Fluorescence lifetimes have been determined for four strains of Rhodopseudomonas sphaeroides. Chromatophore samples were excited with a single picosecond flash, and the fluorescence was detected with a streak camera. The decay times are 100 psec in strains 2.4.1 and Ga, and 300 psec in the carotenoidless strain R-26. These times are related to the transfer of energy from the light-harvesting antenna pigment molecules to the photochemical reaction center. In strain PM-8 dpl, which lacks reaction centers, the lifetime is 1.1 nsec. In addition, we have obtained curves relating the quantum yield of fluorescence to the photon density of the excitation pulse. These curves can be fit with a simple model that relates excitonic processes to properties of the photosynthetic unit and that qualitatively describes differences between the mutant strains. Picosecond laser techniques are now being widely applied in this field of biophysics, especially in the area of photosynthesis. Picosecond flash-photolysis techniques have identified transitions occurring in the primary photochemical reaction in photosynthetic bacteria (1, 2), and streak-camera measurement techniques have been used to measure rapid transfer of excitations between chlorophyll molecules in vivo (3-6). Other recent biophysical applications of picosecond or subnanosecond techniques include measurements on hemoglobin (7), visual pigments (8), and DNA (9-11).This paper is concerned with a determination by picosecond techniques of the kinetics with which the light-harvesting antenna pigment molecules of photosynthetic bacteria transfer energy to the photochemical reaction center. We have used two approaches to this problem. In the first approach, the sample is excited with a 20-psec pulse of low intensity and the fluorescence lifetime is measured. This time reflects the rate of depopulation of excited singlet states of bacteriochlorophyll in the antenna, mainly due to their capture by the reaction center. In the second approach, high-intensity pulses are used to generate nonlinear optical effects. High intensities produce a high density of excited states, leading to exciton annihilation processes, as Mauzerall (12) has demonstrated with nanosecond pulses and Campillo et al. (13) with picosecond pulses. Such processes have now been studied by several groups (6, 12-18). When two or more singlet excitations are simultaneously present in the photosynthetic unit (or within a certain diffusion radius), they can migrate into the vicinity of one another, and singlet-singlet annihilation can take place by the reactions Si +Si Sn + SO [1] Sn -"Si + heat [21 Eq. 1 represents a bimolecular fusion process in which a molecule in the first excited singlet state SI transfers its energy to a similarly excited neighboring molecule, promoting it to a higher singlet state S,. Because higher excited singlet states in large molecules such as bacteriochlorophyll almost always decay nonradiatively to the S1 state, as shown in Eq. 2, the net result is the loss of one excited singlet...