Long-lived charge-separated states in bacterial reaction centers isolated from Rhodobacter sphaeroides

We studied the accumulation of long-lived charge-separated states in reaction centers isolated from Rhodobacter sphaeroides, using continuous illumination, or trains of single-turnover flashes. We found that under both conditions a long-lived state was produced with a quantum yield of about 1%. This long-lived species resembles the normal P(+)Q(-) state in all respects, but has a lifetime of several minutes. Under continuous illumination the long-lived state can be accumulated, leading to close to full conversion of the reaction centers into this state. The lifetime of this accumulated state varies from a few minutes up to more than 20 min, and depends on the illumination history. Surprisingly, the lifetime and quantum yield do not depend on the presence of the secondary quinone, Q(B). Under oxygen-free conditions the accumulation was reversible, no changes in the normal recombination times were observed due to the intense illumination. The long-lived state is responsible for most of the dark adaptation and hysteresis effects observed in room temperature experiments. A simple method for quinone extraction and reconstitution was developed.     

Manganese oxidation by modified reaction centers from Rhodobacter sphaeroides

The transfer of an electron from exogenous manganese (II) ions to the bacteriochlorophyll dimer, P, of bacterial reaction centers was characterized for a series of mutants that have P/P(+) midpoint potentials ranging from 585 to 765 mV compared to 505 mV for wild type. Light-induced changes in optical and EPR spectra of the mutants were measured to monitor the disappearance of the oxidized dimer upon electron donation by manganese in the presence of bicarbonate. The extent of electron transfer was strongly dependent upon the P/P(+) midpoint potential. The midpoint potential of the Mn(2+)/Mn(3+) couple was calculated to decrease linearly from 751 to 623 mV as the pH was raised from 8 to 10, indicating the involvement of a proton. The electron donation had a second order rate constant of approximately 9 x 10(4) M(-1) s(-1), determined from the linear increase in rate for Mn(2+) concentrations up to 200 microM. Weak dissociation constants of 100-200 microM were found. Quantitative EPR analysis of the six-line free Mn(2+) signal revealed that up to seven manganese ions were associated with the reaction centers at a 1 mM concentration of manganese. The association and the electron transfer between manganese and the reaction centers could be inhibited by Ca(2+) and Na(+) ions. The ability of reaction centers with high potentials to oxidize manganese suggests that manganese oxidation could have preceded water oxidation in the evolutionary development of photosystem II.     

Cu2+ site in photosynthetic bacterial reaction centers from Rhodobacter sphaeroides, Rhodobacter capsulatus, and Rhodopseudomonas viridis

The interaction of metal ions with isolated photosynthetic reaction centers (RCs) from the purple bacteria Rhodobacter sphaeroides, Rhodobacter capsulatus, and Rhodopseudomonas viridis has been investigated with transient optical and magnetic resonance techniques. In RCs from all species, the electrochromic response of the bacteriopheophytin cofactors associated with Q(A)(-)Q(B) --> Q(A)Q(B)(-) electron transfer is slowed in the presence of Cu(2+). This slowing is similar to the metal ion effect observed for RCs from Rb. sphaeroides where Zn(2+) was bound to a specific site on the surface of the RC [Utschig et al. (1998) Biochemistry 37, 8278]. The coordination environments of the Cu(2+) sites were probed with electron paramagnetic resonance (EPR) spectroscopy, providing the first direct spectroscopic evidence for the existence of a second metal site in RCs from Rb. capsulatus and Rps. viridis. In the dark, RCs with Cu(2+) bound to the surface exhibit axially symmetric EPR spectra. Electron spin echo envelope modulation (ESEEM) spectral results indicate multiple weakly hyperfine coupled (14)N nuclei in close proximity to Cu(2+). These ESEEM spectra resemble those observed for Cu(2+) RCs from Rb. sphaeroides [Utschig et al. (2000) Biochemistry 39, 2961] and indicate that two or more histidines ligate the Cu(2+) at the surface site in each RC. Thus, RCs from Rb. sphaeroides, Rb. capsulatus, and Rps. viridis each have a structurally analogous Cu(2+) binding site that is involved in modulating the Q(A)(-)Q(B) --> Q(A)Q(B)(-) electron-transfer process. Inspection of the Rps. viridis crystal structure reveals four potential histidine ligands from three different subunits (M16, H178, H72, and L211) located beneath the Q(B) binding pocket. The location of these histidines is surprisingly similar to the grouping of four histidine residues (H68, H126, H128, and L211) observed in the Rb. sphaeroides RC crystal structure. Further elucidation of these Cu(2+) sites will provide a means to investigate localized proton entry into the RCs of Rb. capsulatus and Rps. viridis as well as locate a site of protein motions coupled with electron transfer.     

