ENDOR spectroscopy reveals light induced movement of the H-bond from Ser-L223 upon forming the semiquinone (Q(B)(-)(*)) in reaction centers from Rhodobacter sphaeroides

Proton ENDOR spectroscopy was used to monitor local conformational changes in bacterial reaction centers (RC) associated with the electron-transfer reaction DQB --> D+*QB-* using mutant RCs capable of photoreducing QB at cryogenic temperatures. The charge separated state D+*QB-* was studied in mutant RCs formed by either (i) illuminating at low temperature (77 K) a sample frozen in the dark (ground state protein conformation) or (ii) illuminating at room temperature prior to and during freezing (charge separated state protein conformation). The charge recombination rates from the two states differed greatly (>10(6) fold) as shown previously, indicating a structural change (Paddock et al. (2006) Biochemistry 45, 14032-14042). ENDOR spectra of QB-* from both samples (35 GHz, 77 K) showed several H-bond hyperfine couplings that were similar to those for QB-* in native RCs indicating that in all RCs, QB-* was located at the proximal position near the metal site. In contrast, one set of hyperfine couplings were not observed in the dark frozen samples but were observed only in samples frozen under illumination in which the protein can relax prior to freezing. This flexible H-bond was assigned to an interaction between the Ser-L223 hydroxyl and QB-* on the basis of its absence in Ser L223 --> Ala mutant RCs. Thus, part of the protein relaxation, in response to light induced charge separation, involves the formation of an H-bond between the OH group of Ser-L223 and the anionic semiquinone QB-*. These results show the flexibility of the Ser-L223 H-bond, which is essential for its function in proton transfer to reduced QB.     

Resonance Raman characterization of Rhodobacter sphaeroides reaction centers bearing site-directed mutations at tyrosine M210

Resonance Raman (RR) spectroscopy and low-temperature absorption spectroscopy have been used to investigate the structural changes in the reaction centers (RCs) of Rhodobacter sphaeroides induced by site-specific mutations on the tyrosine (Y) M210 residue. RCs in which Y M210 has been genetically replaced with phenylalanine (F) or leucine (L) exhibit a 5-fold decrease in their primary electron-transfer kinetics (Finkele et al., 1990). The general similarity of RR spectra of the wild-type RCs as compared to those of the two mutant RCs indicates that no significant global structural changes occur upon mutation at the level of any of the six bacteriochlorin pigments. In the RR spectra of the two mutant RCs there is a conspicuous absence of contributions from the BPheM prosthetic group, which is interpreted in terms of a change in the resonance enhancement conditions of this chromophore. Low-temperature adsorption spectroscopy reveals marked shifts in the Qx absorption band of BPheM. This shift is interpreted as arising from a destabilization of the protein in the vicinity of BPheM and accounts for the change in resonance condition for this chromophore in its RR contributions. As well, there is a 3-nm red shift of the Qy absorption band of the BChls from 803 to 806 nm for the mutant RCs. Difference RR spectra yielding structural information concerning, selectively, the primary donor (P) indicate that the structure of the P binding pocket is conserved for these mutant RCs. The tyrosine M210 is not observed to be engaged in a hydrogen bond with either of the acetyl or keto carbonyls of P.     

Trapping conformational intermediate states in the reaction center protein from photosynthetic bacteria

In protein, conformational changes are often crucial for function but not easy to observe. Two functionally relevant conformational intermediate states of photosynthetic reaction center protein (RCs) are trapped and characterized at low temperature. RCs frozen in the dark do not allow electron transfer from the reduced primary quinone, Q(A)(-), to the secondary quinone, Q(B). In contrast, RCs frozen under illumination in the product (P(+)Q(A)Q(B)(-)) state, with the oxidized electron donor, P(+), and reduced Q(B)(-), return to the ground state at cryogenic temperature in a conformation that allows a high yield of Q(B) reduction. Thus, RCs frozen under illumination are found to be trapped above the ground state in a conformation that allows product formation. When the temperature is raised above 120 K, the protein relaxes to an inactive conformation which is different from the RCs frozen in the dark. The activation energy for this change is 87 +/- 8 meV, and the active and inactive states differ in energy by only 16 +/- 3 meV. Thus, there are several conformational substates along the reaction coordinate with different transition temperatures. The ground state spectra of the RCs in active and inactive conformations report differences in the intraprotein electrostatic field, demonstrating that the dipole or charge distribution has changed. In addition, the electrochromic shift associated with the Q(A)(-) to Q(B) electron transfer at low temperature was characterized. The electron-transfer rate from Q(B)(-) to P(+) was measured at cryogenic temperature and is similar to the rate at room temperature, as expected for an exothermic, electron tunneling reaction in RCs.     

