Enhancing the resolution of 1H and 13C solid-state NMR spectra by reduction of anisotropic bulk magnetic susceptibility broadening

dc.contributor.author Hanrahan, Michael
dc.contributor.author Venkatesh, Amrit
dc.contributor.author Carnahan, Scott
dc.contributor.author Calahan, Julie
dc.contributor.author Lubach, Joseph
dc.contributor.author Munson, Eric
dc.contributor.author Rossini, Aaron
dc.contributor.department Ames National Laboratory
dc.contributor.department Department of Chemistry
dc.contributor.department Ames Laboratory
dc.date 2018-08-09T21:57:18.000
dc.date.accessioned 2020-06-29T23:22:57Z
dc.date.available 2020-06-29T23:22:57Z
dc.date.embargo 2018-09-25
dc.date.issued 2017-01-01
dc.description.abstract <p>We demonstrate that natural isotopic abundance 2D heteronuclear correlation (HETCOR) solid-state NMR spectra can be used to significantly reduce or eliminate the broadening of 1H and 13C solid-state NMR spectra of organic solids due to anisotropic bulk magnetic susceptibility (ABMS). ABMS often manifests in solids with aromatic groups, such as active pharmaceutical ingredients (APIs), and inhomogeneously broadens the NMR peaks of all nuclei in the sample. Inhomogeneous peaks with full widths at half maximum (FWHM) of ∼1 ppm typically result from ABMS broadening and the low spectral resolution impedes the analysis of solid-state NMR spectra. ABMS broadening of solid-state NMR spectra has previously been eliminated using 2D multiple-quantum correlation experiments, or by performing NMR experiments on diluted materials or single crystals. However, these experiments are often infeasible due to their poor sensitivity and/or provide limited gains in resolution. 2D 1H–13C HETCOR experiments have previously been applied to reduce susceptibility broadening in paramagnetic solids and we show that this strategy can significantly reduce ABMS broadening in diamagnetic organic solids. Comparisons of 1D solid-state NMR spectra and 1H and 13C solid-state NMR spectra obtained from 2D 1H–13C HETCOR NMR spectra show that the HETCOR spectrum directly increases resolution by a factor of 1.5 to 8. The direct gain in resolution is determined by the ratio of the inhomogeneous 13C/1H linewidth to the homogeneous 1H linewidth, with the former depending on the magnitude of the ABMS broadening and the strength of the applied field and the latter on the efficiency of homonuclear decoupling. The direct gains in resolution obtained using the 2D HETCOR experiments are better than that obtained by dilution. For solids with long proton longitudinal relaxation times, dynamic nuclear polarization (DNP) was applied to enhance sensitivity and enable the acquisition of 2D 1H–13C HETCOR NMR spectra. 2D 1H–13C HETCOR experiments were applied to resolve and partially assign the NMR signals of the form I and form II polymorphs of aspirin in a sample containing both forms. These findings have important implications for ultra-high field NMR experiments, optimization of decoupling schemes and assessment of the fundamental limits on the resolution of solid-state NMR spectra.</p>
dc.identifier archive/lib.dr.iastate.edu/ameslab_manuscripts/41/
dc.identifier.articleid 1044
dc.identifier.contextkey 11155255
dc.identifier.s3bucket isulib-bepress-aws-west
dc.identifier.submissionpath ameslab_manuscripts/41
dc.identifier.uri https://dr.lib.iastate.edu/handle/20.500.12876/7354
dc.language.iso en
dc.relation.ispartofseries IS-J 9484
dc.source.bitstream archive/lib.dr.iastate.edu/ameslab_manuscripts/41/IS_J_9484.pdf|||Sat Jan 15 00:09:59 UTC 2022
dc.source.uri 10.1039/C7CP04223J
dc.subject.disciplines Analytical Chemistry
dc.subject.disciplines Chemistry
dc.subject.disciplines Physical Chemistry
dc.title Enhancing the resolution of 1H and 13C solid-state NMR spectra by reduction of anisotropic bulk magnetic susceptibility broadening
dc.type article
dc.type.genre article
dspace.entity.type Publication
relation.isAuthorOfPublication f6703e72-8e9d-40df-b839-5a9ab4da888d
relation.isOrgUnitOfPublication 25913818-6714-4be5-89a6-f70c8facdf7e
relation.isOrgUnitOfPublication 42864f6e-7a3d-4be3-8b5a-0ae3c3830a11
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