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Pure Isotropic Proton Solid State NMR
Author(s) -
Pinelopi Moutzouri,
Bruno Simões de Almeida,
Daria Torodii,
Lyndon Emsley
Publication year - 2021
Publication title -
journal of the american chemical society
Language(s) - Uncategorized
Resource type - Journals
SCImago Journal Rank - 7.115
H-Index - 612
eISSN - 1520-5126
pISSN - 0002-7863
DOI - 10.1021/jacs.1c03315
Subject(s) - isotropy , chemistry , magic angle spinning , spectral line , spinning , imperfect , solid state nuclear magnetic resonance , proton , pulse sequence , resolution (logic) , spectroscopy , series (stratigraphy) , range (aeronautics) , nuclear magnetic resonance spectroscopy , nmr spectra database , representation (politics) , statistical physics , computational physics , analytical chemistry (journal) , nuclear magnetic resonance , optics , physics , quantum mechanics , stereochemistry , materials science , chromatography , philosophy , artificial intelligence , law , linguistics , computer science , composite material , biology , paleontology , political science , politics , polymer chemistry
Resolution in proton solid state magic angle sample spinning (MAS) NMR is limited by the intrinsically imperfect nature of coherent averaging induced by either MAS or multiple pulse sequence methods. Here, we suggest that instead of optimizing and perfecting a coherent averaging scheme, we could approach the problem by parametrically mapping the error terms due to imperfect averaging in a k -space representation, in such a way that they can be removed in a multidimensional correlation leaving only the desired pure isotropic signal. We illustrate the approach here by determining pure isotropic 1 H spectra from a series of MAS spectra acquired at different spinning rates. For six different organic solids, the approach is shown to produce pure isotropic 1 H spectra that are significantly narrower than the MAS spectrum acquired at the fastest possible rate, with linewidths down to as little as 48 Hz. On average, we observe a 7-fold increase in resolution, and up to a factor of 20, as compared with spectra acquired at 100 kHz MAS. The approach is directly applicable to a range of solids, and we anticipate that the same underlying principle for removing errors introduced here can be applied to other problems in NMR spectroscopy.

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