Possible effect of structural phase transition in the reactive center of Rhodobacter sphaeroides on the rate of dark adaptation of photooxidized bacteriochlorophyll from primary quinone

The dependence of the rate of dark recombination between the photooxidized primary donor--dimer bacteriochlorophyll molecule (P) and reduced primary quinone acceptor (QA), P+QA(-)-->PQA was studied in photosynthetic reaction centers (RC) from Rhodobacter sphaeroides in the temperature range of 100-320 K. Control RC preparations, RC species with the removed H-subunit as well as RC samples with the hydrogen bonds network modified by isotopic D2O-H2O substitution were investigated. An anomalous temperature dependence of the recombination time (tau rec) of dark reaction P+QA(-)-->PQA was found for all RC samples. It was found that upon heating from 120 to 290 K tau rec increased 2.5 fold. However, upon further heating to 320 K, tau rec decreased again. The temperature dependences of the P+QA(-)-->PQA recombination time were compared with those of the thermodepolarization current of RC preparations in the same temperature range. The temperature curve of the thermodepolarization current was also nonmonotonous. The theoretical interpretation of the temperature dependence of tau rec as well as of the thermodepolarization current was made in the framework of the theory of structural phase transitions within the hydrogen bond network in the water-protein surrounding of the redox centers participating in the electron transfer reactions.     

Structural microheterogeneity of a tryptophan residue required for efficient biological electron transfer between putidaredoxin and cytochrome P-450cam

The carboxy-terminal tryptophan of putidaredoxin, the Fe2S2.Cys4 iron-sulfur physiological redox partner of cytochrome P-450cam, is essential for maximal biological activity [Davies, M. D., Qin, L., Beck, J. L., Suslick, K. S., Koga, H., Horiuchi, T., & Sligar, S. G. (1990) J. Am. Chem. Soc. 112, 7396-7398]. This single tryptophan-containing protein thus represents an excellent system for studying the solution dynamics of a residue directly implicated in an electron-transfer pathway. Steady-state and time-resolved measurements of the tryptophan fluorescence have been conducted across the emission spectrum as a function of redox state to probe potential structural changes which might be candidates for structural gating phenomena. The steady-state emission spectrum (lambda max = 358 nm) and anisotropy (alpha = 0.04) suggest that Trp-106 is very solvent-exposed and rotating partially free of global protein constraints. The time-resolved fluorescence kinetics for both oxidized and reduced putidaredoxin are fit best with three discrete components of approximately 5, 2, and 0.3 ns. The lifetime components were assigned to physical species with iodide ion quenching experiments, where differential quenching of the longer components was observed (k tau = 2 = 5.9 X 10(8) M-1 s-1, k tau = 5 = 1.3 X 10(8) M-1 s-1). These findings suggest that the multiexponential fluorescence decay results from ground-state conformational microheterogeneity and thus demonstrate that the essential tryptophan exists in at least two distinguishable conformations. Small differences in the relative proportions of the components between redox states were observed but not cleanly resolved.(ABSTRACT TRUNCATED AT 250 WORDS)     

Vibrational coherence in bacterial reaction centers with genetically modified B-branch pigment composition

