Excitation sculpting (T-L. Hwang and A. J. Shaka, J. Magn. Reson, A 112, 27
5-279 (1995)) used for solvent suppression and selective excitation in NMR
bases its success on the ability to remove baseline and phase errors create
d by the application of selective rf pulses. This is achieved by the applic
ation of two pulsed field gradient (PFG) echoes in sequence. It is essentia
l that the two pairs of PFGs select the coherence transfer steps independen
tly of each other, which is conveniently achieved if they are applied along
orthogonal spatial axes, Here, the much more common case where both PFG pa
irs must be applied along a single axis is investigated. This is shown to l
ead to complications for certain ratios of PFG strengths. The original theo
ry of excitation sculpting is restated in the spherical basis for convenien
ce. Some of the effects can only be explained by invoking the dipolar demag
netizing field. (C) 1999 Academic Press.