Subpicosecond and picosecond studies of electron transfer intermediates in Rhodopseudomonas sphaeroides reaction centers

The primary electron transfer processes in isolated reaction centers of Rhodopseudomonas sphaeroides have been investigated with subpicosecond and picosecond spectroscopic techniques. Spectra and kinetics of the absorbance changes following excitation with 0.7-ps 610-nm pulses, absorbed predominantly by bacteriochlorophyll (BChl), indicate that the radical pair state P⁺BPh^?, in which an electron has been transferred from the BChl dimer (P) to a bacteriopheophytin (BPh), is formed with a time constant no greater than 4 ps. The initial absorbance changes also reveal an earlier state, which could be an excited singlet state, or a P⁺BChl^? radical pair.The bleaching at 870 nm produced by 7 ps excitation pulses at 530 nm (absorbed by BPh) or at 600 nm (absorbed predominantly by BChl) shows no resolvable delay with respect to standard compounds in solution, suggesting that the time for energy transfer from BPh to P is less than 7 ps. However, the bleaching in the BPh band at 545 nm following 7-ps 600-nm excitation, exhibits an 8- to 10-ps lag with respect to standard compounds. This finding is qualitatively similar to the 35-ps delay previously observed at 760 nm by Shuvalov at al. (Shuvalov, V.A., Klevanik, A.V., Sharkov, A.V., Matveetz, Y.A. and Kryukov, P.G. (1978) FEBS Lett. 91, 135–139) when 25-ps 880-nm excitation flashes were used. A delay in the bleaching approximately equal to the width of the excitation flash can be explained in terms of the opposing effects of bleaching due to the reduction of BPh, and absorbance increases due to short-lived excited states (probably of BChl) that turn over rapidly during the flash.The decay of the initial bleaching at 800 nm produced by 7-ps 530- or 600-nm excitation flashes shows a fast component with a 30-ps time constant, in addition to a slower component having the 200-ps kinetics expected for the decay of P⁺BPh^?. The dependence on excitation intensity of the absorbance changes due to the 30-ps component indicate that the quantum yield of the state responsible for this step is lower than that observed for the primary electron transfer reactions. This suggests that at least part of the transient bleaching at 800 nm is due to a secondary process, possibly caused by excitation with an excessive number of photons. If the 800-nm absorbing BChl (B) acts as an intermediate electron carrier in the primary photochemical reaction, electron transfer between B and the BPh must have a time constant no greater than 4 ps.     

Kinetics and thermodynamics of the P870+Q−A → P870+Q−B reaction in isolated reaction centers from the photosynthetic bacterium Rhodopseudomonas sphaeroides

The temperature dependences of the P870⁺Q^?_A → P870Q_A and P870⁺Q^?_B → P870Q_B recombination reactions were measured in reaction centers from Rhodopseudomonas sphaeroides. The data indicate that the P870⁺Q^?_B state decays by thermal repopulation of the P870⁺Q^?_A state, followed by recombination. ΔG° for the P870⁺Q^?_A → P870⁺Q^?_B reaction is ?6.89 kJ · mol^?1, while ΔH° = ?14.45 kJ · mol^?1 and ?TΔS° = + 7.53 kJ · mol^?1. The activation ethalpy, $\text{H}{}^3$, for the P870⁺Q^?_A Δ P870⁺Q^?_B reaction is +56.9 kJ · mol^?1, while the activation entropy is near zero. The results permit an estimate of the shape of the potential energy curve for the P870⁺Q^?_A → P870⁺Q^?_B electron transfer reaction.     

