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Hyperpolarized (131)Xe NMR spectroscopy

Hyperpolarized (hp) (131)Xe with up to 2.2% spin polarization (i.e., 5000-fold signal enhancement at 9.4 T) was obtained after separation from the rubidium vapor of the spin-exchange optical pumping (SEOP) process. The SEOP was applied for several minutes in a stopped-flow mode, and the fast, quadru...

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Autores principales: Stupic, Karl F., Cleveland, Zackary I., Pavlovskaya, Galina E., Meersmann, Thomas
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Elsevier 2011
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3160776/
https://www.ncbi.nlm.nih.gov/pubmed/21051249
http://dx.doi.org/10.1016/j.jmr.2010.10.004
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author Stupic, Karl F.
Cleveland, Zackary I.
Pavlovskaya, Galina E.
Meersmann, Thomas
author_facet Stupic, Karl F.
Cleveland, Zackary I.
Pavlovskaya, Galina E.
Meersmann, Thomas
author_sort Stupic, Karl F.
collection PubMed
description Hyperpolarized (hp) (131)Xe with up to 2.2% spin polarization (i.e., 5000-fold signal enhancement at 9.4 T) was obtained after separation from the rubidium vapor of the spin-exchange optical pumping (SEOP) process. The SEOP was applied for several minutes in a stopped-flow mode, and the fast, quadrupolar-driven T(1) relaxation of this spin I = 3/2 noble gas isotope required a rapid subsequent rubidium removal and swift transfer into the high magnetic field region for NMR detection. Because of the xenon density dependent (131)Xe quadrupolar relaxation in the gas phase, the SEOP polarization build-up exhibits an even more pronounced dependence on xenon partial pressure than that observed in (129)Xe SEOP. (131)Xe is the only stable noble gas isotope with a positive gyromagnetic ratio and shows therefore a different relative phase between hp signal and thermal signal compared to all other noble gases. The gas phase (131)Xe NMR spectrum displays a surface and magnetic field dependent quadrupolar splitting that was found to have additional gas pressure and gas composition dependence. The splitting was reduced by the presence of water vapor that presumably influences xenon-surface interactions. The hp (131)Xe spectrum shows differential line broadening, suggesting the presence of strong adsorption sites. Beyond hp (131)Xe NMR spectroscopy studies, a general equation for the high temperature, thermal spin polarization, P, for spin [Formula: see text] nuclei is presented.
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spelling pubmed-31607762011-08-30 Hyperpolarized (131)Xe NMR spectroscopy Stupic, Karl F. Cleveland, Zackary I. Pavlovskaya, Galina E. Meersmann, Thomas J Magn Reson Article Hyperpolarized (hp) (131)Xe with up to 2.2% spin polarization (i.e., 5000-fold signal enhancement at 9.4 T) was obtained after separation from the rubidium vapor of the spin-exchange optical pumping (SEOP) process. The SEOP was applied for several minutes in a stopped-flow mode, and the fast, quadrupolar-driven T(1) relaxation of this spin I = 3/2 noble gas isotope required a rapid subsequent rubidium removal and swift transfer into the high magnetic field region for NMR detection. Because of the xenon density dependent (131)Xe quadrupolar relaxation in the gas phase, the SEOP polarization build-up exhibits an even more pronounced dependence on xenon partial pressure than that observed in (129)Xe SEOP. (131)Xe is the only stable noble gas isotope with a positive gyromagnetic ratio and shows therefore a different relative phase between hp signal and thermal signal compared to all other noble gases. The gas phase (131)Xe NMR spectrum displays a surface and magnetic field dependent quadrupolar splitting that was found to have additional gas pressure and gas composition dependence. The splitting was reduced by the presence of water vapor that presumably influences xenon-surface interactions. The hp (131)Xe spectrum shows differential line broadening, suggesting the presence of strong adsorption sites. Beyond hp (131)Xe NMR spectroscopy studies, a general equation for the high temperature, thermal spin polarization, P, for spin [Formula: see text] nuclei is presented. Elsevier 2011-01 /pmc/articles/PMC3160776/ /pubmed/21051249 http://dx.doi.org/10.1016/j.jmr.2010.10.004 Text en © 2011 Elsevier Inc. https://creativecommons.org/licenses/by/3.0/ Open Access under CC BY 3.0 (https://creativecommons.org/licenses/by/3.0/) license
spellingShingle Article
Stupic, Karl F.
Cleveland, Zackary I.
Pavlovskaya, Galina E.
Meersmann, Thomas
Hyperpolarized (131)Xe NMR spectroscopy
title Hyperpolarized (131)Xe NMR spectroscopy
title_full Hyperpolarized (131)Xe NMR spectroscopy
title_fullStr Hyperpolarized (131)Xe NMR spectroscopy
title_full_unstemmed Hyperpolarized (131)Xe NMR spectroscopy
title_short Hyperpolarized (131)Xe NMR spectroscopy
title_sort hyperpolarized (131)xe nmr spectroscopy
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3160776/
https://www.ncbi.nlm.nih.gov/pubmed/21051249
http://dx.doi.org/10.1016/j.jmr.2010.10.004
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