In photosystem II of green plants the key photosynthetic reaction consists of the transfer of an electron from the primary donor called P680 to a nearby pheophytin molecule. We analyzed the temperature dependence of this reaction by subpicosecond transient absorption spectroscopy over the temperature range 20-240 K using isolated photosystem II reaction centers from spinach. After excitation in the red edge of the Q y absorption band, the decay of the excited state can conveniently be described by two kinetic components that both accelerate with temperature. This temperature behavior differs remarkably from that observed in purple bacterial reaction centers. We attribute the first component, which accelerates from 2.6 ps at 20 K to 0.4 ps at 240 K, to charge separation after direct excitation of P680, and explain its temperature dependence by an intermediate that lies in energy above the singlet-excited P680 and that possibly has charge-transfer character. The second component accelerates from 120 ps at 20 K to 18 ps at 240 K and is attributed to charge separation after direct excitation of the ''trap'' state near-degenerate with P680 and subsequent slow energy transfer from this trap state to P680. We suggest that the slow energy transfer from the trap state to P680 plays an important role in the kinetics of radical pair formation at room temperature.The photochemical reaction center (RC) of photosystem II (PSII) (the D1-D2 cyt.b559 complex) is the smallest unit in PSII that shows photochemical activity. The RC contains six chlorophyll (Chl) a and two pheophytin (Pheo) a molecules (1-4) that all have their lowest electronic transition around 675 nm, as well as two -carotenes. The D1 and D2 polypeptides are homologous to the L and M subunits of bacterial RCs, suggesting an arrangement of the core pigments in the RC of PSII similar to that in the bacterial RC (5). The two additional Chl molecules are probably located near the periphery of the D1-D2 complex.The characterization of energy transfer and charge separation in the PSII RC is less well established than is the case for the bacterial RC (for a review, see ref. 6). This may be due to the fact that the first PSII RC was isolated only in 1987 (7) and that there is no structure available. However, the excited state kinetics of the PSII RC are also inherently more complicated than those of bacterial RCs. The primary electron donor in PSII, called P680, is isoenergetic with some of the other pigments in the RC (8-13) and as a consequence forms only a very shallow trap for excitations.After excitation of P680 an electron is transferred to the photoactive Pheo molecule (6). In isolated PSII RC preparations, further electron transport cannot occur, because the quinone acceptors are lost during the isolation procedure. A straightforward interpretation of the results from pump-probe measurements in terms of pigment to pigment energy transfer and charge separation rates has proven difficult, mainly due to the congested absorption spectrum of the PSII RC. At r...