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Date publication

avril 2024

Journal

Journal of magnetic resonance (San Diego, Calif. : 1997)

Auteurs

Membres identifiés du Cancéropôle Est :
Mr LECLERC Sébastien


Tous les auteurs :
Guendouz L, Leclerc S, Canet D

Résumé

The measurement of translational diffusion coefficients by NMR generally makes use basically of two magnetic field gradient pulses separated by a so-called diffusion interval. The magnetic field gradient arises either from the static magnetic field (denoted by B used for polarizing the nuclear spins) or from the radio-frequency field (denoted by B used for inducing NMR transitions). The B method may be hampered by short effective transverse relaxation times (T), by important gradient rise and fall times or by eddy currents. This does not occur with B gradients. Moreover, the effect of short transverse relaxation times during the gradient pulses is reduced by at least a factor of two. However, for B gradients, one might face with the limited volume in which the gradient is uniform and with the effect of short relaxation times which imply to reduce the various intervals in the diffusion experiment (this is as well true for the B method). Examples will be given for which the measurement of the diffusion coefficient by B gradients turned out to be impossible while a proper result was obtained with B gradients as far as a correction taking into account the limited volume is applied, together with a correction about the gradient calibration especially when dealing with samples containing paramagnetic species.

Mots clés

Diffusion measurements, Radio-frequency field gradients

Référence

J Magn Reson. 2024 04;361:107668