<HashMap><database>biostudies-literature</database><scores/><additional><omics_type>Unknown</omics_type><volume>126(41)</volume><submitter>Shimon D</submitter><pubmed_abstract>We use microwave-induced dynamic nuclear polarization (DNP) of the substitutional nitrogen defects (P1 centers) in diamond to hyperpolarize bulk &lt;sup>13&lt;/sup>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 &lt;sup>13&lt;/sup>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 (&lt;i>m&lt;/i> &lt;sub>&lt;i>I&lt;/i>&lt;/sub> = 0) manifold o</pubmed_abstract><journal>The journal of physical chemistry. C, Nanomaterials and interfaces</journal><pagination>17777-17787</pagination><full_dataset_link>https://www.ebi.ac.uk/biostudies/studies/S-EPMC9589901</full_dataset_link><repository>biostudies-literature</repository><pubmed_title>Large Room Temperature Bulk DNP of &lt;sup>13&lt;/sup>C via P1 Centers in Diamond.</pubmed_title><pmcid>PMC9589901</pmcid><pubmed_authors>Joseph L</pubmed_authors><pubmed_authors>Williams EQ</pubmed_authors><pubmed_authors>Ramanathan C</pubmed_authors><pubmed_authors>Cantwell KA</pubmed_authors><pubmed_authors>Takahashi S</pubmed_authors><pubmed_authors>Shimon D</pubmed_authors><pubmed_authors>Peng Z</pubmed_authors></additional><is_claimable>false</is_claimable><name>Large Room Temperature Bulk DNP of &lt;sup>13&lt;/sup>C via P1 Centers in Diamond.</name><description>We use microwave-induced dynamic nuclear polarization (DNP) of the substitutional nitrogen defects (P1 centers) in diamond to hyperpolarize bulk &lt;sup>13&lt;/sup>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 &lt;sup>13&lt;/sup>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 (&lt;i>m&lt;/i> &lt;sub>&lt;i>I&lt;/i>&lt;/sub> = 0) manifold o</description><dates><release>2022-01-01T00:00:00Z</release><publication>2022 Oct</publication><modification>2025-04-04T23:19:53.51Z</modification><creation>2025-04-04T23:19:53.51Z</creation></dates><accession>S-EPMC9589901</accession><cross_references><pubmed>36304670</pubmed><doi>10.1021/acs.jpcc.2c06145</doi></cross_references></HashMap>