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Asymmetric C13–C13 polarization transfer under dipolar-assisted rotational resonance in magic-angle spinning NMR
A two-dimensional (2D) homonuclear exchange NMR spectrum in solids often shows an asymmetric cross-peak pattern, which disturbs a quantitative analysis of peak intensities. When magnetization is prepared using cross polarization (CP), the asymmetry can naively be ascribed to nonequilibrium initial m...
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Published in: | The Journal of chemical physics 2006-12, Vol.125 (21) |
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Main Authors: | , |
Format: | Article |
Language: | English |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | A two-dimensional (2D) homonuclear exchange NMR spectrum in solids often shows an asymmetric cross-peak pattern, which disturbs a quantitative analysis of peak intensities. When magnetization is prepared using cross polarization (CP), the asymmetry can naively be ascribed to nonequilibrium initial magnetization. We show, however, that the CP effect cannot fully explain the observed mixing-time dependence of the peak intensities in 2D C13–C13 exchange spectra of [2,3-C13] l-alanine (2,3-Ala) under C13–H1 dipolar-assisted rotational resonance (DARR) recoupling, which has recently been proposed for a broadband recoupling method under magic-angle spinning. We develop a theory to describe polarization transfer in a two-spin system under DARR recoupling. By taking into account the effects of the partial spectral overlap among C13 signals, which is a unique feature of DARR recoupling, and H1–H1 flip-flop exchange, we can successfully explain the observed mixing-time dependence of the peak intensities of 2D C13–C13 DARR exchange spectra of 2,3-Ala. A simple initial-rate analysis is also examined. |
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ISSN: | 0021-9606 1089-7690 |
DOI: | 10.1063/1.2364503 |