Charge separation is an essential step in the conversion of solar energy into chemical energy in photosynthesis. To investigate this process, we performed transient absorption experiments at 77 K with various excitation conditions on the isolated Photosystem II reaction center preparations from spinach. The results have been analyzed by global and target analysis and demonstrate that at least two different excited states, (Chl D1 Phe D1 )* and (P D1 P D2 Chl D1 )*, give rise to two different pathways for ultrafast charge separation. We propose that the disorder produced by slow protein motions causes energetic differentiation among reaction center complexes, leading to different charge separation pathways. Because of the low temperature, two excitation energy trap states are also present, generating charge-separated states on long time scales. We conclude that these slow trap states are the same as the excited states that lead to ultrafast charge separation, indicating that at 77 K charge separation can be either activation-less and fast or activated and slow.Charge separation is one of the key processes in photosynthetic energy conversion. After absorption of a photon by the photochemically active reaction center, an electronically excited state is transformed into a short-lived charge-separated state. Subsequent electron transfer results in a stable charge-separated state which ultimately powers the photosynthetic organism.Type II reaction centers found in purple bacteria and in oxygenevolving organisms (cyanobacteria, algae, and higher plants) are membrane proteins that contain four (bacterio)chlorophyll [(B)Chl] 1 and two (bacterio)pheophytin [(B)Phe] molecules arranged in two symmetric branches spanning the membrane in the center of the complex. It is established that only one branch is active in charge separation (1-4).The best understanding of the kinetics and energetics of charge separation has been obtained for the reaction center (RC) of photosynthetic purple bacteria (5). The central excitonically coupled special pair, P, of BChl molecules [P A and P B , ∼8 Å apart, center to center (6)], absorbing at ∼875 nm in Rhodobacter sphaeroides, are electronically excited after the energy transfer from the LH1 core antenna (absorbing at approximately equal energy). Then, an electron is transferred to the BChl molecule on the active branch (B A ) in 3 ps, and from B A to the BPhe (H A ) in 1 ps, resulting in the final charge-separated state, P þ H A -. However, in isolated reaction centers, excitation of the accessory BChl absorbing at ∼800 nm (B A ) resulted in an even faster charge separation, either via B A þ H A -or via P þ B A -(7-9). In vivo, this second route does not occur to a significant extent, because B A is too high in energy to receive excitation energy from the antenna.In the photosystem II reaction center (PSII RC) of oxygenevolving organisms, there is no special pair, and the similar distance of ∼10-11 Å between neighboring pigments in the center of the complex (10-13) gives rise to a...