Stimulated emission and lasing have been demonstrated for chlorophyll a, chlorophyll b, and bacteriochlorophyll a as well as for the Mg-free chlorophyll derivatives pheophytin a and methyl pheophorbide a. Population inversion was obtained by optically pumping with an N2 laser. For the three chlorophylls, lasing was observed for only the (0,0) vibronic region of the SI -_ So fluorescence band. In contrast, lasing was observed for both the (0,0) and (0,1) vibronic regions of the SI SO fluorescence band of pheophytin a and methyl pheophorbide a. Differences between the lasing behavior of the chlorophylls and the Mg-free derivatives probably reflect differences in aggregation behavior. Laser pulses of duration shorter than the fluorescence lifetimes were generated. This result suggests that stimulated emission must be considered in the interpretation of fluorescence lifetime data for in vitro and in vivo chlorophyll-containing systems.Chlorophylls (Chi) are the principal photoreceptors for photosynthesis in green plants, algae, and bacteria as well as the electron donors in the primary event of photosynthesis. It is therefore not surprising that keen interest continues in the excited electronic states of the chlorophylls and their Mg-free derivatives. The chlorophylls are intensely fluorescent, and consideration of the lifetimes of the first excited singlet states (SI) and the fluorescence quantum yields suggested that the chlorophylls should have the ability to function as dye lasers. In addition to the usefulness of ChI dye lasers in photosynthesis experiments, lasing of the chlorophylls could be expected to yield interesting information about the properties of their SI electronic states. This has proved to be the case. Chlorophyll a (Chi a), chlorophyll b (Chi b), bacteriochlorophyll a (Bchl a), and the Mg-free derivatives pheophytin a (Pheo a) and methyl pheophorbide a (MePheo a) all have excellent lasing properties, some of which we describe in this paper. The Mg-free derivatives exhibit an interesting, although not unprecedented, dependence of the lasing frequency on the concentration. The characteristics of the laser pulse raise some interesting questions, which we discuss below, about the properties of high densities of excited ChI electronic states such as may be produced in in vwo picosecond irradiations by high photon fluxes. EXPERIMENTAL A 1-MW N2 laser (Molectron model UV 1000) with output at 337.1 nm was used as an optical pump to produce population inversion. This N2 laser was also used as an excitation source for the fluorescence spectra. The experimental configuration was similar to that employed by Sorokin and Lankard (1) in the first demonstration of lasing from an organic compound, aluminum phthalocyanine chloride, in solution when pumped by a giant pulse ruby laser. The cells used for the lasing and fluorescence studies were stoppered 1-cm-square quartz cuvettes polished on all four sides. The laser cavity was defined by the two surfaces of the cuvette perpendicular to the optical pumpin...