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The Effect of Disorder on Endogenous MAS-DNP: Study of Silicate Glasses and Crystals

[Image: see text] In dynamic nuclear polarization nuclear magnetic resonance (DNP-NMR) experiments, the large Boltzmann polarization of unpaired electrons is transferred to surrounding nuclei, leading to a significant increase in the sensitivity of the NMR signal. In order to obtain large polarizati...

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Autores principales: Thomas, Brijith, Jardón-Álvarez, Daniel, Carmieli, Raanan, van Tol, Johan, Leskes, Michal
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2023
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10009812/
https://www.ncbi.nlm.nih.gov/pubmed/36925559
http://dx.doi.org/10.1021/acs.jpcc.2c08849
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author Thomas, Brijith
Jardón-Álvarez, Daniel
Carmieli, Raanan
van Tol, Johan
Leskes, Michal
author_facet Thomas, Brijith
Jardón-Álvarez, Daniel
Carmieli, Raanan
van Tol, Johan
Leskes, Michal
author_sort Thomas, Brijith
collection PubMed
description [Image: see text] In dynamic nuclear polarization nuclear magnetic resonance (DNP-NMR) experiments, the large Boltzmann polarization of unpaired electrons is transferred to surrounding nuclei, leading to a significant increase in the sensitivity of the NMR signal. In order to obtain large polarization gains in the bulk of inorganic samples, paramagnetic metal ions are introduced as minor dopants acting as polarizing agents. While this approach has been shown to be very efficient in crystalline inorganic oxides, significantly lower enhancements have been reported when applying this approach to oxide glasses. In order to rationalize the origin of the difference in the efficiency of DNP in amorphous and crystalline inorganic matrices, we performed a detailed comparison in terms of their magnetic resonance properties. To diminish differences in the DNP performance arising from distinct nuclear interactions, glass and crystal systems of similar compositions were chosen, Li(2)OCaO·2SiO(2) and Li(2)CaSiO(4), respectively. Using Gd(III) as polarizing agent, DNP provided signal enhancements in the range of 100 for the crystalline sample, while only up to around factor 5 in the glass, for both (6)Li and (29)Si nuclei. We find that the drop in enhancement in glasses can be attributed to three main factors: shorter nuclear and electron relaxation times as well as the dielectric properties of glass and crystal. The amorphous nature of the glass sample is responsible for a high dielectric loss, leading to efficient microwave absorption and consequently lower effective microwave power and an increase in sample temperature which leads to further reduction of the electron relaxation time. These results help rationalize the observed sensitivity enhancements and provide guidance in identifying materials that could benefit from the DNP approach.
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spelling pubmed-100098122023-03-14 The Effect of Disorder on Endogenous MAS-DNP: Study of Silicate Glasses and Crystals Thomas, Brijith Jardón-Álvarez, Daniel Carmieli, Raanan van Tol, Johan Leskes, Michal J Phys Chem C Nanomater Interfaces [Image: see text] In dynamic nuclear polarization nuclear magnetic resonance (DNP-NMR) experiments, the large Boltzmann polarization of unpaired electrons is transferred to surrounding nuclei, leading to a significant increase in the sensitivity of the NMR signal. In order to obtain large polarization gains in the bulk of inorganic samples, paramagnetic metal ions are introduced as minor dopants acting as polarizing agents. While this approach has been shown to be very efficient in crystalline inorganic oxides, significantly lower enhancements have been reported when applying this approach to oxide glasses. In order to rationalize the origin of the difference in the efficiency of DNP in amorphous and crystalline inorganic matrices, we performed a detailed comparison in terms of their magnetic resonance properties. To diminish differences in the DNP performance arising from distinct nuclear interactions, glass and crystal systems of similar compositions were chosen, Li(2)OCaO·2SiO(2) and Li(2)CaSiO(4), respectively. Using Gd(III) as polarizing agent, DNP provided signal enhancements in the range of 100 for the crystalline sample, while only up to around factor 5 in the glass, for both (6)Li and (29)Si nuclei. We find that the drop in enhancement in glasses can be attributed to three main factors: shorter nuclear and electron relaxation times as well as the dielectric properties of glass and crystal. The amorphous nature of the glass sample is responsible for a high dielectric loss, leading to efficient microwave absorption and consequently lower effective microwave power and an increase in sample temperature which leads to further reduction of the electron relaxation time. These results help rationalize the observed sensitivity enhancements and provide guidance in identifying materials that could benefit from the DNP approach. American Chemical Society 2023-02-27 /pmc/articles/PMC10009812/ /pubmed/36925559 http://dx.doi.org/10.1021/acs.jpcc.2c08849 Text en © 2023 The Authors. Published by American Chemical Society https://creativecommons.org/licenses/by/4.0/Permits the broadest form of re-use including for commercial purposes, provided that author attribution and integrity are maintained (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Thomas, Brijith
Jardón-Álvarez, Daniel
Carmieli, Raanan
van Tol, Johan
Leskes, Michal
The Effect of Disorder on Endogenous MAS-DNP: Study of Silicate Glasses and Crystals
title The Effect of Disorder on Endogenous MAS-DNP: Study of Silicate Glasses and Crystals
title_full The Effect of Disorder on Endogenous MAS-DNP: Study of Silicate Glasses and Crystals
title_fullStr The Effect of Disorder on Endogenous MAS-DNP: Study of Silicate Glasses and Crystals
title_full_unstemmed The Effect of Disorder on Endogenous MAS-DNP: Study of Silicate Glasses and Crystals
title_short The Effect of Disorder on Endogenous MAS-DNP: Study of Silicate Glasses and Crystals
title_sort effect of disorder on endogenous mas-dnp: study of silicate glasses and crystals
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10009812/
https://www.ncbi.nlm.nih.gov/pubmed/36925559
http://dx.doi.org/10.1021/acs.jpcc.2c08849
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