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Article Dans Une Revue Journal of Chemical Physics Année : 2008

Solid-state NMR covariance of homonuclear correlation spectra

Résumé

Direct covariance NMR spectroscopy, which does not involve a Fourier transformation along the indirect dimension, is demonstrated to obtain homonuclear correlation two-dimensional (2D) spectra in the solid state. In contrast to the usual 2D Fourier transform (2D-FT) NMR, in a 2D covariance (2D-Cov) spectrum the spectral resolution in the indirect dimension is determined by the resolution along the detection dimension, thereby largely reducing the time-consuming indirect sampling requirement. The covariance method does not need any separate phase correction or apodization along the indirect dimension because it uses those applied in the detection dimension. We compare in detail the specifications obtained with 2D-FT and 2D-Cov, for narrow and broad resonances. The efficiency of the covariance data treatment is demonstrated in organic and inorganic samples that are both well crystallized and amorphous, for spin -12 nuclei with C13, Si29, and P31 through-space or through-bond homonuclear 2D correlation spectra. In all cases, the experimental time has been reduced by at least a factor of 10, without any loss of resolution and signal to noise ratio, with respect to what is necessary with the 2D-FT NMR. According to this method, we have been able to study the silicate network of glasses by 2D NMR within reasonable experimental time despite the very long relaxation time of the Si29 nucleus. The main limitation of the 2D-Cov data treatment is related to the introduction of autocorrelated peaks onto the diagonal, which does not represent any actual connectivity.

Domaines

Matériaux
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Dates et versions

hal-00289875 , version 1 (23-06-2008)

Identifiants

Citer

Jean-Paul Amoureux, Bingwen Hu, Julien Trébosc, Michaël Deschamps, Grégory Tricot. Solid-state NMR covariance of homonuclear correlation spectra. Journal of Chemical Physics, 2008, 128,, pp.134502. ⟨10.1063/1.2884341⟩. ⟨hal-00289875⟩
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