Linear dichroism and the orientation of reaction centers of Rhodopseudomonas sphaeroides in dried gelatin films

Aqueous mixtures of reaction centers of Rhodopseudomonas sphaeroides and gelatin were dried to form thin films. Following hydration, these films were stretched as much as two to three times their original length. Polarized absorption spectra showing linear dichroism were obtained for both unstretched and stretched films, with the planes and stretching axes of the films mounted in various geometries relative to the electric vector of the measuring beam. These data were analyzed in terms of the following model: Reaction centers possess an axis of symmetry that is fixed in relation to the reaction center structure. In unstretched films this axis is confined to the film plane and oriented at random within the plane. In stretched films the symmetry axis is aligned with the direction of stretching. In both preparations reaction centers are distributed randomly with respect to rotation about the axis of symmetry. The data are consistent with this model when the analysis acknowledges less than perfect orientation. For perfect orientation in a stretched film the model predicts uniaxial symmetry about the axis of stretching. The approach to this condition was examined with films stretched to different extents. Extrapolation yielded dichroic ratios for the ideal case of perfect orientation, and allowed calculation of the angles between the axis of symmetry and the various optical transition dipoles in the reaction center. This treatment included the two absorption bands of the bacteriochlorophyll ‘special pair’ (photochemical electron donor) in the Q_x region, at 600 and 630 nm, which we were able to resolve in light minus dark difference spectra.     

Coupling of nuclear wavepacket motion and charge separation in bacterial reaction centers

The mechanism of the charge separation and stabilization of separated charges was studied using the femtosecond absorption spectroscopy. It was found that nuclear wavepacket motions on potential energy surface of the excited state of the primary electron donor P* leads to a coherent formation of the charge separated states P⁺B_A⁻, P⁺H_A⁻ and P⁺H_B⁻ (where B_A, H_B and H_A are the primary and secondary electron acceptors, respectively) in native, pheophytin-modified and mutant reaction centers (RCs) of Rhodobacter sphaeroides R-26 and in Chloroflexus aurantiacus RCs. The processes were studied by measurements of coherent oscillations in kinetics at 890 and 935 nm (the stimulated emission bands of P*), at 800 nm (the absorption band of B_A) and at 1020 nm (the absorption band of B_A⁻) as well as at 760 nm (the absorption band of H_A) and at 750 nm (the absorption band of H_B). It was found that wavepacket motion on the 130–150 cm⁻¹ potential surface of P* is accompanied by approaches to the intercrossing region between P* and P⁺B_A⁻ surfaces at 120 and 380 fs delays emitting light at 935 nm (P*) and absorbing light at 1020 nm (P⁺B_A⁻). In the presence of Tyr M210 (Rb. sphaeroides) or M195 (C. aurantiacus) the stabilization of P⁺B_A⁻ is observed within a few picosseconds in contrast to YM210W. At even earlier delay (40 fs) the emission at 895 nm and bleaching at 748 nm are observed in C. aurantiacus RCs showing the wavepacket approach to the intercrossing between the P* and P⁺H_B⁻ surfaces at that time. The 32 cm⁻¹ rotation mode of HOH was found to modulate the electron transfer rate probably due to including of this molecule in polar chain connecting P_B and B_A and participating in the charge separation. The mechanism of the charge separation and stabilization of separated charges is discussed in terms of the role of nuclear motions, of polar groups connecting P and acceptors and of proton of OH group of TyrM210.     

Different temperature dependencies of the charge recombination reaction in photoreaction centers isolated from different bacterial species

We compared the temperature dependency of the rate of the charge recombination reaction in photoreaction centers isolated from Ectothiorhodospira sp. and from Rhodospirillum rubrum G9. We also examined the temperature dependency of the bandwidth and peak wavelength of their far-red absorption band. In both preparations, the peak wavelength and the bandwidth vary monotonically with temperature between 80 and 300 K. However, the rate of the charge recombination reaction has a quite different temperature dependency. In the preparation from R. rubrum, the reaction is accelerated 5-fold in a typical sigmoidal fashion as the temperature is lowered from 300 to 80 K. In the preparation from Ectothiorhodospira sp., the reaction is accelerated monotonically only about 1.5-fold in the same temperature range. At temperatures below 100 K, the rates are similar in the two preparations. We interpret the temperature dependency of the charge recombination reaction in terms of an activationless electron-transfer model formulated by Jortner (Jortner, J. (1980) Biochim. Biophys. Acta 394, 193–230). The minimal model provides a good fit for the temperature dependency of charge recombination in the preparation from Ectothiorhodospira sp. However, to fit the temperature dependency of the R. rubrum preparation with the same model, we must further postulate that the electronic coupling factor varies with temperature in this preparation. We find that, in both preparations, the temperature dependency of the far-red absorption bandwidth is consistent with the assumption that similar vibrational modes are involved in electron transfer and in electronic excitation.     

