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Instrumental resolution as a function of scattering angle and wavelength as exemplified for the POWGEN instrument
The method of angular- and wavelength-dispersive (e.g. two-dimensional) Rietveld refinement is a new and emerging tool for the analysis of neutron diffraction data measured at time-of-flight instruments with large area detectors. Following the approach for one-dimensional refinements (using either s...
Autores principales: | , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
International Union of Crystallography
2017
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5458595/ https://www.ncbi.nlm.nih.gov/pubmed/28656041 http://dx.doi.org/10.1107/S1600576717005398 |
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author | Jacobs, Philipp Houben, Andreas Schweika, Werner Tchougréeff, Andrei L. Dronskowski, Richard |
author_facet | Jacobs, Philipp Houben, Andreas Schweika, Werner Tchougréeff, Andrei L. Dronskowski, Richard |
author_sort | Jacobs, Philipp |
collection | PubMed |
description | The method of angular- and wavelength-dispersive (e.g. two-dimensional) Rietveld refinement is a new and emerging tool for the analysis of neutron diffraction data measured at time-of-flight instruments with large area detectors. Following the approach for one-dimensional refinements (using either scattering angle or time of flight), the first step at each beam time cycle is the calibration of the instrument including the determination of instrumental contributions to the peak shape variation to be expected for diffraction patterns measured by the users. The aim of this work is to provide the users with calibration files and – for the later Rietveld refinement of the measured data – with an instrumental resolution file (IRF). This article will elaborate on the necessary steps to generate such an IRF for the angular- and wavelength-dispersive case, exemplified for the POWGEN instrument. A dataset measured on a standard diamond sample is used to extract the profile function in the two-dimensional case. It is found that the variation of reflection width with 2θ and λ can be expressed by the standard equation used for evaluating the instrumental resolution, which yields a substantially more fundamental approach to the parameterization of the instrumental contribution to the peak shape. Geometrical considerations of the POWGEN instrument and sample effects lead to values for Δθ, Δt and ΔL that yield a very good match to the extracted FWHM values. In a final step the refinement results are compared with the one-dimensional, i.e. diffraction-focused, case. |
format | Online Article Text |
id | pubmed-5458595 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2017 |
publisher | International Union of Crystallography |
record_format | MEDLINE/PubMed |
spelling | pubmed-54585952017-06-27 Instrumental resolution as a function of scattering angle and wavelength as exemplified for the POWGEN instrument Jacobs, Philipp Houben, Andreas Schweika, Werner Tchougréeff, Andrei L. Dronskowski, Richard J Appl Crystallogr Research Papers The method of angular- and wavelength-dispersive (e.g. two-dimensional) Rietveld refinement is a new and emerging tool for the analysis of neutron diffraction data measured at time-of-flight instruments with large area detectors. Following the approach for one-dimensional refinements (using either scattering angle or time of flight), the first step at each beam time cycle is the calibration of the instrument including the determination of instrumental contributions to the peak shape variation to be expected for diffraction patterns measured by the users. The aim of this work is to provide the users with calibration files and – for the later Rietveld refinement of the measured data – with an instrumental resolution file (IRF). This article will elaborate on the necessary steps to generate such an IRF for the angular- and wavelength-dispersive case, exemplified for the POWGEN instrument. A dataset measured on a standard diamond sample is used to extract the profile function in the two-dimensional case. It is found that the variation of reflection width with 2θ and λ can be expressed by the standard equation used for evaluating the instrumental resolution, which yields a substantially more fundamental approach to the parameterization of the instrumental contribution to the peak shape. Geometrical considerations of the POWGEN instrument and sample effects lead to values for Δθ, Δt and ΔL that yield a very good match to the extracted FWHM values. In a final step the refinement results are compared with the one-dimensional, i.e. diffraction-focused, case. International Union of Crystallography 2017-05-25 /pmc/articles/PMC5458595/ /pubmed/28656041 http://dx.doi.org/10.1107/S1600576717005398 Text en © Philipp Jacobs et al. 2017 http://creativecommons.org/licenses/by/2.0/uk/ 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.http://creativecommons.org/licenses/by/2.0/uk/ |
spellingShingle | Research Papers Jacobs, Philipp Houben, Andreas Schweika, Werner Tchougréeff, Andrei L. Dronskowski, Richard Instrumental resolution as a function of scattering angle and wavelength as exemplified for the POWGEN instrument |
title | Instrumental resolution as a function of scattering angle and wavelength as exemplified for the POWGEN instrument |
title_full | Instrumental resolution as a function of scattering angle and wavelength as exemplified for the POWGEN instrument |
title_fullStr | Instrumental resolution as a function of scattering angle and wavelength as exemplified for the POWGEN instrument |
title_full_unstemmed | Instrumental resolution as a function of scattering angle and wavelength as exemplified for the POWGEN instrument |
title_short | Instrumental resolution as a function of scattering angle and wavelength as exemplified for the POWGEN instrument |
title_sort | instrumental resolution as a function of scattering angle and wavelength as exemplified for the powgen instrument |
topic | Research Papers |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5458595/ https://www.ncbi.nlm.nih.gov/pubmed/28656041 http://dx.doi.org/10.1107/S1600576717005398 |
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