As the use of volume-selective nuclear magnetic resonance has become more widespread, both for high-resolution spectroscopy and for “zoom-imaging,” so techniques for extracting signal from a reduced volume of spins within an extended sample have proliferated. The most versatile and generally applicable are those involving magnetic field B,-, gradients in conjunction with selective RF pulses and they fall broadly into two groups: techniques which achieve localization by selectively exciting spins inside the volume of interest and those which saturate all the magnetization except that within the volume of interest. From the former group the STEAM (I) sequence, involving stimulated echoes, is probably the most easily implemented. As with all echo techniques, the results are T2 weighted, which rules out its application to short T2 species such as 31P metabolites, but proves favorable for water and lipid suppression in ‘H metabolite detection. DRESS (2) achieves good sensitivity with surface coils but also suffers from T2 limitations, while the OSIRIS (3) technique is useful for observing fast relaxing magnetization although it suffers from pulse bandwidth limitations and unlike STEAM, it is not feasible to shim on the selected volume. New techniques which achieve 2D selective excitation in a single radiofrequency/gradient pulse and are much less limited by T2 relaxation have recently been developed (4, 5). However, they also suffer from problems such as poor outer volume suppression, difficulty in moving the selected volume under computer control, and off-resonance effects. Localization methods which work by removing signal contributions from outside the volume of interest through saturation are particularly attractive because of their T2 independence, an important factor for 31P in vivo work. Such methods include VSE (6)) SPARS ( 7)) SPACE (8), and DIGGER ( 9). All of these selectively create transverse magnetization outside the volume of interest at some point in the pulse sequence which is then dephased by the applied field gradients, while magnetization inside the volume of interest is stored along the 2 axis. A problem common to all these existing techniques is the high RF power level required to saturate all the spins in the outer volume. Other problems associated with pulse bandwidth and pulse imperfections mean that spins near the edge of the sample are not fully saturated while some magnetization is excited inside the volume of interest. Also, since these tech-