Femtosecond absorption difference spectroscopy was applied to study the time and spectral evolution of low-temperature (90 K) absorbance changes in isolated reaction centers (RCs) of the HM182L mutant of Rhodobacter (Rb.) sphaeroides. In this mutant, the composition of the B-branch RC cofactors is modified with respect to that of wild-type RCs by replacing the photochemically inactive BB accessory bacteriochlorophyll (BChl) by a photoreducible bacteriopheophytin molecule (referred to as PhiB). We have examined vibrational coherence within the first 400 fs after excitation of the primary electron donor P with 20-fs pulses at 870 nm by studying the kinetics of absorbance changes at 785 nm (PhiB absorption band), 940 nm (P*-stimulated emission), and 1020 nm (BA- absorption band). The results of the femtosecond measurements are compared with those recently reported for native Rb. sphaeroides R-26 RCs containing an intact BB BChl. At delay times longer than approximately 50 fs (maximum at 120 fs), the mutant RCs exhibit a pronounced BChl radical anion (BA-) absorption band at 1020 nm, which is similar to that observed for Rb. sphaeroides R-26 RCs and represents the formation of the intermediate charge-separated state P+ BA-. Femtosecond oscillations are revealed in the kinetics of the absorption development at 1020 nm and of decay of the P*-stimulated emission at 940 nm, with the oscillatory components of both kinetics displaying a generally synchronous behavior. These data are interpreted in terms of coupling of wave packet-like nuclear motions on the potential energy surface of the P* excited state to the primary electron-transfer reaction P*-->P+ BA- in the A-branch of the RC cofactors. At very early delay times (up to 80 fs), the mutant RCs exhibit a weak absorption decrease around 785 nm that is not observed for Rb. sphaeroides R-26 RCs and can be assigned to a transient bleaching of the Qy ground-state absorption band of the PhiB molecule. In the range of 740-795 nm, encompassing the Qy optical transitions of bacteriopheophytins HA, HB, and PhiB, the absorption difference spectra collected for mutant RCs at 30-50 fs resemble the difference spectrum of the P+ PhiB- charge-separated state previously detected for this mutant in the picosecond time domain (E. Katilius, Z. Katiliene, S. Lin, A.K.W. Taguchi, N.W. Woodbury, J. Phys. Chem., B 106 (2002) 1471-1475). The dynamics of bleaching at 785 nm has a non-monotonous character, showing a single peak with a maximum at 40 fs. Based on these observations, the 785-nm bleaching is speculated to reflect reduction of 1% of PhiB in the B-branch within about 40 fs, which is earlier by approximately 80 fs than the reduction process in the A-branch, both being possibly linked to nuclear wave packet motion in the P* state.     

Kinetics of recombination of photoseparated charges in Rhodobacter sphaeroides reaction centers analyzed by relaxation rate constant distribution

We studied the kinetics of dark recombination of charges photoseparated between the bacteriochlorophyll dimer (P) and the quinone acceptors of the photosynthetic reaction centers (RCs) of Rhodobacter sphaeroides. The time of light activation was varied from 1 to 60 s. The relaxation rate constant distribution was computed from experimental kinetic curves of charge recombination, using our original method whereby relaxation curves are approximated by a set of Gaussian-like peaks in the time domain that correspond to different conformational sub-states of RCs. With increasing photoactivation exposure, some peaks shift toward longer relaxation times. A ‘bifurcation’ of the slower peak is observed at exposures of 20–30 s. The phenomenon is interpreted as evidence of a conformational transition induced by separated charges in the RC structure.     

Experimental evidence of dynamic self-organization in the electron transfer system (example of reaction centers of purple bacteria)

The results of an experimental study of nonlinear dynamic processes in the electron transfer system, the reaction centers (RCs) of purple bacteria are presented. A difference was observed in the absorption spectra of RCs exposed to a rising intensity of acting light compared to a descending intensity of acting light. We observed the hysteresis of the RC optical transmission coefficient at =865 nm, with a quasistationary increase and subsequent decrease of the optical excitation level. The kinetics of charge recombination in an RC containing two quinone acceptors revealed a dependence on the prehistory of the RC illumination. The results were interpreted in terms of the existence of a light-induced memory effect in the electron-conformational system and the appearance of bifurcation in the system at critical values of the photoinduced electron flux through the macromolecule.     

Kinetic evidence of microscopic states in protein folding.