Electron acceptors of bacterial photosynthetic reaction centers II. H+ binding coupled to secondary electron transfer in the quinone acceptor complex

The photoreduction of ubiquinone in the electron acceptor complex (Q₁Q₁₁) of photosynthetic reaction centers from Rhodopseudomonas sphaeroides, R26, was studied in a series of short, saturating flashes. The specific involvement of H⁺ in the reduction was revealed by the pH dependence of the electron transfer events and by net H⁺ binding during the formation of ubiquinol, which requires two turnovers of the photochemical act. On the first flash Q₁₁ receives an electron via Q₁ to form a stable ubisemiquinone anion (Q?^?₁₁); the second flash generates Q?^?₁. At low pH the two semiquinones rapidly disproportionate with the uptake of 2 H⁺, to produce Q₁₁H₂. This yields out-of-phase binary oscillations for the formation of anionic semiquinone and for H⁺ uptake. Above pH 6 there is a progressive increase in H⁺ binding on the first flash and an equivalent decrease in binding on the second flash until, at about pH 9.5, the extent of H⁺ binding is the same on all flashes. The semiquinone oscillations, however, are undiminished up to pH 9. It is suggested that a non-chromophoric, acid-base group undergoes a pK shift in response to the appearance of the anionic semiquinone and that this group is the site of protonation on the first flash. The acid-base group, which may be in the reaction center protein, appears to be subsequently involved in the protonation events leading to fully reduced ubiquinol. The other proton in the two electron reduction of ubiquinone is always taken up on the second flash and is bound directly to Q?^?₁₁. At pH values above 8.0, it is rate limiting for the disproportionation and the kinetics, which are diffusion controlled, are properly responsive to the prevailing pH. Below pH 8, however, a further step in the reaction mechanism was shown to be rate limiting for both H⁺ binding electron transfer following the second flash.     

Temperature dependence of the primary electron transfer reaction in pigment-modified bacterial reaction centers

The initial electron transfer steps in pigment modified reaction centers, where bacteriopheophytin is replaced by plant pheophytin (R26.Phe-a RCs) have been investigated over a wide temperature range by femtosecond time-resolved spectroscopy. The experimental data obtained in the maximum of the bacteriochlorophyll anion band at 1020 nm show the existence of a high and long-lived population of the primary acceptor P⁺B_A ^– even at 10 K. The data suggest a stepwise electron transfer mechanism with B_A as primary acceptor also in the low temperature domain. A detailed data analysis suggests that the pigment modification leads to a situation with almost isoenergetic primary and secondary acceptor levels, approximately 450 cm^–1 below P^*. A Gaussian distribution (with = 400 cm ^–1) of the G values has to be assumed to account for the strong dispersive character of the kinetics in this sample. Based on these assumptions, a model is presented that reproduces the observed kinetics, heterogeneity and temperature dependence.     

Determination of the primary charge separation rate in Photosystem II reaction centers at 15 K

We have measured the rate constant for the formation of the oxidized chlorophyll a electron donor (P680⁺) and the reduced electron acceptor pheophytin a ^– (Pheo a ^–) following excitation of isolated Photosystem II reaction centers (PS II RC) at 15 K. This PS II RC complex consists of D₁, D₂, and cytochrome b-559 proteins and was prepared by a procedure which stabilizes the protein complex. Transient absorption difference spectra were measured from 450–840 nm as a function of time with 500fs resolution following 610 nm laser excitation. The formation of P680⁺-Pheo a ^– is indicated by the appearance of a band due to P680⁺ at 820 nm and corresponding absorbance changes at 490, 515 and 546 nm due to the formation of Pheo a ^–. The appearance of the 490 nm and 820 nm bands is monoexponenital with =1.4±0.2 ps. Treatment of the PS II RC with sodium dithionite and methyl viologen followed by exposure to laser excitation results in accumulation of Pheo a ^–. Laser excitation of these prereduced RCs at 15 K results in formation of a transient absorption spectrum assigned to ^1*P680. We observe wavelength-dependent kinetics for the recovery of the transient bleach of the Q_y absorption bands of the pigments in both untreated and pre-reduced PS II RCs at 15K. This result is attributed to an energy transfer process within the PS II RC at low temperature that is not connected with charge separation.Abbreviations PS I Photosystem I - PS II Photosystem II - RC reaction center - P680 primary electron donor in Photosystem II - Chl a chlorophyll a - Pheo a pheophytin a     

