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DOSY Experiments - Emory University

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<strong>DOSY</strong> pulse sequences use the gradient stimulated echo element (or one of its modifications):<br />

In the <strong>DOSY</strong> experiments the strength of the diffusion-encoding gradient is arrayed and the<br />

diffusion coefficients are calculated according to the Stejskal-Tanner formula:<br />

where S(Gzi) and S(0) are the signal intensities obtained with gradients strengths of Giz and 0,<br />

respectively, D is the diffusion coefficient, γ is the gyromagnetic constant, δ is the gradient pulse<br />

duration and Δ is the diffusion delay.<br />

From the formula alone one can get valuable hints on how to set <strong>DOSY</strong>-related parameters in<br />

different pulse sequences.<br />

(γδGzi) 2 – gradient pulse area squared<br />

a: nuclei with higher γ are more sensitive to diffusion than the low-γ nuclei. (If possible,<br />

observe 1 H or 19 F, or at least do the diffusion-encoding step on the high-γ nucleus (see<br />

Dbppsteinept).<br />

b: shaping a gradient dramatically reduces its phase encoding efficiency. Although the<br />

VNMR software enables the shaping of gradients on VNMRS or 400-MR spectrometers,<br />

it is not really recommended.<br />

δ – gradient pulse duration<br />

during δ (and the subsequent gradient stabilization delay, gstab) the magnetization is<br />

transverse and subject to T2 relaxation and homonuclear J-evolution. Do not use long δ<br />

values in the presence of large homonuclear couplings or short T2 relaxation times (δ

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