Staphylococcal nuclease unfolds at acidic pHs and refolds at neutral pH. Previous kinetic analysis based on both the direct pH jump and the sequential pH jump, from a native condition (pH 7.0) to pHs beyond unfolding transition zones (pH 3.0 and pH 12), and vice versa, supports the mechanism, D3<-->D2<-->D1<-->N0, in which N0 is the native state and D's are the three substates of the denatured form [Chen, H.M., You, J.L., Markin, V.S., & Tsong, T.Y. (1990) J. Mol. Biol. 220, 771-778; Chen, H.M., Markin, V.S., & Tsong, T.Y. (1992) Biochemistry 31, 1483-1491]. Here we show that both the single- and the double-pH jump kinetics of folding and unfolding to the intermediate pHs (3.4-5.0, i.e., in the transition zone), in which both the native and the denatured states coexist, are not compatible with this simple sequential model. At 25 degrees C, log tau 1(-1) (for the D1<-->N0 step) and log tau 2(-1) (for the D2<-->D1 step) vs pH show a square root of-shaped dependence on the final pH, with minimal values (tau 1(-1) of 0.56 s-1 and tau 2(-1) of around pH 3.9. The third relaxation tau 3 (for the D3<-->D2 step, 35 s) was independent of pH in the range 3.4-8.5. The square root of-shaped dependence on pH of log tau 1(-1) and log tau 2(-1) cannot be reproduced by the above but can be accounted for if each of N0, D1, and D2 is composed of many microscopic states in rapid equilibrium.(ABSTRACT TRUNCATED AT 250 WORDS)     

The interaction of quinone and detergent with reaction centers of purple bacteria. I. Slow quinone exchange between reaction center micelles and pure detergent micelles.

The kinetics of light-induced electron transfer in reaction centers (RCs) from the purple photosynthetic bacterium Rhodobacter sphaeroides were studied in the presence of the detergent lauryldimethylamine-N-oxide (LDAO). After the light-induced electron transfer from the primary donor (P) to the acceptor quinone complex, the dark re-reduction of P+ reflects recombination from the reduced acceptor quinones, QA- or QB-. The secondary quinone, QB, which is loosely bound to the RC, determines the rate of this process. Electron transfer to QB slows down the return of the electron to P+, giving rise to a slow phase of the recovery kinetics with time tau P approximately 1 s, whereas charge recombination in RCs lacking QB generates a fast phase with time tau AP approximately 0.1 s. The amount of quinone bound to RC micelles can be reduced by increasing the detergent concentration. The characteristic time of the slow component of P+ dark relaxation, observed at low quinone content per RC micelle (at high detergent concentration), is about 1.2-1.5 s, in sharp contrast to expectations from previous models, according to which the time of the slow component should approach the time of the fast component (about 0.1 s) when the quinone concentration approaches zero. To account for this large discrepancy, a new quantitative approach has been developed to analyze the kinetics of electron transfer in isolated RCs with the following key features: 1) The exchange of quinone between different micelles (RC and detergent micelles) occurs more slowly than electron transfer from QB- to P+; 2) The exchange of quinone between the detergent "phase" and the QB binding site within the same RC micelle is much faster than electron transfer between QA- and P+; 3) The time of the slow component of P+ dark relaxation is determined by (n) > or = 1, the average number of quinones in RC micelles, calculated only for those RC micelles that have at least one quinone per RC (in excess of QA). An analytical function is derived that relates the time of the slow component of P+ relaxation, tau P, and the relative amplitude of the slow phase. This provides a useful means of determining the true equilibrium constant of electron transfer between QA and QB (LAB), and the association equilibrium constant of quinone binding at the QB site (KQ+). We found that LAB = 22 +/- 3 and KQ = 0.6 +/- 0.2 at pH 7.5. The analysis shows that saturation of the QB binding site in detergent-solubilized RCs is difficult to achieve with hydrophobic quinones. This has important implications for the interpretation of apparent dependencies of QB function on environmental parameters (e.g. pH) and on mutational alterations. The model accounts for the effects of detergent and quinone concentration on electron transfer in the acceptor quinone complex, and the conclusions are of general significance for the study of quinone-binding membrane proteins in detergent solutions.     

Iron-sulfur cluster in aconitase. Crystallographic evidence for a three-iron center

Native x-ray diffraction data from single crystals of inactive aconitase from pig heart (Mr 80,000) have been collected on oscillation films to 2.7 A. Analysis shows that significant measurements of the anomalous scattering signal from the Fe-S cluster in the enzyme are available in the film data. The 5.0-A resolution anomalous difference Patterson function contains vectors for one Fe-S cluster (one aconitase molecule) per asymmetric unit in space group P2(1)2(1)2 with a = 173.6, b = 72.0, and c = 72.7 A. At 2.7-A resolution, the vector map is best interpreted by three Fe sites separated from each other by less than 3 A. The single-crystal diffraction data thus confirm the presence of a 3Fe center in the inactive form of aconitase. Furthermore, the data provide crystallographic evidence that 3Fe clusters exhibit structural heterogeneity. The Fe-Fe vectors cannot be interpreted in terms of 4-A distances as observed for the [3Fe-3S] cluster in Azotobacter ferrodoxin (Ghosh, D., O'Donnell, S., Furey, W., Robbins, A. H., and Stout, C. D. (1982) J. Mol. Biol. 158, 73-109). The results are therefore in agreement with a [3Fe-4S] cluster having 2.7-A Fe-Fe distances (Beinert, H., Emptage, M. H., Dreyer, J.-L., Scott, R. A., Hahn, J. E., Hodgson, K. O., and Thomson, A. J. (1983) Proc. Natl. Acad. Sci. U. S. A. 80, 393-396). However, the data do not unambiguously discriminate between this model and other 3Fe clusters having short Fe-Fe distances.     