Electrostatic role of the non-heme iron complex in bacterial photosynthetic reaction center

To elucidate the role of the non-heme iron complex (Fe-complex) in the electron transfer (ET) events of bacterial photosynthetic reaction centers (bRC), we calculated redox potentials of primary/secondary quinones Q(A/B) (E(m)(Q(A/B))) in the Fe-depleted bRC. Removing the Fe-complex, the calculated E(m)(Q(A/B)) are downshifted by approximately 220 mV/ approximately 80 mV explaining both the 15-fold decrease in ET rate from bacteriopheophytin (H(A)(-)) to Q(A) and triplet state occurrence in Fe-depleted bRC. The larger downshift in E(m)(Q(A)) relative to E(m)(Q(B)) increases the driving-energy for ET from Q(A) to Q(B) by 140 meV, in agreement with approximately 100 meV increase derived from kinetic studies.     

Redox potential of the non-heme iron complex in bacterial photosynthetic reaction center

In bacterial photosynthetic reaction centers (bRC), the electron is transferred from the special pair (P) via accessory bacteriochlorophyll (B_A), bacteriopheopytin (H_A), the primary quinone (Q_A) to the secondary quinone (Q_B). Although the non-heme iron complex (Fe complex) is located between Q_A and Q_B, it was generally supposed not to be redox-active. Involvement of the Fe complex in electron transfer (ET) was proposed in recent FTIR studies [A. Remy and K. Gerwert, Coupling of light-induced electron transfer to proton uptake in photosynthesis, Nat. Struct. Biol. 10 (2003) 637-644]. However, other FTIR studies resulted in opposite results [J. Breton, Steady-state FTIR spectra of the photoreduction of Q_A and Q_B in Rhodobacter sphaeroides reaction centers provide evidence against the presence of a proposed transient electron acceptor X between the two quinones, Biochemistry 46 (2007) 4459-4465]. In this study, we calculated redox potentials of Q_A/B (E_m(Q_A/B)) and the Fe complex (E_m(Fe)) based on crystal structure of the wild-type bRC (WT-bRC), and we investigated the energetics of the system where the Fe complex is assumed to be involved in the ET. E_m(Fe) in WT-bRC is much less pH-dependent than that in PSII. In WT-bRC, we observed significant coupling of ET with Glu-L212 protonation upon oxidation of the Fe complex and a dramatic E_m(Fe) downshift by 230 mV upon formation of Q_A⁻ (but not Q_B⁻) due to the absence of proton uptake of Glu-L212. Changes in net charges of the His ligands of the Fe complex appear to be the nature of the redox event if we assume the involvement of the Fe complex in the ET.     

Delayed fluorescence from Rhodopseudomonas sphaeroides reaction centers. Enthalpy and free energy changes accompanying electron transfer from P-870 to quinones