Trapped tyrosyl radical populations in modified reaction centers from Rhodobacter sphaeroides

The photosynthetic reaction center from the purple bacterium Rhodobacter sphaeroides has been modified such that the bacteriochlorophyll dimer, when it becomes oxidized after light excitation, is capable of oxidizing tyrosine residues. One factor in this ability is a high oxidation-reduction midpoint potential for the dimer, although the location and protein environment of the tyrosine residue appear to be critical as well. These factors were tested in a series of mutants, each of which contains changes, at residues L131, M160, M197, and M210, that give rise to a bacteriochlorophyll dimer with a midpoint potential of at least 800 mV. The protein environment was altered near tyrosine residues that are either present in the wild type or introduced by mutagenesis, focusing on residues that could act as acceptors for the phenolic proton of the tyrosine upon oxidation. These mutations include Ser M190 to His, which is near Tyr L162, the combination of His M193 to Tyr and Arg M164 to His, which adds a Tyr-His pair, and the combinations of Arg L135 to Tyr with Tyr L164 to His, Arg L135 to Tyr with Tyr L144 to Glu, and Arg L135 to Tyr with Tyr L164 to Phe. Radicals were produced in the mutants by using light to initiate electron transfer. The radicals were trapped by freezing the samples, and the relative populations of the oxidized dimer and tyrosyl radicals were determined by analysis of low-temperature electron paramagnetic resonance spectra. The mutants all showed evidence of tyrosyl radical formation at high pH, and the extent of radical formation at Tyr L135 with pH differed depending on the identity of L144 and L164. The results show that tyrosine residues within approximately 10 A of the dimer can become oxidized when provided with a suitable protein environment.     

Effects of mutations near the bacteriochlorophylls in reaction centers from Rhodobacter sphaeroides.

Mutations were made in four residues near the bacteriochlorophyll cofactors of the photosynthetic reaction center from Rhodobacter sphaeroides. These mutations, L131 Leu to His and M160 Leu to His, near the dimer bacteriochlorophylls, and M203 Gly to Asp and L177 Ile to Asp, near the monomer bacteriochlorophylls, were designed to result in the placement of a hydrogen bond donor group near the ring V keto carbonyl of each bacteriochlorophyll. Perturbations of the electronic structures of the bacteriochlorophylls in the mutants are indicated by additional resolved transitions in the bacteriochlorophyll absorption bands in steady-state low-temperature and time-resolved room temperature spectra in three of the resulting mutant reaction centers. The major effect of the two mutations near the dimer was an increase up to 80 mV in the donor oxidation-reduction midpoint potential. Correspondingly, the calculated free energy difference between the excited state of the primary donor and the initial charge separated state decreased by up to 55 mV, the initial forward electron-transfer rate was up to 4 times slower, and the rate of charge recombination between the primary quinone and the donor was approximately 30% faster in these two mutants compared to the wild type. The two mutations near the monomer bacteriochlorophylls had minor changes of 25 mV or less in the donor oxidation-reduction potential, but the mutation close to the monomer bacteriochlorophyll on the active branch resulted in a roughly 3-fold decrease in the rate of the initial electron transfer.     

Proton release upon oxidation of tyrosine in reaction centers from Rhodobacter sphaeroides

Markedly different light-induced protonational changes were measured in two reaction center mutants of Rhodobacter sphaeroides. A quadruple mutant containing alterations, at residues L131, M160, M197, and M210, that elevate the midpoint potential of the bacteriochlorophyll dimer was compared to the Y(M) mutant, which contains these alterations plus a tyrosine at M164 serving as a secondary electron donor [Kálmán et al., Nature 402 (1999) 696]. In the quadruple mutant, a proton uptake of 0.1-0.3 H(+)/reaction center between pH 6 and 10 resulted from formation of the oxidized bacteriochlorophyll donor and reduced primary quinone. In the Y(M) mutant, a maximal proton release of -0.5 H(+)/reaction center at pH 8 was attributed to formation of the tyrosyl radical and modeled using electrostatic and direct proton-releasing mechanisms.     