The effect of an applied electric field on the charge recombination kinetics in reaction centers reconstituted in planar lipid bilayers.

Reaction Centers (RCs) from the photosynthetic bacterium Rhodopseudomonas sphaeroides were incorporated in planar bilayers made from monolayers derived from liposomes reconstituted with purified RCs. The photocurrents associated with the charge recombination process between the reduced primary quinone (QA-) and the oxidized bacteriochlorophyll donor (D+) were measured as a function of voltage (-150 mV less than V less than 150 mV) applied across the bilayer. When QA was the native ubiquinone (UQ) the charge recombination was voltage independent. However, when UQ was replaced by anthraquinone (AQ), the recombination time depended on the applied voltage V according to the relation tau = 8.5 X 10(-3) eV/0.175S. These results were explained by a simple model in which the charge recombination from UQ- proceeds directly to D+ while that from AQ occurs via a thermally activated intermediate state, D+I-QA, where I is the intermediate acceptor. The voltage dependence arises from an electric field induced change in the energy gap, delta G0, between the states D+I-QA and D+IQA-. This model is supported by the measured temperature dependence of the charge recombination time, which for RCs with AQ gave a value of delta G0 = 340 +/- 20 meV. In contrast, delta G0 for RCs with UQ as the primary acceptor, is sufficiently large (approximately 550 meV) so that even in the presence of the field, the direct pathway dominates. The voltage dependence shows that the electron transfer from I- to QA is electrogenic. From a quantitative analysis of the voltage dependence on the recombination rate it was concluded that the component of the distance between I and QA along the normal to the membrane is about one-seventh of the thickness of the membrane. This implies that the electron transfer from I to Q contributes at least one-seventh to the potential generated by the charge separation between D+ and QA-.     

Photooxidation of cytochrome b559 in oxygen-evolving photosystem II.

Cytochrome b559 (cyt b559) is an intrinsic and essential component of the photosystem II (PSII) protein complex, but its function, stoichiometry, and electron-transfer kinetics in the physiological system are not well-defined. In this study, we have used flash-detection optical spectroscopy to measure the kinetics and yields of photooxidation and dark reduction of cyt b559 in untreated, O2-evolving PSII-enriched membranes at room temperature. The dark redox states of cyt b559 and the primary electron acceptor, QA, were determined over the pH range 5.0-8.5. Both the fraction of dark-oxidized cyt b559 and dark-reduced QA increased with increasing acidity. Consistent with these results, an acid-induced drop in pH from 8.5 to 4.9 in a dark-adapted sample caused the oxidation of cyt b559, indicating a shift in the redox state during the dark reequilibration. As expected from the dark redox state of cyt b559, the rate and extent of photooxidation of cyt b559 during continuous illumination decreased toward more acidic pH values. After a single, saturating flash, the rate of photooxidation of cyt b559 was of the same order of magnitude as the rate of S2QA- charge recombination. In untreated PSII samples at pH 8.0 with 42% of cyt b559 oxidized and 15% of QA reduced in the dark, 4.7% of one copy of cyt b559 was photooxidized after one flash with a t1/2 of 540 +/- 90 ms. On the basis of our previous work [Buser, C. A., Thompson, L. K., Diner, B. A., & Brudvig, G. W (1990) Biochemistry 29, 8977] and the data presented here, we conclude that Sn+1, YZ., and P680+ are in redox equilibrium and cyt b559 (and YD) are oxidized via P680+. After a period of illumination sufficient to fully reduce the plastoquinone pool, we also observed the pH-dependent dark reduction of photooxidized cyt b559, where the rate of reduction decreased with decreasing pH and was not observed at pH < 6.4. To determine the direct source of reductant to oxidized cyt b559, we studied the dark reduction of cyt b559 and the reduction of the PQ pool as a function of 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU) concentration. We find that DCMU inhibits the reduction of cyt b559 under conditions where the plastoquinone pool and QA are reduced. We conclude that QB-. (H+) or QBH2 is the most likely source of the electron required for the reduction of oxidized cyt b559.(ABSTRACT TRUNCATED AT 400 WORDS)     

