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A measurement of the attenuation of radiation from F‐18 by a PET/MR scanner

The attenuation of 511 keV photons by the structure of a PET/MR scanner was measured prior to energizing the magnet. The exposure rate from a source of fluorine‐18 was measured in air and, with the source placed at the isocenter of the instrument, at various points outside of the scanner. In an arc...

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Autores principales: Wendt, Richard E., Ai, Hua A., Meier, Joseph G., Lopez, Benjamin P., Fahrenholtz, Samuel J., Mawlawi, Osama R.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: John Wiley and Sons Inc. 2018
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6236846/
https://www.ncbi.nlm.nih.gov/pubmed/30338918
http://dx.doi.org/10.1002/acm2.12479
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author Wendt, Richard E.
Ai, Hua A.
Meier, Joseph G.
Lopez, Benjamin P.
Fahrenholtz, Samuel J.
Mawlawi, Osama R.
author_facet Wendt, Richard E.
Ai, Hua A.
Meier, Joseph G.
Lopez, Benjamin P.
Fahrenholtz, Samuel J.
Mawlawi, Osama R.
author_sort Wendt, Richard E.
collection PubMed
description The attenuation of 511 keV photons by the structure of a PET/MR scanner was measured prior to energizing the magnet. The exposure rate from a source of fluorine‐18 was measured in air and, with the source placed at the isocenter of the instrument, at various points outside of the scanner. In an arc from 45 to 135 degrees relative to the long axis of the scanner and at a distance of 1.5 m from the isocenter, the attenuation by the scanner is at least 5.6 half‐value layers from the MR component alone and at least 6.6 half‐value layers with the PET insert installed. This information could inform better design of the radiation shielding for PET/MR scanners.
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spelling pubmed-62368462018-11-20 A measurement of the attenuation of radiation from F‐18 by a PET/MR scanner Wendt, Richard E. Ai, Hua A. Meier, Joseph G. Lopez, Benjamin P. Fahrenholtz, Samuel J. Mawlawi, Osama R. J Appl Clin Med Phys Technical Notes The attenuation of 511 keV photons by the structure of a PET/MR scanner was measured prior to energizing the magnet. The exposure rate from a source of fluorine‐18 was measured in air and, with the source placed at the isocenter of the instrument, at various points outside of the scanner. In an arc from 45 to 135 degrees relative to the long axis of the scanner and at a distance of 1.5 m from the isocenter, the attenuation by the scanner is at least 5.6 half‐value layers from the MR component alone and at least 6.6 half‐value layers with the PET insert installed. This information could inform better design of the radiation shielding for PET/MR scanners. John Wiley and Sons Inc. 2018-10-19 /pmc/articles/PMC6236846/ /pubmed/30338918 http://dx.doi.org/10.1002/acm2.12479 Text en © 2018 The Authors. Journal of Applied Clinical Medical Physics published by Wiley Periodicals, Inc. on behalf of American Association of Physicists in Medicine. This is an open access article under the terms of the http://creativecommons.org/licenses/by/4.0/ License, which permits use, distribution and reproduction in any medium, provided the original work is properly cited.
spellingShingle Technical Notes
Wendt, Richard E.
Ai, Hua A.
Meier, Joseph G.
Lopez, Benjamin P.
Fahrenholtz, Samuel J.
Mawlawi, Osama R.
A measurement of the attenuation of radiation from F‐18 by a PET/MR scanner
title A measurement of the attenuation of radiation from F‐18 by a PET/MR scanner
title_full A measurement of the attenuation of radiation from F‐18 by a PET/MR scanner
title_fullStr A measurement of the attenuation of radiation from F‐18 by a PET/MR scanner
title_full_unstemmed A measurement of the attenuation of radiation from F‐18 by a PET/MR scanner
title_short A measurement of the attenuation of radiation from F‐18 by a PET/MR scanner
title_sort measurement of the attenuation of radiation from f‐18 by a pet/mr scanner
topic Technical Notes
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6236846/
https://www.ncbi.nlm.nih.gov/pubmed/30338918
http://dx.doi.org/10.1002/acm2.12479
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