Pressure effects on the photochemistry of bacterial photosynthetic reaction centers from Rhodobacter sphaeroides R-26 and Rhodopseudomonas viridis

Electron-transfer reactions and triplet decay rates have been studied at pressures up to 300 MPa. In reaction centers from Rhodobacter sphaeroides R-26, high pressure hastened the electron transfers from both the primary and secondary quinones (Q_A and Q_B) to the primary electron donor bacteriochlorophyll, P. Motion of Q_A between two sites, one nearer to P and the other nearer to Q_B, could account for these pressure effects. In reaction centers from Rhodopseudomonas viridis, charge recombination was slowed by high pressure. Decay rates were also studied for the triplet state, P^R. In Rb. sphaeroides R-26 with Q_A reduced with Na₂S₂O₄, the decay was hastened by pressure. This could be explained if P^R decays through a charge-transfer triplet state, or if the decay kinetics of P^R are sensitive to the distance between P and Q_A⁻. In Rps. viridis reaction centers, and in Rb. sphaeroides reaction centers that were depleted of Q_A, the lifetime of P^R was not altered by pressure.     

Inhibition and labelling of isolated reaction centers from Rhodobacter sphaeroides by dicyclohexylcarbodiimide

The effect of dicyclohexylcarbodiimide (DCCD) on electron transfer in the acceptor quinone complex of reaction centers (RC) from Rhodobacter sphaeroides is reported. DCCD covalently labelled the RC over a wide concentration range. At low concentrations (<10 M) the binding was specific for the L subunit. At relatively high concentrations (>100 M) DCCD accelerated the rate of charge recombination of the P⁺Q_B ^- state, consistent with a decrease in the equilibrium constant between Q_A ^-Q_B and Q_AQ_B ^-. At similar concentrations, in the presence of cytochrome c as exogenous donor, turnover of the RC was inhibited such that only three cytochromes were oxidized in a train of flashes. Both these inhibitory effects were fully reversed by dialysis, indicating that stable covalent binding was not involved. Possible mechanisms of action are discussed in terms of the putative role of specific residues in proton transfer and protonation and release of quinol from the RC.     

A picosecond circular dichroism study of photosynthetic reaction centers from Rhodobacter sphaeroides

Picosecond transient circular dichroism spectra are reported for the primary intermediates in the photocycle of reaction centers isolated from Rhodobacter sphaeroides. The time-resolved circular dichroism spectra of the two electron transfer intermediates (BChl2) +BPh-LQA and (BChl2) +BPhLQ-A reveal a large, nonconservative, and fairly stationary CD band at 800 nm. These results suggests that mechanisms other than exciton interactions need to be included in order to explain the optical activity of this biological system.     

Characterization of a semi-stable,charge-separated state in reaction centers from Rhodobacter sphaeroides

In reaction centers from Rhodobacter sphaeroides, subjected to continuous illumination in the presence of an inhibitor of the Q_A to Q_B electron transfer, the oxidation of P870 consisted of several kinetic phases with a fast initial reaction followed by very slow accumulation of P870⁺ with a halftime of several minutes. When the light was turned off, a phase of fast charge recombination was followed by an equally slow reduction of P870⁺. In reaction centers depleted of Q_B, where forward electron transfer from Q_A is also prevented, the slow reactions were also observed but with different kinetic properties. The kinetic traces of accumulation and decay of P870⁺ could be fitted to a simple three-state model where the initial, fast charge separation is followed by a slow reversible conversion to a long-lived, charge-stabilized state. Spectroscopic examination of the charge-separated, semi-stable state, using optical absorbance and EPR spectroscopy, suggests that the unpaired electron on the acceptor side is located in an environment significantly different from normal. The activation parameters and enthalpy and entropy changes, determined from the temperature dependence of the slow conversion reaction, suggest that this might be coupled to changes in the protein structure of the reaction centers, supporting the spectroscopic results. One model that is consistent with the present observations is that reaction centers, after the primary charge separation, undergo a slow, light-induced change in conformation affecting the acceptor side. This revised version was published online in June 2006 with corrections to the Cover Date.     

Implications of spin dynamics for the charge recombination in iron-depleted and quinone-substituted reaction centers from Rhodobacter sphaeroides R-26

Detailed calculations on the spin-dependent recombination dynamics are presented for reaction centers of Rhodobacter sphaeroides R-26 in which electron transfer from the primary radical pair to the iron-quinone acceptor complex has been slowed down by either iron depletion or replacement of the native ubiquinone by other quinones with different midpoint potential. Recombination yields reported for iron-depleted samples (Kirmaier, C., Holten, D., Debus, R.J., Feher, G. and Okamura, M.Y. (1986) Proc. Natl. Acad. Sci. USA 83, in the press) are compared to those in quinone-depleted reaction centers, where the forward electron transfer is completely blocked by extraction of the quinone. Within the scatter of the experimental data, the recombination pattern appears to be similar in the two different preparations indicating that the structural and kinetic features of the recombining radical pair state are not seriously affected by removal of the iron.     