Observation of the protonated semiquinone intermediate in isolated reaction centers from Rhodobacter sphaeroides: implications for the mechanism of electron and proton transfer in proteins.

A proton-activated electron transfer (PAET) mechanism, involving a protonated semiquinone intermediate state, had been proposed for the electron-transfer reaction k(2)AB [Q(A)(-)(*)Q(B)(-)(*) + H(+) <--> Q(A)(-)(*)(Q(B)H)(*) --> Q(A)(Q(B)H)(-)] in reaction centers (RCs) from Rhodobacter sphaeroides [Graige, M. S., Paddock, M. L., Bruce, M. L., Feher, G., and Okamura, M. Y. (1996) J. Am. Chem. Soc. 118, 9005-9016]. Confirmation of this mechanism by observing the protonated semiquinone (Q(B)H)(*) had not been possible, presumably because of its low pK(a). By replacing the native Q(10) in the Q(B) site with rhodoquinone (RQ), which has a higher pK(a), we were able to observe the (Q(B)H)(*) state. The pH dependence of the semiquinone optical spectrum gave a pK(a) = 7.3 +/- 0.2. At pH < pK(a), the observed rate for the reaction was constant and attributed to the intrinsic electron-transfer rate from Q(A)(-)(*) to the protonated semiquinone (i.e., k(2)AB = k(ET)(RQ) = 2 x 10(4) s(-)(1)). The rate decreased at pH > pK(a) as predicted by the PAET mechanism in which fast reversible proton transfer precedes rate-limiting electron transfer. Consequently, near pH 7, the proton-transfer rate k(H) > 10(4) s(-)(1). Applying the two step mechanism to RCs containing native Q(10) and taking into account the change in redox potential, we find reasonable values for the fraction of (Q(B)H)(*) congruent with 0.1% (consistent with a pK(a)(Q(10)) of approximately 4.5) and k(ET)(Q(10)) congruent with 10(6) s(-)(1). These results confirm the PAET mechanism in RCs with RQ and give strong support that this mechanism is active in RCs with Q(10) as well.     

Effect of low temperatures on photochemical activity of PS1 reaction centers from <Emphasis Type="Italic">Synechocystis</Emphasis> sp. frozen under illumination

After cooling of Synechocystis sp. photosystem 1 (PS1) reaction centers (RC) to 160 K under illumination most of the photoactive pigment is fixed for a long time in the oxidized state. The same effect is observed in purple bacteria RC. The dark reduction kinetics of PS1 P700 chlorophyll, which still retains its photochemical activity, in these samples was similar to that in samples cooled in the dark. We suggest that the photoinduced charge separation in PS1 RC, as well as in purple bacteria RC, is accompanied by conformational changes that can be fixed in samples cooled under illumination. As a result, the electrons photomobilized in RC cooled under illumination are unable to return backward the process of electron transfer to P700(+) after cessation of actinic illumination. Such irreversible trapping of electrons can take place in different parts of the PS1 RC electron acceptor chain.     

Observation of multiple radical pair states in photosystem 2 reaction centers.

Charge recombination of the primary radical pair in D1/D2 reaction centers from photosystem 2 has been studied by time-resolved fluorescence and absorption spectroscopy. The kinetics of the primary radical pair are multiexponential and exhibit at least two lifetimes of 20 and 52 ns. In addition, a third lifetime of approximately 500 ps also appears to be present. These multiexponential charge-recombination kinetics reflect either different conformational states of D1/D2 reaction centers, with the different conformers exhibiting different radical pair lifetimes, or relaxations in the free energy of the radical pair state. Whichever model is invoked, the free energies of formation of the different radical pair states exhibit a linear temperature dependence from 100 to 220 K, indicating that they are dominated by entropy with negligible enthalpy contributions. These results are in agreement with previous determinations of the thermodynamics that govern primary charge separation in both D1/D2 reaction centers [Booth, P.J., Crystall, B., Giorgi, L. B., Barber, J., Klug, D.R., & Porter, G. (1990) Biochim. Biophys. Acta 1016, 141-152] and reaction centers of purple bacteria [Woodbury, N.W.T., & Parson, W.W. (1984) Biochim. Biophys. Acta 767, 345-361]. It is possible that these observations reflect structural changes that accompanying primary charge separation and assist in stabilization of the radical pair state thus optimizing the efficiency of primary electron transfer.     

