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Cryogenics free production of hyperpolarized (129)Xe and (83)Kr for biomedical MRI applications()

As an alternative to cryogenic gas handling, hyperpolarized (hp) gas mixtures were extracted directly from the spin exchange optical pumping (SEOP) process through expansion followed by compression to ambient pressure for biomedical MRI applications. The omission of cryogenic gas separation generall...

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Autores principales: Hughes-Riley, Theodore, Six, Joseph S., Lilburn, David M.L., Stupic, Karl F., Dorkes, Alan C., Shaw, Dominick E., Pavlovskaya, Galina E., Meersmann, Thomas
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Elsevier 2013
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3863958/
https://www.ncbi.nlm.nih.gov/pubmed/24135800
http://dx.doi.org/10.1016/j.jmr.2013.09.008
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author Hughes-Riley, Theodore
Six, Joseph S.
Lilburn, David M.L.
Stupic, Karl F.
Dorkes, Alan C.
Shaw, Dominick E.
Pavlovskaya, Galina E.
Meersmann, Thomas
author_facet Hughes-Riley, Theodore
Six, Joseph S.
Lilburn, David M.L.
Stupic, Karl F.
Dorkes, Alan C.
Shaw, Dominick E.
Pavlovskaya, Galina E.
Meersmann, Thomas
author_sort Hughes-Riley, Theodore
collection PubMed
description As an alternative to cryogenic gas handling, hyperpolarized (hp) gas mixtures were extracted directly from the spin exchange optical pumping (SEOP) process through expansion followed by compression to ambient pressure for biomedical MRI applications. The omission of cryogenic gas separation generally requires the usage of high xenon or krypton concentrations at low SEOP gas pressures to generate hp (129)Xe or hp (83)Kr with sufficient MR signal intensity for imaging applications. Two different extraction schemes for the hp gasses were explored with focus on the preservation of the nuclear spin polarization. It was found that an extraction scheme based on an inflatable, pressure controlled balloon is sufficient for hp (129)Xe handling, while (83)Kr can efficiently be extracted through a single cycle piston pump. The extraction methods were tested for ex vivo MRI applications with excised rat lungs. Precise mixing of the hp gases with oxygen, which may be of interest for potential in vivo applications, was accomplished during the extraction process using a piston pump. The (83)Kr bulk gas phase T(1) relaxation in the mixtures containing more than approximately 1% O(2) was found to be slower than that of (129)Xe in corresponding mixtures. The experimental setup also facilitated (129)Xe T(1) relaxation measurements as a function of O(2) concentration within excised lungs.
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spelling pubmed-38639582013-12-17 Cryogenics free production of hyperpolarized (129)Xe and (83)Kr for biomedical MRI applications() Hughes-Riley, Theodore Six, Joseph S. Lilburn, David M.L. Stupic, Karl F. Dorkes, Alan C. Shaw, Dominick E. Pavlovskaya, Galina E. Meersmann, Thomas J Magn Reson Article As an alternative to cryogenic gas handling, hyperpolarized (hp) gas mixtures were extracted directly from the spin exchange optical pumping (SEOP) process through expansion followed by compression to ambient pressure for biomedical MRI applications. The omission of cryogenic gas separation generally requires the usage of high xenon or krypton concentrations at low SEOP gas pressures to generate hp (129)Xe or hp (83)Kr with sufficient MR signal intensity for imaging applications. Two different extraction schemes for the hp gasses were explored with focus on the preservation of the nuclear spin polarization. It was found that an extraction scheme based on an inflatable, pressure controlled balloon is sufficient for hp (129)Xe handling, while (83)Kr can efficiently be extracted through a single cycle piston pump. The extraction methods were tested for ex vivo MRI applications with excised rat lungs. Precise mixing of the hp gases with oxygen, which may be of interest for potential in vivo applications, was accomplished during the extraction process using a piston pump. The (83)Kr bulk gas phase T(1) relaxation in the mixtures containing more than approximately 1% O(2) was found to be slower than that of (129)Xe in corresponding mixtures. The experimental setup also facilitated (129)Xe T(1) relaxation measurements as a function of O(2) concentration within excised lungs. Elsevier 2013-12 /pmc/articles/PMC3863958/ /pubmed/24135800 http://dx.doi.org/10.1016/j.jmr.2013.09.008 Text en © 2013 The Authors https://creativecommons.org/licenses/by/3.0/ Open Access under CC BY 3.0 (https://creativecommons.org/licenses/by/3.0/) license
spellingShingle Article
Hughes-Riley, Theodore
Six, Joseph S.
Lilburn, David M.L.
Stupic, Karl F.
Dorkes, Alan C.
Shaw, Dominick E.
Pavlovskaya, Galina E.
Meersmann, Thomas
Cryogenics free production of hyperpolarized (129)Xe and (83)Kr for biomedical MRI applications()
title Cryogenics free production of hyperpolarized (129)Xe and (83)Kr for biomedical MRI applications()
title_full Cryogenics free production of hyperpolarized (129)Xe and (83)Kr for biomedical MRI applications()
title_fullStr Cryogenics free production of hyperpolarized (129)Xe and (83)Kr for biomedical MRI applications()
title_full_unstemmed Cryogenics free production of hyperpolarized (129)Xe and (83)Kr for biomedical MRI applications()
title_short Cryogenics free production of hyperpolarized (129)Xe and (83)Kr for biomedical MRI applications()
title_sort cryogenics free production of hyperpolarized (129)xe and (83)kr for biomedical mri applications()
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3863958/
https://www.ncbi.nlm.nih.gov/pubmed/24135800
http://dx.doi.org/10.1016/j.jmr.2013.09.008
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