High-order derivative spectroscopy of infrared absorption spectra of the reaction centers from Rhodobacter sphaeroides

The infrared absorption spectra of reduced and chemically oxidized reaction center preparations from the purple bacterium Rhodobacter sphaeroides were investigated by means of high-order derivative spectroscopy. The model Gaussian band with a maximum at 810 nm and a half-band of 15 nm found in the absorption spectrum of the reduced reaction center preparation is eliminated after the oxidation of photoactive bacteriochlorophyll dimer (P). This band was related to the absorption of the P(+)y excitonic band of P. On the basis of experimental results, it was concluded that the bleaching of the P(+)y absorption band at 810 nm in the oxidized reaction center preparations gives the main contribution to the blue shift of the 800 nm absorption band of Rb. sphaeroides reaction centers.     

Replacement of bacteriopheophytin in reaction centers from Rhodobacter sphaeroides RS601 with plant pheophytin

In the presence of acetone and an excess of exogenous plant pheophytins,bacteriopheophytins in the reaction centers from Rhodobacter sphaeroides RS601 were replaced by pheophytins at sites HA and HB,when incubated at 43.5℃ for more than 15 min.The substitution of bacteriopheophytins in the reaction centers was 50% and 71% with incubation of 15 and 60 min,respectively.In the absorption spectra of pheophytin-replaced reaction centers (Phe RCs),bands assigned to the transition moments QX (537 nm) and QY (758 nm) of bacteriopheophytin disappeared,and three distinct bands assigned to the transition moments QX (509/542 nm) and QY (674 nm) of pheophytin appeared instead.Compared to that of the control reaction centers,the photochemical activities of Phe RCs are 78% and 71% of control,with the incubation time of 15 and 60 min.Differences might exist between the redox properties of Phe RC and of native reaction centers,but the substitution is significant,and the new system is available for further studies.     

Energetics of proton transfer pathways in reaction centers from Rhodobacter sphaeroides. The Glu-H173 activated mutants

Electron transfer between the primary and secondary quinones (Q(A), Q(B)) in the bacterial photosynthetic reaction center (bRC) is coupled with proton uptake at Q(B). The protons are conducted from the cytoplasmic side, probably with the participation of two water channels. Mutations of titratable residues like Asp-L213 to Asn (inhibited mutant) or the double mutant Glu-L212 to Ala/Asp-L213 to Ala inhibit these electron transfer-coupled proton uptake events. The inhibition of the proton transfer (PT) process in the single mutant can be restored by a second mutation of Arg-M233 to Cys or Arg-H177 to His (revertant mutant). These revertant mutants shed light on the location of the main proton transfer pathway of wild type bRC. In contrast to the wild type and inhibited mutant bRC, the revertant mutant bRC showed notable proton uptake at Glu-H173 upon formation of the Q(B)- state. In all of these mutants, the pK(a) of Asp-M17 decreased by 1.4-2.4 units with respect to the wild type bRC, whereas a significant pK(a) upshift of up to 5.8 units was observed at Glu-H122, Asp-H170, Glu-H173, and Glu-H230 in the revertant mutants. These residues belonging to the main PT pathway are arranged along water channel P1 localized mainly in subunit H. bRC possesses subunit H, which has no counterpart in photosystem II. Thus, bRC may possess alternative PT pathways involving water channels in subunit H, which becomes active in case the main PT pathway is blocked.     

