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A finite difference scheme for integrating the Takagi–Taupin equations on an arbitrary orthogonal grid

Calculating dynamical diffraction patterns for X-ray diffraction imaging techniques requires numerical integration of the Takagi–Taupin equations. This is usually performed with a simple, second-order finite difference scheme on a sheared computational grid in which two of the axes are aligned with...

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Autores principales: Carlsen, Mads, Simons, Hugh
Formato: Online Artículo Texto
Lenguaje:English
Publicado: International Union of Crystallography 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9434601/
https://www.ncbi.nlm.nih.gov/pubmed/36047396
http://dx.doi.org/10.1107/S2053273322004934
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author Carlsen, Mads
Simons, Hugh
author_facet Carlsen, Mads
Simons, Hugh
author_sort Carlsen, Mads
collection PubMed
description Calculating dynamical diffraction patterns for X-ray diffraction imaging techniques requires numerical integration of the Takagi–Taupin equations. This is usually performed with a simple, second-order finite difference scheme on a sheared computational grid in which two of the axes are aligned with the wavevectors of the incident and scattered beams. This dictates, especially at low scattering angles, an oblique grid of uneven step sizes. Here a finite difference scheme is presented that carries out this integration in slab-shaped samples on an arbitrary orthogonal grid by implicitly utilizing Fourier interpolation. The scheme achieves the expected second-order convergence and a similar error to the traditional approach for similarly dense grids.
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spelling pubmed-94346012022-09-19 A finite difference scheme for integrating the Takagi–Taupin equations on an arbitrary orthogonal grid Carlsen, Mads Simons, Hugh Acta Crystallogr A Found Adv Research Papers Calculating dynamical diffraction patterns for X-ray diffraction imaging techniques requires numerical integration of the Takagi–Taupin equations. This is usually performed with a simple, second-order finite difference scheme on a sheared computational grid in which two of the axes are aligned with the wavevectors of the incident and scattered beams. This dictates, especially at low scattering angles, an oblique grid of uneven step sizes. Here a finite difference scheme is presented that carries out this integration in slab-shaped samples on an arbitrary orthogonal grid by implicitly utilizing Fourier interpolation. The scheme achieves the expected second-order convergence and a similar error to the traditional approach for similarly dense grids. International Union of Crystallography 2022-07-08 /pmc/articles/PMC9434601/ /pubmed/36047396 http://dx.doi.org/10.1107/S2053273322004934 Text en © Carlsen and Simons 2022 https://creativecommons.org/licenses/by/4.0/This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.
spellingShingle Research Papers
Carlsen, Mads
Simons, Hugh
A finite difference scheme for integrating the Takagi–Taupin equations on an arbitrary orthogonal grid
title A finite difference scheme for integrating the Takagi–Taupin equations on an arbitrary orthogonal grid
title_full A finite difference scheme for integrating the Takagi–Taupin equations on an arbitrary orthogonal grid
title_fullStr A finite difference scheme for integrating the Takagi–Taupin equations on an arbitrary orthogonal grid
title_full_unstemmed A finite difference scheme for integrating the Takagi–Taupin equations on an arbitrary orthogonal grid
title_short A finite difference scheme for integrating the Takagi–Taupin equations on an arbitrary orthogonal grid
title_sort finite difference scheme for integrating the takagi–taupin equations on an arbitrary orthogonal grid
topic Research Papers
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9434601/
https://www.ncbi.nlm.nih.gov/pubmed/36047396
http://dx.doi.org/10.1107/S2053273322004934
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