different crystals. The first map describes the non-uniformity of the response over the surface area of the detector. The second map accounts for distortions dependent on the setting angles of the goniometer. The methods were checked for data measured on an Oxford Diffraction Xcalibur Sapphire 3 CCD diffractometer. The proposed methods significantly improve the results of the refinement and make it possible to obtain a structure model that is reproduced in repeated investigations of samples of the same compound.


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