Electron transfer in reaction centers of Rhodobacter sphaeroides and Rhodobacter capsulatus monitored by fluorescence of the bacteriochlorophyll dimer

Spectral and kinetic characteristics of fluorescence from isolated reaction centers of photosynthetic purple bacteria Rhodobacter sphaeroides and Rhodobacter capsulatus were measured at room temperature under rectangular shape of excitation at 810 nm. The kinetics of fluorescence at 915 nm reflected redox changes due to light and dark reactions in the donor and acceptor quinone complex of the reaction center as identified by absorption changes at 865 nm (bacteriochlorophyll dimer) and 450 nm (quinones) measured simultaneously with the fluorescence. Based on redox titration and gradual bleaching of the dimer, the yield of fluorescence from reaction centers could be separated into a time-dependent (originating from the dimer) and a constant part (coming from contaminating pigment (detached bacteriochlorin)). The origin was also confirmed by the corresponding excitation spectra of the 915 nm fluorescence. The ratio of yields of constant fluorescence over variable fluorescence was much smaller in Rhodobacter sphaeroides (0.15±0.1) than in Rhodobacter capsulatus (1.2±0.3). It was shown that the changes in fluorescence yield reflected the disappearance of the dimer and the quenching by the oxidized primary quinone. The redox changes of the secondary quinone did not have any influence on the yield but excess quinone in the solution quenched the (constant part of) fluorescence. The relative yields of fluorescence in different redox states of the reaction center were tabulated. The fluorescence of the dimer can be used as an effective tool in studies of redox reactions in reaction centers, an alternative to the measurements of absorption kinetics.Abbreviations Bchl bacteriochlorophyll - Bpheo bacteriopheophytin - D electron donor to P⁺ - P bacteriochlorophyll dimer - Q quinone acceptor - Q_A primary quinone acceptor - Q_B secondary quinone acceptor - RC reaction center protein - UQ₆ ubiquinone-30     

Coupling of collective motions of the protein matrix to vibrations of the non-heme iron in bacterial photosynthetic reaction centers

Non-heme iron is a conservative component of type II photosynthetic reaction centers of unknown function. We found that in the reaction center from Rba. sphaeroides it exists in two forms, high and low spin ferrous states, whereas in Rsp. rubrum mostly in a low spin state, in line with our earlier finding of its low spin state in the algal photosystem II reaction center (Burda et al., 2003). The temperature dependence of the non-heme iron displacement studied by Mössbauer spectroscopy shows that the surrounding of the high spin iron is more flexible (Debye temperature ~ 165 K) than that of the low spin atom (~ 207 K). Nuclear inelastic scattering measurements of the collective motions in the Rba. sphaeroides reaction center show that the density of vibrational states, originating from non-heme iron, has well-separated modes between lower (4-17 meV) and higher (17-25 meV) energies while in the one from Rsp. rubrum its distribution is more uniform with only little contribution of low energy (~ 6 meV) vibrations. It is the first experimental evidence that the fluctuations of the protein matrix in type II reaction center are correlated to the spin state of non-heme iron. We propose a simple mechanism in which the spin state of non-heme iron directly determines the strength of coupling between the two quinone acceptors (Q_A and Q_B) and fast collective motions of protein matrix that play a crucial role in activation and regulation of the electron and proton transfer between these two quinones. We suggest that hydrogen bond network on the acceptor side of reaction center is responsible for stabilization of non-heme iron in different spin states.     

B-branch electron transfer in reaction centers of Rhodobacter sphaeroides assessed with site-directed mutagenesis

Mutants of Rhodobacter (Rba.) sphaeroides are described which were designed to study electron transfer along the so-called B-branch of reaction center (RC) cofactors. Combining the mutation L(M214)H, which results in the incorporation of a bacteriochlorophyll, β, for H_A [Kirmaier et al. (1991) Science 251: 922–927] with two mutations, G(M203)D and Y(M210)W, near B_A, we have created a double and a triple mutant with long lifetimes of the excited state P^* of the primary donor P, viz. 80 and 160 ps at room temperature, respectively. The yield of P⁺Q_A ⁻ formation in these mutants is reduced to 50 and 30%, respectively, of that in wildtype RCs. For both mutants, the quantum yield of P⁺H_B ⁻ formation was less than 10%, in contrast to the 15% B-branch electron transfer demonstrated in RCs of a similar mutant of Rba. capsulatus with a P^* lifetime of 15 ps [Heller et al. (1995) Science 269: 940–945]. We conclude that the lifetime of P^* is not a governing factor in switching to B-branch electron transfer. The direct photoreduction of the secondary quinone, Q_B, was studied with a triple mutant combining the G(M203)D, L(M214)H and A(M260)W mutations. In this triple mutant Q_A does not bind to the reaction center [Ridge et al. (1999) Photosynth Res 59: 9–26]. It is shown that B-branch electron transfer leading to P⁺Q_B ⁻ formation occurs to a minor extent at both room temperature and at cryogenic temperatures (about 3% following a saturating laser flash at 20 K). In contrast, in wildtype RCs P⁺Q_B ⁻ formation involves the A-branch and does not occur at all at cryogenic temperatures. Attempts to accumulate the P⁺Q_B ⁻ state under continuous illumination were not successful. Charge recombination of P⁺Q_B ⁻ formed by B-branch electron transfer in the new mutant is much faster (seconds) than has been previously reported for charge recombination of P⁺Q_B ⁻ trapped in wildtype RCs (10⁵ s) [Kleinfeld et al. (1984b) Biochemistry 23: 5780–5786]. This difference is discussed in light of the different binding sites for Q_B and Q_B ⁻ that recently have been found by X-ray crystallography at cryogenic temperatures [Stowell et al. (1997) Science 276: 812–816]. We present the first low-temperature absorption difference spectrum due to P⁺Q_B ⁻. This revised version was published online in June 2006 with corrections to the Cover Date.     

