Lj. Zielinski et Pn. Sen, Relaxation of nuclear magnetization in a nonuniform magnetic field gradient and in a restricted geometry, J MAGN RES, 147(1), 2000, pp. 95-103
We study the influence of restriction on Carr-Purcell-Meiboom-Gill spin ech
o response of magnetization of spins diffusing in a bounded region in the p
resence of a nonuniform magnetic field gradient. We consider two fields in
detail-a parabolic field which, like the uniform-gradient field, scales wit
h the system size, and a cosine field which remains bounded. Corresponding
to three main length scales, the pore size, L-S, the dephasing length, L-G,
and the diffusion length during half-echo time, L-D, we identify three mai
n regimes of decay of the total magnetization: motionally averaged, localiz
ation, and short-time. In the short-time regime (L-D << L-S, L-G), we confi
rm that the leading order behavior is controlled by the average of the squa
re of the gradient, <((<del>B-z)(2))over bar>, and in the motionally averag
ed regime (MAv), where L-S << L-D, L-G, by <((<integral> dxBz)(2))over bar>
. We verify numerically that two different fields for which those two avera
ges are identical result in very similar decay profiles not only in the lim
its of short and long times but also in the intermediate times, with import
ant practical implications. In the motionally averaged regime we found that
previous estimates of the decay exponent for the parabolic field, based on
a soft-boundary condition, are significantly altered in the presence of a
more realistic, hard wall. We find the scaling of the decay exponent in the
MAv regime with pore size to be L-S(2) for the cosine field and L-S(6) for
the parabolic field, as contrasted with the linear gradient scaling of L-S
(4). In the localization regime, for both the cosine and the parabolic fiel
ds, the decay exponent depends on a fractional power of the gradient, imply
ing a breakdown of the second cumulant or the Gaussian phase approximation.
We also examined the validity of time-evolving the total magnetization acc
ording to a distribution of effective local gradients and found that such a
pproximation works well only in the short-time regime and breaks down stron
gly for long times. (C) 2000 Academic Press.