Time-resolved excited-state absorption intensities after direct twophoton excitation of the carotenoid S 1 state are reported for light-harvesting complexes of purple bacteria. Direct excitation of the carotenoid S 1 state enables the measurement of subsequent dynamics on a fs time scale without interference from higher excited states, such as the optically allowed S 2 state or the recently discovered dark state situated between S1 and S2. The lifetimes of the carotenoid S 1 states in the B800-B850 complex and B800-B820 complex of Rhodopseudomonas acidophila are 7 ؎ 0.5 ps and 6 ؎ 0.5 ps, respectively, and in the light-harvesting complex 2 of Rhodobacter sphaeroides Ϸ1.9 ؎ 0.5 ps. These results explain the differences in the carotenoid to bacteriochlorophyll energy transfer efficiency after S 2 excitation. In Rps. acidophila the carotenoid S1 to bacteriochlorophyll energy transfer is found to be quite inefficient ( ET1 <28%) whereas in Rb. sphaeroides this energy transfer is very efficient ( ET1 Ϸ80%). The results are rationalized by calculations of the ensemble averaged time constants. We find that the Car S 1 3 B800 electronic energy transfer (EET) pathway (Ϸ85%) dominates over Car S 1 3 B850 EET (Ϸ15%) in Rb. sphaeroides, whereas in Rps. acidophila the Car S 1 3 B850 EET (Ϸ60%) is more efficient than the Car S 1 3 B800 EET (Ϸ40%). The individual electronic couplings for the Car S1 3 BChl energy transfer are estimated to be approximately 5-26 cm ؊1 . A major contribution to the difference between the energy transfer efficiencies can be explained by different Car S 1 energy gaps in the two species. P lants and some bacteria have achieved remarkably high efficiencies of solar light conversion in photosynthesis. Recently, high-resolution crystal structures of some peripheral light-harvesting complexes of photosynthetic purple bacteria (1-3) have become available, enabling us to study the basic principles of the highly efficient collection of solar energy (4-8).In the light-harvesting complexes of purple bacteria, such as light-harvesting complex 2 (LH2) of Rhodobacter sphaeroides or Rhodopseudomonas acidophila, carotenoids (Cars) play important roles as light-harvesting and photoprotective pigments, as they do in the chloroplasts of higher plants (9, 10). In Rb. sphaeroides Ͼ95% of the photons absorbed by the Cars are transferred as excitation energy to the reaction center; in the strain 7050 of Rps. acidophila, which is the strain used in this report, the corresponding number is Ϸ70% (9, 11, 12). In the subunits of the B800-B850 complex of Rps. acidophila there is one Car (rhodopin glucoside) molecule per two bacteriochlorophyll (BChl) molecules in the B850 ring and one BChl in the B800 ring (1). Nine of these subunits comprise the LH2 ring, B800-B850 complex, of Rps. acidophila. Spectroscopic and biochemical reports suggest that the structures of the B800-B820 complex of Rps. acidophila and LH2 of Rb. sphaeroides (with the Car spheroidene) are similar (13,14).Despite intensive investigation of the underlying me...