This sequence is intended for direct polarization experiments on nuclei with significant background signals arising from probe materials, e.g., 1H, 19F, 13C, 29Si, 11B, among others. It will be most effective in spin-1/2 systems, and may have limited utilities for quadrupolar nuclei such as 11B. If the B1 field of the probe is not sufficiently homogeneous, this sequence can have an effect on the relative integrated intensities of the peaks in the spectrum.