Delayed fluorescence from isolated reaction centers of Rhodopseudomonas sphaeroides was measured to study the energetics of electron transfer from the bacteriochlorophyll complex (P-870, or P) to the primary and secondary quinones (Q_A and Q_B). The analysis was based on the assumption that electron transfer between P and Q reaches equilibrium quickly after flash excitation, and stays in equilibrium during the lifetime of the P⁺Q⁻ radical pair. Delayed fluorescence of 1Q reaction centers (reaction centers that contain only Q_A) has a lifetime of about 0.1 s, which corresponds to the decay of P⁺Q⁻_A. 2Q reaction centers (which contain both Q_A and Q_B) have a much weaker delayed fluorescence, with a lifetime that corresponds to that of P⁺Q⁻_B (about 1 s). In the presence of o-phenanthroline, the delayed fluorescence of 2Q reaction centers becomes similar in intensity and decay kinetics to that of 1Q reaction centers. From comparisons of the intensities of the delayed fluorescence from P⁺Q⁻_A and P⁺Q⁻_B, the standard free energy difference between P⁺Q⁻_A and P⁺Q⁻_B is calculated to be 78 ± 8 meV. From a comparison of the intensity of the delayed fluorescence with that of prompt fluorescence, we calculate that P⁺Q⁻_A is 0.86 ± 0.02 eV below the excited singlet state of P in free energy, or about 0.52 eV above the ground state PQ_A. The temperature dependence of the delayed fluorescence indicates that P⁺Q⁻_A is about 0.75 eV below the excited singlet state in enthalpy, or about 0.63 eV above the ground state.     

A study of the primary charge separation in green bacteria by means of flash spectroscopy

A reaction-center pigment-protein complex of the green bacterium Prosthecochloris aestuarii was studied by means of nanosecond-flash spectroscopy. In this complex electron transfer between the primary and secondary acceptor is blocked. The spectra and kinetics of the absorption changes induced by a short flash indicated the formation of the radical pair P-840⁺I^?, which decayed in 20–35 ns, mainly to the triplet state of the primary electron donor P-840. The absorption difference spectrum of the initial absorption change indicated that the primary acceptor I is either bacteriopheophytin c or another pigment with absorption maximum at 665 nm.     

Effect of inhibitors,redox state and isoprenoid chain length on the affinity of ubiquinone for the secondary acceptor binding site in the reaction centers of photosynthetic bacteria

Quinone and inhibitor binding to Rhodopseudomonas sphaeroides (R-26 and GA) reaction centers were studied using spectroscopic methods and by direct adsorption of reaction centers onto anion exchange filters in the presence of ¹⁴C-labelled quinone or inhibitor. These measurements show that as secondary acceptor, Q_B, ubiquinone (UQ) is tightly bound in the semiquinone form and loosely bound in the quinone and quinol forms. The quinol is probably more loosely bound than the quinone. o-Phenanthroline and terbutryn, a triazine inhibitor, compete with UQ and with each other for binding to the reaction center. Inhibition by o-phenanthroline of electron transfer from the primary to the secondary quinone acceptor (Q_A to Q_B) occurs via displacement of UQ from the Q_B binding site. Displacement of UQ by terbutryn is apparently accessory to the inhibition of electron transfer. Terbutryn binding is lowered by reduction of Q_B to Q^?_B but is practically unaffected by reduction of Q_A to Q^?_A in the absence of Q_B. UQ-9 and UQ-10 have a 5- to 6-fold higher binding affinity to the Q_B site than does UQ-1, indicating that the long isoprenoid chain facilitates the binding to the Q_B site.     

Enthalpy and volume changes accompanying electron transfer from P-870 to quinones in Rhodopseudomonas sphaeroides reaction centers

