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Continuous diffraction of molecules and disordered molecular crystals

The intensities of far-field diffraction patterns of orientationally aligned molecules obey Wilson statistics, whether those molecules are in isolation (giving rise to a continuous diffraction pattern) or arranged in a crystal (giving rise to Bragg peaks). Ensembles of molecules in several orientati...

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Autores principales: Chapman, Henry N., Yefanov, Oleksandr M., Ayyer, Kartik, White, Thomas A., Barty, Anton, Morgan, Andrew, Mariani, Valerio, Oberthuer, Dominik, Pande, Kanupriya
Formato: Online Artículo Texto
Lenguaje:English
Publicado: International Union of Crystallography 2017
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5541353/
https://www.ncbi.nlm.nih.gov/pubmed/28808434
http://dx.doi.org/10.1107/S160057671700749X
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author Chapman, Henry N.
Yefanov, Oleksandr M.
Ayyer, Kartik
White, Thomas A.
Barty, Anton
Morgan, Andrew
Mariani, Valerio
Oberthuer, Dominik
Pande, Kanupriya
author_facet Chapman, Henry N.
Yefanov, Oleksandr M.
Ayyer, Kartik
White, Thomas A.
Barty, Anton
Morgan, Andrew
Mariani, Valerio
Oberthuer, Dominik
Pande, Kanupriya
author_sort Chapman, Henry N.
collection PubMed
description The intensities of far-field diffraction patterns of orientationally aligned molecules obey Wilson statistics, whether those molecules are in isolation (giving rise to a continuous diffraction pattern) or arranged in a crystal (giving rise to Bragg peaks). Ensembles of molecules in several orientations, but uncorrelated in position, give rise to the incoherent sum of the diffraction from those objects, modifying the statistics in a similar way as crystal twinning modifies the distribution of Bragg intensities. This situation arises in the continuous diffraction of laser-aligned molecules or translationally disordered molecular crystals. This paper develops the analysis of the intensity statistics of such continuous diffraction to obtain parameters such as scaling, beam coherence and the number of contributing independent object orientations. When measured, continuous molecular diffraction is generally weak and accompanied by a background that far exceeds the strength of the signal. Instead of just relying upon the smallest measured intensities or their mean value to guide the subtraction of the background, it is shown how all measured values can be utilized to estimate the background, noise and signal, by employing a modified ‘noisy Wilson’ distribution that explicitly includes the background. Parameters relating to the background and signal quantities can be estimated from the moments of the measured intensities. The analysis method is demonstrated on previously published continuous diffraction data measured from crystals of photosystem II [Ayyer et al. (2016 ▸), Nature, 530, 202–206].
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spelling pubmed-55413532017-08-14 Continuous diffraction of molecules and disordered molecular crystals Chapman, Henry N. Yefanov, Oleksandr M. Ayyer, Kartik White, Thomas A. Barty, Anton Morgan, Andrew Mariani, Valerio Oberthuer, Dominik Pande, Kanupriya J Appl Crystallogr Research Papers The intensities of far-field diffraction patterns of orientationally aligned molecules obey Wilson statistics, whether those molecules are in isolation (giving rise to a continuous diffraction pattern) or arranged in a crystal (giving rise to Bragg peaks). Ensembles of molecules in several orientations, but uncorrelated in position, give rise to the incoherent sum of the diffraction from those objects, modifying the statistics in a similar way as crystal twinning modifies the distribution of Bragg intensities. This situation arises in the continuous diffraction of laser-aligned molecules or translationally disordered molecular crystals. This paper develops the analysis of the intensity statistics of such continuous diffraction to obtain parameters such as scaling, beam coherence and the number of contributing independent object orientations. When measured, continuous molecular diffraction is generally weak and accompanied by a background that far exceeds the strength of the signal. Instead of just relying upon the smallest measured intensities or their mean value to guide the subtraction of the background, it is shown how all measured values can be utilized to estimate the background, noise and signal, by employing a modified ‘noisy Wilson’ distribution that explicitly includes the background. Parameters relating to the background and signal quantities can be estimated from the moments of the measured intensities. The analysis method is demonstrated on previously published continuous diffraction data measured from crystals of photosystem II [Ayyer et al. (2016 ▸), Nature, 530, 202–206]. International Union of Crystallography 2017-07-07 /pmc/articles/PMC5541353/ /pubmed/28808434 http://dx.doi.org/10.1107/S160057671700749X Text en © Henry N. Chapman 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
Chapman, Henry N.
Yefanov, Oleksandr M.
Ayyer, Kartik
White, Thomas A.
Barty, Anton
Morgan, Andrew
Mariani, Valerio
Oberthuer, Dominik
Pande, Kanupriya
Continuous diffraction of molecules and disordered molecular crystals
title Continuous diffraction of molecules and disordered molecular crystals
title_full Continuous diffraction of molecules and disordered molecular crystals
title_fullStr Continuous diffraction of molecules and disordered molecular crystals
title_full_unstemmed Continuous diffraction of molecules and disordered molecular crystals
title_short Continuous diffraction of molecules and disordered molecular crystals
title_sort continuous diffraction of molecules and disordered molecular crystals
topic Research Papers
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5541353/
https://www.ncbi.nlm.nih.gov/pubmed/28808434
http://dx.doi.org/10.1107/S160057671700749X
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