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Large Room Temperature Bulk DNP of (13)C via P1 Centers in Diamond

[Image: see text] We use microwave-induced dynamic nuclear polarization (DNP) of the substitutional nitrogen defects (P1 centers) in diamond to hyperpolarize bulk (13)C nuclei in both single crystal and powder samples at room temperature at 3.34 T. The large (>100-fold) enhancements demonstrated...

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Autores principales: Shimon, Daphna, Cantwell, Kelly A., Joseph, Linta, Williams, Ethan Q., Peng, Zaili, Takahashi, Susumu, Ramanathan, Chandrasekhar
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2022
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9589901/
https://www.ncbi.nlm.nih.gov/pubmed/36304670
http://dx.doi.org/10.1021/acs.jpcc.2c06145
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author Shimon, Daphna
Cantwell, Kelly A.
Joseph, Linta
Williams, Ethan Q.
Peng, Zaili
Takahashi, Susumu
Ramanathan, Chandrasekhar
author_facet Shimon, Daphna
Cantwell, Kelly A.
Joseph, Linta
Williams, Ethan Q.
Peng, Zaili
Takahashi, Susumu
Ramanathan, Chandrasekhar
author_sort Shimon, Daphna
collection PubMed
description [Image: see text] We use microwave-induced dynamic nuclear polarization (DNP) of the substitutional nitrogen defects (P1 centers) in diamond to hyperpolarize bulk (13)C nuclei in both single crystal and powder samples at room temperature at 3.34 T. The large (>100-fold) enhancements demonstrated correspond to a greater than 10 000-fold improvement in terms of signal averaging of the 1% abundant (13)C spins. The DNP was performed using low-power solid state sources under static (nonspinning) conditions. The DNP spectrum (DNP enhancement as a function of microwave frequency) of diamond powder shows features that broadly correlate with the EPR spectrum. A well-defined negative Overhauser peak and two solid effect peaks are observed for the central (m(I) = 0) manifold of the (14)N spins. Previous low temperature measurements in diamond had measured a positive Overhauser enhancement in this manifold. Frequency-chirped millimeter-wave excitation of the electron spins is seen to significantly improve the enhancements for the two outer nuclear spin manifolds (m(I) = ±1) and to blur some of the sharper features associated with the central manifold. The outer lines are best fit using a combination of the cross effect and the truncated cross effect, which is known to mimic features of an Overhauser effect. Similar features are also observed in experiments on single crystal samples. The observation of all of these mechanisms in a single material system under the same experimental conditions is likely due to the significant heterogeneity of the high pressure, high temperature (HPHT) type Ib diamond samples used. Large room temperature DNP enhancements at fields above a few tesla enable spectroscopic studies with better chemical shift resolution under ambient conditions.
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spelling pubmed-95899012022-10-25 Large Room Temperature Bulk DNP of (13)C via P1 Centers in Diamond Shimon, Daphna Cantwell, Kelly A. Joseph, Linta Williams, Ethan Q. Peng, Zaili Takahashi, Susumu Ramanathan, Chandrasekhar J Phys Chem C Nanomater Interfaces [Image: see text] We use microwave-induced dynamic nuclear polarization (DNP) of the substitutional nitrogen defects (P1 centers) in diamond to hyperpolarize bulk (13)C nuclei in both single crystal and powder samples at room temperature at 3.34 T. The large (>100-fold) enhancements demonstrated correspond to a greater than 10 000-fold improvement in terms of signal averaging of the 1% abundant (13)C spins. The DNP was performed using low-power solid state sources under static (nonspinning) conditions. The DNP spectrum (DNP enhancement as a function of microwave frequency) of diamond powder shows features that broadly correlate with the EPR spectrum. A well-defined negative Overhauser peak and two solid effect peaks are observed for the central (m(I) = 0) manifold of the (14)N spins. Previous low temperature measurements in diamond had measured a positive Overhauser enhancement in this manifold. Frequency-chirped millimeter-wave excitation of the electron spins is seen to significantly improve the enhancements for the two outer nuclear spin manifolds (m(I) = ±1) and to blur some of the sharper features associated with the central manifold. The outer lines are best fit using a combination of the cross effect and the truncated cross effect, which is known to mimic features of an Overhauser effect. Similar features are also observed in experiments on single crystal samples. The observation of all of these mechanisms in a single material system under the same experimental conditions is likely due to the significant heterogeneity of the high pressure, high temperature (HPHT) type Ib diamond samples used. Large room temperature DNP enhancements at fields above a few tesla enable spectroscopic studies with better chemical shift resolution under ambient conditions. American Chemical Society 2022-10-03 2022-10-20 /pmc/articles/PMC9589901/ /pubmed/36304670 http://dx.doi.org/10.1021/acs.jpcc.2c06145 Text en © 2022 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 Shimon, Daphna
Cantwell, Kelly A.
Joseph, Linta
Williams, Ethan Q.
Peng, Zaili
Takahashi, Susumu
Ramanathan, Chandrasekhar
Large Room Temperature Bulk DNP of (13)C via P1 Centers in Diamond
title Large Room Temperature Bulk DNP of (13)C via P1 Centers in Diamond
title_full Large Room Temperature Bulk DNP of (13)C via P1 Centers in Diamond
title_fullStr Large Room Temperature Bulk DNP of (13)C via P1 Centers in Diamond
title_full_unstemmed Large Room Temperature Bulk DNP of (13)C via P1 Centers in Diamond
title_short Large Room Temperature Bulk DNP of (13)C via P1 Centers in Diamond
title_sort large room temperature bulk dnp of (13)c via p1 centers in diamond
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9589901/
https://www.ncbi.nlm.nih.gov/pubmed/36304670
http://dx.doi.org/10.1021/acs.jpcc.2c06145
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