Energetics of quinone-dependent electron and proton transfers in Rhodobacter sphaeroides photosynthetic reaction centers

Proteins bind redox cofactors, modifying their electrochemistry and affinity by specific interactions of the binding site with each cofactor redox state. Photosynthetic reaction centers from Rhodobacter sphaeroides have three ubiquinone-binding sites, Q(A), and proximal and distal Q(B) sites. Ubiquinones, which can be doubly reduced and bind 2 protons, have 9 redox states. However, only Q and Q(-) are seen in the Q(A) site and Q, Q(-), and QH(2) in the proximal Q(B) site. The distal Q(B) function is uncertain. Multiple conformation continuum electrostatics (MCCE) was used to compare the ubiquinone electrochemical midpoints (E(m)) and pK(a) values at these three sites. At pH 7, the Q(A)/Q(A)(-) E(m) is -40 mV and proximal Q(B)/Q(B)(-) -10 mV in agreement with the experimental values (assuming a solution ubiquinone E(m) of -145 mV). Q(B) reduction requires changes in nearby residue protonation and SerL223 reorientation. The distal Q(B)/Q(B)(-) E(m) is a much more unfavorable -260 mV. Q(A) and proximal Q(B) sites generally stabilize species with a -1 charge, while the distal Q(B) site prefers binding neutral species. In each site, the dianion is destabilized because favorable interactions with the residues and backbone increase with charge (q), while the unfavorable loss of solvation energy increases with q(2). Therefore, proton binding before a second reduction, forming QH and then QH(-), is always preferred to forming the dianion (Q(-)(2)). The final product QH(2) is higher in energy at the proximal Q(B) site than in solution; therefore, it binds poorly, favoring release. In contrast, QH(2) binds more tightly than Q at the distal Q(B) site.     

Identification of the first steps in charge separation in bacterial photosynthetic reaction centers of Rhodobacter sphaeroides by ultrafast mid-infrared spectroscopy: electron transfer and protein dynamics

Time-resolved visible pump/mid-infrared (mid-IR) probe spectroscopy in the region between 1600 and 1800 cm⁻¹ was used to investigate electron transfer, radical pair relaxation, and protein relaxation at room temperature in the Rhodobacter sphaeroides reaction center (RC). Wild-type RCs both with and without the quinone electron acceptor Q_A, were excited at 600 nm (nonselective excitation), 800 nm (direct excitation of the monomeric bacteriochlorophyll (BChl) cofactors), and 860 nm (direct excitation of the dimer of primary donor (P) BChls (P_L/P_M)). The region between 1600 and 1800 cm⁻¹ encompasses absorption changes associated with carbonyl (CO) stretch vibrational modes of the cofactors and protein. After photoexcitation of the RC the primary electron donor P excited singlet state (P*) decayed on a timescale of 3.7 ps to the state (where B_L is the accessory BChl electron acceptor). This is the first report of the mid-IR absorption spectrum of ; the difference spectrum indicates that the 9-keto CO stretch of B_L is located around 1670-1680 cm⁻¹. After subsequent electron transfer to the bacteriopheophytin H_L in ∼1 ps, the state was formed. A sequential analysis and simultaneous target analysis of the data showed a relaxation of the radical pair on the ∼20 ps timescale, accompanied by a change in the relative ratio of the and bands and by a minor change in the band amplitude at 1640 cm⁻¹ that may be tentatively ascribed to the response of an amide CO to the radical pair formation. We conclude that the drop in free energy associated with the relaxation of , is due to an increased localization of the electron hole on the P_L half of the dimer and a further consequence is a reduction in the electrical field causing the Stark shift of one or more amide CO oscillators.