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Comparison of Overhauser DNP at 0.34 and 3.4 T with Frémy’s Salt

Dynamic nuclear polarization (DNP) is investigated in the liquid state using a model system of Frémy’s salt dissolved in water. Nuclear magnetic resonance signal enhancements at 0.34 and 3.4 T of the bulk water protons are recorded as a function of the irradiation time and the polarizer concentratio...

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Detalles Bibliográficos
Autores principales: Türke, M.-T., Bennati, M.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Springer Vienna 2012
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3396338/
https://www.ncbi.nlm.nih.gov/pubmed/22815593
http://dx.doi.org/10.1007/s00723-012-0362-5
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author Türke, M.-T.
Bennati, M.
author_facet Türke, M.-T.
Bennati, M.
author_sort Türke, M.-T.
collection PubMed
description Dynamic nuclear polarization (DNP) is investigated in the liquid state using a model system of Frémy’s salt dissolved in water. Nuclear magnetic resonance signal enhancements at 0.34 and 3.4 T of the bulk water protons are recorded as a function of the irradiation time and the polarizer concentration. The build-up rates are consistent with the T (1n) of the observed water protons at room temperature (for 9 GHz/0.34 T) and for about 50 ± 10 °C at 94 GHz/3.4 T. At 94 GHz/3.4 T, we observe in our setup a maximal enhancement of −50 at 25 mM polarizer concentration. The use of Frémy’s salt allows the determination of the saturation factors at 94 GHz by pulsed ELDOR experiments. The results are well consistent with the Overhauser DNP mechanism and indicate that higher enhancements at this intermediate frequency require higher sample temperatures.
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spelling pubmed-33963382012-07-17 Comparison of Overhauser DNP at 0.34 and 3.4 T with Frémy’s Salt Türke, M.-T. Bennati, M. Appl Magn Reson Article Dynamic nuclear polarization (DNP) is investigated in the liquid state using a model system of Frémy’s salt dissolved in water. Nuclear magnetic resonance signal enhancements at 0.34 and 3.4 T of the bulk water protons are recorded as a function of the irradiation time and the polarizer concentration. The build-up rates are consistent with the T (1n) of the observed water protons at room temperature (for 9 GHz/0.34 T) and for about 50 ± 10 °C at 94 GHz/3.4 T. At 94 GHz/3.4 T, we observe in our setup a maximal enhancement of −50 at 25 mM polarizer concentration. The use of Frémy’s salt allows the determination of the saturation factors at 94 GHz by pulsed ELDOR experiments. The results are well consistent with the Overhauser DNP mechanism and indicate that higher enhancements at this intermediate frequency require higher sample temperatures. Springer Vienna 2012-06-03 2012 /pmc/articles/PMC3396338/ /pubmed/22815593 http://dx.doi.org/10.1007/s00723-012-0362-5 Text en © The Author(s) 2012 https://creativecommons.org/licenses/by/4.0/ This article is distributed under the terms of the Creative Commons Attribution License which permits any use, distribution, and reproduction in any medium, provided the original author(s) and the source are credited.
spellingShingle Article
Türke, M.-T.
Bennati, M.
Comparison of Overhauser DNP at 0.34 and 3.4 T with Frémy’s Salt
title Comparison of Overhauser DNP at 0.34 and 3.4 T with Frémy’s Salt
title_full Comparison of Overhauser DNP at 0.34 and 3.4 T with Frémy’s Salt
title_fullStr Comparison of Overhauser DNP at 0.34 and 3.4 T with Frémy’s Salt
title_full_unstemmed Comparison of Overhauser DNP at 0.34 and 3.4 T with Frémy’s Salt
title_short Comparison of Overhauser DNP at 0.34 and 3.4 T with Frémy’s Salt
title_sort comparison of overhauser dnp at 0.34 and 3.4 t with frémy’s salt
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3396338/
https://www.ncbi.nlm.nih.gov/pubmed/22815593
http://dx.doi.org/10.1007/s00723-012-0362-5
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