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The XFP (17-BM) beamline for X-ray footprinting at NSLS-II
Hydroxyl-radical mediated synchrotron X-ray footprinting (XF) is a powerful solution-state technique in structural biology for the study of macromolecular structure and dynamics of proteins and nucleic acids, with several synchrotron resources available to serve the XF community worldwide. The XFP (...
Autores principales: | , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
International Union of Crystallography
2019
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6613119/ https://www.ncbi.nlm.nih.gov/pubmed/31274468 http://dx.doi.org/10.1107/S1600577519003576 |
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author | Asuru, Awuri Farquhar, Erik R. Sullivan, Michael Abel, Donald Toomey, John Chance, Mark R. Bohon, Jen |
author_facet | Asuru, Awuri Farquhar, Erik R. Sullivan, Michael Abel, Donald Toomey, John Chance, Mark R. Bohon, Jen |
author_sort | Asuru, Awuri |
collection | PubMed |
description | Hydroxyl-radical mediated synchrotron X-ray footprinting (XF) is a powerful solution-state technique in structural biology for the study of macromolecular structure and dynamics of proteins and nucleic acids, with several synchrotron resources available to serve the XF community worldwide. The XFP (Biological X-ray Footprinting) beamline at the NSLS-II was constructed on a three-pole wiggler source at 17-BM to serve as the premier beamline for performing this technique, providing an unparalleled combination of high flux density broadband beam, flexibility in beam morphology, and sample handling capabilities specifically designed for XF experiments. The details of beamline design, beam measurements, and science commissioning results for a standard protein using the two distinct XFP endstations are presented here. XFP took first light in 2016 and is now available for general user operations through peer-reviewed proposals. Currently, beam sizes from 450 µm × 120 µm to 2.7 mm × 2.7 mm (FWHM) are available, with a flux of 1.6 × 10(16) photons s(−1) (measured at 325 mA ring current) in a broadband (∼5–16 keV) beam. This flux is expected to rise to 2.5 × 10(16) photons s(−1) at the full NSLS-II design current of 500 mA, providing an incident power density of >500 W mm(−2) at full focus. |
format | Online Article Text |
id | pubmed-6613119 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2019 |
publisher | International Union of Crystallography |
record_format | MEDLINE/PubMed |
spelling | pubmed-66131192019-07-17 The XFP (17-BM) beamline for X-ray footprinting at NSLS-II Asuru, Awuri Farquhar, Erik R. Sullivan, Michael Abel, Donald Toomey, John Chance, Mark R. Bohon, Jen J Synchrotron Radiat Beamlines Hydroxyl-radical mediated synchrotron X-ray footprinting (XF) is a powerful solution-state technique in structural biology for the study of macromolecular structure and dynamics of proteins and nucleic acids, with several synchrotron resources available to serve the XF community worldwide. The XFP (Biological X-ray Footprinting) beamline at the NSLS-II was constructed on a three-pole wiggler source at 17-BM to serve as the premier beamline for performing this technique, providing an unparalleled combination of high flux density broadband beam, flexibility in beam morphology, and sample handling capabilities specifically designed for XF experiments. The details of beamline design, beam measurements, and science commissioning results for a standard protein using the two distinct XFP endstations are presented here. XFP took first light in 2016 and is now available for general user operations through peer-reviewed proposals. Currently, beam sizes from 450 µm × 120 µm to 2.7 mm × 2.7 mm (FWHM) are available, with a flux of 1.6 × 10(16) photons s(−1) (measured at 325 mA ring current) in a broadband (∼5–16 keV) beam. This flux is expected to rise to 2.5 × 10(16) photons s(−1) at the full NSLS-II design current of 500 mA, providing an incident power density of >500 W mm(−2) at full focus. International Union of Crystallography 2019-06-04 /pmc/articles/PMC6613119/ /pubmed/31274468 http://dx.doi.org/10.1107/S1600577519003576 Text en © Awuri Asuru et al. 2019 http://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.http://creativecommons.org/licenses/by/4.0/ |
spellingShingle | Beamlines Asuru, Awuri Farquhar, Erik R. Sullivan, Michael Abel, Donald Toomey, John Chance, Mark R. Bohon, Jen The XFP (17-BM) beamline for X-ray footprinting at NSLS-II |
title | The XFP (17-BM) beamline for X-ray footprinting at NSLS-II |
title_full | The XFP (17-BM) beamline for X-ray footprinting at NSLS-II |
title_fullStr | The XFP (17-BM) beamline for X-ray footprinting at NSLS-II |
title_full_unstemmed | The XFP (17-BM) beamline for X-ray footprinting at NSLS-II |
title_short | The XFP (17-BM) beamline for X-ray footprinting at NSLS-II |
title_sort | xfp (17-bm) beamline for x-ray footprinting at nsls-ii |
topic | Beamlines |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6613119/ https://www.ncbi.nlm.nih.gov/pubmed/31274468 http://dx.doi.org/10.1107/S1600577519003576 |
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