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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...

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Autores principales: Jacobs, Philipp, Houben, Andreas, Schweika, Werner, Tchougréeff, Andrei L., Dronskowski, Richard
Formato: Online Artículo Texto
Lenguaje:English
Publicado: International Union of Crystallography 2017
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.
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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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