Abstract
We have observed a peak in the inelastic light scattering of CdS in high magnetic fields at an energy slightly less than twice the bound electron spin-flip energy μgH. The intensity, selection rules, field dependence, and binding energy of this process cannot be explained as second-order scattering. At very high excitation energies (>~1 MW/cm2) the single spin-flip scattering becomes stimulated, with a sharp threshold and high conversion efficiency.