Is bicarbonate in Photosystem II the equivalent of the glutamate ligand to the iron atom in bacterial reaction centers?

Photosystem II of oxygen-evolving organisms exhibits a bicarbonate-reversible formate effect on electron transfer between the primary and secondary acceptor quinones, QA and QB. This effect is absent in the otherwise similar electron acceptor complex of purple bacteria, e.g., Rhodobacter sphaeroides. This distinction has led to the suggestion that the iron atom of the acceptor quinone complex in PS II might lack the fifth and sixth ligands provided in the bacterial reaction center (RC) by a glutamate residue at position 234 of the M-subunit in Rb. sphaeroides RCs (M232 in Rps. viridis). By site-directed mutagenesis we have altered GluM234 in RCs from Rb. sphaeroides, replacing it with valine, glutamine and glycine to form mutants M234EV, M234EQ and M234EG, respectively. These mutants grew competently under phototrophic conditions and were tested for the formate-bicarbonate effect. In chromatophores there were no detectable differences between wild type (Wt) and mutant M234EV with respect to cytochrome b-561 reduction following a flash, and no effect of bicarbonate depletion (by incubation with formate). In isolated RCs, several electron transfer activities were essentially unchanged in Wt and M234EV, M234EQ and M234EG mutants, and no formate-bicarbonate effect was observed on: (a) the fast or slow phases of recovery of the oxidized primary donor (P+) in the absence of exogenous donor, i.e., the recombination of P+Q-A or P+Q-B, respectively; (b) the kinetics of electron transfer from Q-A to QB; or (c) the flash dependent oscillations of semiquinone formation in the presence of donor to P+ (QB turnover). The absence of a formate-bicarbonate effect in these mutants suggests that GluM234 is not responsible for the absence of the formate-bicarbonate effect in Wt bacterial RCs, or at least that other factors must be taken into account. The mutant RCs were also examined for the fast primary electron transfer along the active (A-)branch of the pigment chain, leading to reduction of QA. The kinetics were resolved to reveal the reduction of the monomer bacteriochlorophyll (tau = 3.5 ps), followed by reduction of the bacteriopheophytin (tau = 0.9 ps). Both steps were essentially unaltered from the wild type. However, the rate of reduction of QA was slowed by a factor of 2 (tau = 410 +/- 30 and 47 +/- 30 ps for M234EQ and M234EV, respectively, compared to 220 ps in the wild type).(ABSTRACT TRUNCATED AT 400 WORDS)     

Kinetics of pigment-acceptor interaction induced by continuous illumination in Synechocystis spaeroides photosystem I preparations cooled to 160 K in the dark and light

The kinetics of dark reduction of chlorophyll P700 oxidized by continuous light in preparations of photosystem I reaction centers from cyanobacterium Synechosystis spharoides cooled in the dark to 160 K is essentially nonexponential. The characteristic times of the components range from fractions of a second to minutes or more. During the cooling of reaction center preparations under illumination with actinic light, most of the chlorophyll P700 molecules are fixed in the oxidized state at 160 K. The kinetics of dark reduction of P700⁺ in the fraction of reaction centers that retain photochemical activity under these conditions is somewhat faster compared to the samples cooled in the dark. A theoretical analysis of substantial deceleration of P700⁺ dark recovery kinetics was done for preparations of photosystem I reaction centers oxidized by continuous light at 160 K in comparison to the experiments where reaction centers were oxidized by short single light flashes. This slowing down of the kinetics in samples excited by continuous illumination can be explained by microconformational relaxation processes related to proton shifts in the reaction center.     

