2008
DOI: 10.1016/j.jmr.2008.05.013
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3D 1H–13C–14N correlation solid-state NMR spectrum

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Cited by 21 publications
(31 citation statements)
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“…The selectivity with which 1 H-13 C cross-peaks are observed can be controlled by a selective (differing) 1 H-13 C cross-polarization step. It must be noted that this experiment does not require a very large magnetic field, a perfectly adjusted magic angle or a perfectly stabilized spinning speed, as with previous 1 H- 14 N and 13 C-14 N HMQC experiments [9][10][11][12][13][14]. Indeed, the different 14 N magnetizations are utilized, instead of being observed as previously.…”
Section: Resultsmentioning
confidence: 89%
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“…The selectivity with which 1 H-13 C cross-peaks are observed can be controlled by a selective (differing) 1 H-13 C cross-polarization step. It must be noted that this experiment does not require a very large magnetic field, a perfectly adjusted magic angle or a perfectly stabilized spinning speed, as with previous 1 H- 14 N and 13 C-14 N HMQC experiments [9][10][11][12][13][14]. Indeed, the different 14 N magnetizations are utilized, instead of being observed as previously.…”
Section: Resultsmentioning
confidence: 89%
“…Spectra (b and c) are acquired using a pulse sequence that selects pure SQ 14 close proximity to nitrogen-14 nuclei. The selectivity with which 1 H-13 C cross-peaks are observed can be controlled by a selective (differing) 1 H-13 C cross-polarization step.…”
Section: Resultsmentioning
confidence: 99%
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