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research article

Single crystal nuclear magnetic resonance in spinning powders

Pell, Andrew J.
•
Pintacuda, Guido
•
Emsley, Lyndon  
2011
Journal of Chemical Physics

We present a method for selectively exciting nuclear magnetic resonances (NMRs) from well-defined subsets of crystallites from a powdered sample under magic angle spinning. Magic angle spinning induces a time dependence in the anisotropic interactions, which results in a time variation of the resonance frequencies which is different for different crystallite orientations. The proposed method exploits this by applying selective pulses, which we refer to as XS (for crystallite-selective) pulses, that follow the resonance frequencies of nuclear species within particular crystallites, resulting in the induced flip angle being orientation dependent. By selecting the radiofrequency field to deliver a 180 degrees pulse for the target orientation and employing a train of such pulses combined with cogwheel phase cycling, we obtain a high degree of orientational selectivity with the resulting spectrum containing only contributions from orientations close to the target. Typically, this leads to the selection of between 0.1% and 10% of the crystallites, and in extreme cases to the excitation of a single orientation resulting in single crystal spectra of spinning powders. Two formulations of this method are described and demonstrated with experimental examples on [1 -(13) C]-alanine and the paramagnetic compound Sm(2)Sn(2)O(7). (C) 2011 American Institute of Physics. [doi:10.1063/1.3640418]

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Type
research article
DOI
10.1063/1.3640418
Web of Science ID

WOS:000295884400028

Author(s)
Pell, Andrew J.
Pintacuda, Guido
Emsley, Lyndon  
Date Issued

2011

Publisher

AMER INST PHYSICS

Published in
Journal of Chemical Physics
Volume

135

Issue

14

Article Number

144201

Editorial or Peer reviewed

REVIEWED

Written at

OTHER

EPFL units
LRM  
Available on Infoscience
January 8, 2015
Use this identifier to reference this record
https://infoscience.epfl.ch/handle/20.500.14299/110001
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