1991
DOI: 10.1038/351467a0
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Diffraction-like effects in NMR diffusion studies of fluids in porous solids

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Cited by 620 publications
(564 citation statements)
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“…In highly regular porous structures, such as packed beads, the echo attenuation will exhibit diffraction peaks and pore geometry information can be directly read from the peaks (Callaghan et al, 1991). However, diffraction patterns in biological systems have only been observed in packed erythrocytes and not in tissues such as multi-axonal systems, possibly due to structural heterogeneity as our simulations suggest.…”
Section: Discussion Estimating Mean Axon Diameter With Qsimentioning
confidence: 85%
See 1 more Smart Citation
“…In highly regular porous structures, such as packed beads, the echo attenuation will exhibit diffraction peaks and pore geometry information can be directly read from the peaks (Callaghan et al, 1991). However, diffraction patterns in biological systems have only been observed in packed erythrocytes and not in tissues such as multi-axonal systems, possibly due to structural heterogeneity as our simulations suggest.…”
Section: Discussion Estimating Mean Axon Diameter With Qsimentioning
confidence: 85%
“…QSI allows assessment of microarchitecture by exploiting the regularity of restrictions to molecular diffusion in porous systems as applied to determine pore geometry in porous solids (Callaghan et al, 1991), the study of packed erythrocytes (Torres et al, 1998), and the assessment of axonal architecture (Chin et al, 2004;Cohen and Assaf, 2002;Malmborg et al, 2006). In WM tracts, the porous system consists of water diffusion restricted by axon membranes and myelin sheaths (Beaulieu, 2002).…”
Section: Introductionmentioning
confidence: 99%
“…The normalized signal, E[G d , ⌬], following the application of such a diffusion-sensitizing gradient pair is given by (9,16,17),…”
Section: Q-space Theorymentioning
confidence: 99%
“…As such, the signal attenuation curve (q-plot), is no longer linear with g 2 , even for single-component diffusion. When t is large enough for spins to completely sample the restrictions of a given pore, Ps reduces to the pore spin density function, ρ(r'), and the echo attenuation becomes the Fourier power spectrum of ρ(r') [5,24]. Specifically, for spins…”
Section: Methodsmentioning
confidence: 99%