THE NARROW-PULSE CRITERION FOR PULSED-GRADIENT SPIN-ECHO DIFFUSION MEASUREMENTS

Citation
Lz. Wang et al., THE NARROW-PULSE CRITERION FOR PULSED-GRADIENT SPIN-ECHO DIFFUSION MEASUREMENTS, Journal of magnetic resonance. Series A, 117(2), 1995, pp. 209-219
Citations number
29
Categorie Soggetti
Physics, Atomic, Molecular & Chemical
ISSN journal
10641858
Volume
117
Issue
2
Year of publication
1995
Pages
209 - 219
Database
ISI
SICI code
1064-1858(1995)117:2<209:TNCFPS>2.0.ZU;2-Q
Abstract
The narrow-pulse criterion for pulsed-gradient NMR spin-echo diffusion in the presence of impenetrable barriers is examined from an expressi on by Stepisnik [Physica B 183, 343 (1993)] for the attenuation caused by diffusion in any magnetic-field gradient for various parameters. T hese parameters are delta, Delta, a, D, and g, where delta and Delta a re the duration and the interval between bipolar magnetic-field-gradie nt pulses, respectively, a is the separation of the impenetrable barri ers, D is the diffusion coefficient, and g is the gradient strength. T he pulsed-gradient spin-echo (PGSE) experiment is a subclass of this s et. The attenuation, with the assumption that the diffusive motion of the spins leads to Gaussian distribution of spin phases, goes to known expressions in the free-diffusion (Delta D/a(2) much less than 1), re stricted-diffusion (delta D/a(2) much less than 1 much less than Delta D/a(2)), and rapid-diffusion (1 much less than delta D/a(2)) limits. This general expression is found to be valid for all combinations of D elta and delta provided that gamma delta ga/2 pi = qa much less than 1 . A criterion for the applicability of the commonly used narrow-pulse expressions for the signal attenuation is calculated from the fraction F of total attenuation that takes place only during the gradient. An independent check was performed from the shifts of the diffraction min ima as a function of increasing pulse widths obtained from the simulat ion by Blees [J. Magn. Reson. A 109, 203 (1994)]. If the narrow-pulse criterion is valid for F much less than 0.1 or for less than a 5% shif t in the second minimum of the diffraction pattern, a sufficient condi tion for its applicability is delta D/a(2) much less than 0.02, a much more stringent condition than is usually supposed. (C) 1995 Academic Press, Inc.