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By B. W Mangum

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48) shows the resulting density matrix at t = 2τ . When evaluating the resulting density matrix, it can be seen that the application of the 180° RF-pulse is equivalent to a change in the polarity of the effective magnetic field gradient. Thus, in the evaluation of the echo attenuation for more complicated PFGSTE sequences the 180° RF-pulse may be replaced by a change in sign of the magnetic field gradient following the RF-pulse. 56) Even though the cross term vanishes only if (δ1−δ2) = 0, it is significantly reduced as there is no Δ dependency.

Magn. Reson. S. Johnson Jr, Diffusion ordered nuclear magnetic resonance spectroscopy: principles and applications. Prog. Nucl. Magn. Reson. Spectrosc. M. Loening, J. A. Morris, One-dimensional DOSY. J. Magn. Reson. A. Morris, H. Barjat, Chapter 11 high resolution diffusion ordered spectroscopy, in Analytical Spectroscopy Library, ed. E. Kévér, Gy. Batta, Cs. Széntay (Elsevier, 1997), pp. M. A. Morris, Improving pulse sequences for 3D DOSY: convection compensation. J. Magn. Reson. A. , J-modulation effects in DOSY experiments and their suppression: the Oneshot45 experiment.

Instrum. H. D. S. Johnson, An improved diffusion-ordered spectroscopy experiment incorporating bipolar-gradient pulses. J. Magn. Reson. Y. M. Purcell, Effects of diffusion on free precession in nuclear magnetic resonance experiments. Phys. Rev. H. , Improved convection compensating pulsed field gradient spin-echo and stimulated-echo methods. J. Magn. Reson. H. W. Anthonsen, K. Zick, J. Sjoblom, A spoiler recovery method for rapid diffusion measurements. Diffus. Fundam. H. Sørland, Characterization of emulsions by PFG-NMR.

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