Decay products of the S(3) state of the oxygen-evolving complex of photosystem II at cryogenic temperatures. Pathways to the formation of the S = 7/2 S(2) state configuration

The water-oxidizing complex of photosystem II cycles through five oxidation states, denoted S(i)() (i = 0-4), during water oxidation to molecular oxygen, which appears at the (transient) S(4) state. The recent detection of bimodal EPR signals from the S(3) state [Matsukawa, T., Mino, H., Yoneda, D., Kawamori, A. (1999) Biochemistry 38, 4072-4077] has drawn significant attention to this critical state. An interesting property of the S(3) state is the sensitivity to near-IR (NIR) light excitation. Excitation of the S(3) state by near-IR light at cryogenic temperatures induces among other signals a derivative-shaped EPR signal at g= 5 [Ioannidis, N., and Petrouleas, V. (2000) Biochemistry 39, 5246-5254]. The signal bears unexpected similarities to a signal observed earlier in samples that had undergone multiple turnovers and subsequently had been stored at 77 K for a week or longer [Nugent, J. H. A., Turconi, S., and Evans, M. C. W. (1997) Biochemistry 36, 7086-7096]. Recently, both signals were assigned to an S = 7/2 configuration of the Mn cluster [Sanakis, Y., Ioannidis, N., Sioros, G., and Petrouleas, V. (2001) J. Am. Chem. Soc. 123, 10766-10767]. In the present study, we employ bimodal EPR spectroscopy to investigate the pathways of formation of this unusual state. The following observations are made: (i) The g = 5 signal evolves in apparent correlation with the diminution of the S(3) state signals during the slow (tens of hours to several days range) charge recombination of S(3) with Q(A)(-) at 77 K. The tyrosyl radical D* competes with S(3) for recombination with Q(A)(-), the functional redox couple at cryogenic temperatures inferred to be D*/D(-). Transfer to -50 degrees C and above results in the relaxation of the g = 5 to the multiline and g = 4.1 signals of the normal S(2) state. (ii) The transition of S(3) to the state responsible for the g = 5 signal can be reversed by visible light illumination directly at -30 degrees C or by illumination at 4.2 K followed by brief (2 min) transfer to -50 degrees C in the dark. The latter step is required in order to overcome an apparent thermal activation barrier (charge recombination appears to be faster than forward electron transfer at 4.2 K). (iii) The "g = 5" state can be reached in a few tens of minutes at 4.2 K by near-IR light excitation of the S(3) state. This effect is attributed to the transfer of the positive hole from the Mn cluster to a radical (probably tyr Z), which recombines much faster than the Mn cluster with Q(A)(-). (iv) The above properties strongly support the assignment of the configuration responsible for the g = 5 signal to a modified S(2) state, denoted S(2)'. Evidence supporting the assignment of the S(2)' to a proton-deficient S(2) configuration is provided by the observation that the spectrum of S(2) at pH 8.1 (obtained by illumination of the S(1) state at -30 degrees C) contains a g = 5 contribution.     

Two redox-active beta-carotene molecules in photosystem II

Photosystem II (PS II) contains secondary electron-transfer paths involving cytochrome b(559) (Cyt b(559)), chlorophyll (Chl), and beta-carotene (Car) that are active under conditions when oxygen evolution is blocked such as in inhibited samples or at low temperature. Intermediates of the secondary electron-transfer pathways of PS II core complexes from Synechocystis PCC 6803 and Synechococcus sp. and spinach PS II membranes have been investigated using low temperature near-IR spectroscopy and electron paramagnetic resonance (EPR) spectroscopy. We present evidence that two spectroscopically distinct redox-active carotenoids are formed upon low-temperature illumination. The Car(+) near-IR absorption peak varies in wavelength and width as a function of illumination temperature. Also, the rate of decay during dark incubation of the Car(+) peak varies as a function of wavelength. Factor analysis indicates that there are two spectral forms of Car(+) (Car(A)(+) has an absorbance maximum of 982 nm, and Car(B)(+) has an absorbance maximum of 1027 nm) that decay at different rates. In Synechocystis PS II, we observe a shift of the Car(+) peak to shorter wavelength when oxidized tyrosine D (Y(D)*) is present in the sample that is explained by an electrostatic interaction between Y(D)* and a nearby beta-carotene that disfavors oxidation of Car(B). The sequence of electron-transfer reactions in the secondary electron-transfer pathways of PS II is discussed in terms of a hole-hopping mechanism to attain the equilibrated state of the charge separation at low temperatures.