A capacitor microphone was used to measure the enthalpy and volume changes that accompany the electron transfer reactions, $\text{PQ}{}_{\mathrm{A}}\text{→}\text{hv}\text{P}{}^{\mathrm{+}}\text{Q}{}^{\mathrm{?}}{}_{\mathrm{A}}\text{and PQ}{}_{\mathrm{A}}\text{Q}{}_{\mathrm{B}}\text{→}\text{hv}\text{P}{}^{\mathrm{+}}\text{Q}{}_{\mathrm{A}}\text{Q}{}^{\mathrm{?}}{}_{\mathrm{B}}$, following flash excitation of photosynthetic reaction centers isolated from Rhodopseudomonas sphaeroides. P is a bacteriochlorophyll dimer (P-870), and Q_A and Q_B are ubiquinones. In reaction centers containing only Q_A, the enthalpy of P⁺Q^?_A is very close to that of the PQ_A ground state (ΔH_r = 0.05 ± 0.03 eV). The free energy of about 0.65 eV that is captured in the photochemical reaction evidently takes the form of a substantial entropy decrease. In contrast, the formation of P⁺Q_AQ^?_B in reaction centers containing both quinones has a ΔH_r of 0.32 ± 0.02 eV. The entropy change must be near zero in this case. In the presence of o-phenanthroline, which blocks electron transfer between Q^?_A and Q_B, ΔH_r for forming P⁺Q^?_AQ_B is 0.13 ± 0.03 eV. The influence of flash-induced proton uptake on the results was investigated, and the ΔH_r values given above were measured under conditions that minimized this influence. Although the reductions of Q_A and Q_B involve very different changes in enthalpy and entropy, both reactions are accompanied by a similar volume decrease of about 20 ml/mol. The contraction probably reflects electrostriction caused by the charges on P⁺ and Q^?_A or Q^?_B.     

Femtosecond nuclear oscillations under charge separation in reaction centers of photosynthesis

Results are presented of a study of primary processes of formation of the charge separated states P⁺B_A ^- and P⁺H_A ^- (where P is the primary electron donor, B_A and H_A the primary and secondary electron acceptors) in native and pheophytin-modified reaction centers (RCs) of Rhodobacter sphaeroides R-26 by methods of femtosecond spectroscopy of absorption changes at low temperature. Coherent oscillations were studied in the kinetics at 935 nm (P* stimulated emission band), at 1020 nm (B_A ^- absorption band), and at 760 nm (H_A absorption band). It was found that when the wavepacket created under femtosecond light excitation approaches the intersection between P* and P⁺B_A ^- potential surfaces at 120- and 380-fsec delays, the formation of two electron states emitting light at 935 nm (P*) and absorbing light at 1020 nm (P⁺B_A ^-) takes place. At the later time the wavepacket motion has a frequency of 32 cm^-1 and is accompanied by electron transfer from P* to B_A in pheophytin-modified and native RCs and further to H_A in native RCs. It was shown that electron transfer processes monitored by the 1020-nm absorption band development as well as by bleaching of 760-nm absorption band have the enhanced 32 cm^-1 mode in the Fourier transform spectra.     

Resolution of electron and proton transfer events in the electrochromism associated with quinone reduction in bacterial reaction centers

We have measured the electrochromic response of the bacteriopheophytin, BPh, and bacteriochlorophyll, BChl, cofactors during the Q_A ^–Q_B Q_AQ_B ^– electron transfer in chromatophores of Rhodobacter (Rb.) capsulatus and Rb. sphaeroides. The electrochromic response rises faster in chromatophores and is more clearly biexponential than it is in isolated reaction centers. The chromatophore spectra can be interpreted in terms of a clear kinetic separation between fast electron transfer and slower non-electron transfer events such as proton transfer or protein relaxation. The electrochromic response to electron transfer exhibits rise times of about 4 µs (70%) and 40 µs (30%) in Rb. capsulatus and 4 µs (60%) and 80 µs (40%) in Rb. sphaeroides. The BPh absorption band is shifted to nearly equivalent positions in the Q_A ^– and nascent Q_B ^– states, indicating that the electrochromic perturbation of BPh absorption from the newly formed Q_B ^– state is comparable to that of Q_A ^– . Subsequently, partial attenuation of the Q_B ^– electrochromism occurs with a time constant on the order of 200 µs. This can be attributed to partial charge compensation by H⁺ (or other counter ion) movement into the Q_B pocket. Electron transfer events were found to be slower in detergent isolated RCs than in chromatophores, more nearly monoexponential, and overlap H⁺ transfer, suggesting that a change in rate-limiting step has occurred upon detergent solubilization.     

Effects of detergent on the excited state structure and relaxation dynamics of the photosystem II reaction center: A high resolution hole burning study

Low temperature (4.2 K) absorption and hole burned spectra are reported for a stabilized preparation (no excess detergent) of the photosystem II reaction center complex. The complex was studied in glasses to which detergent had and had not been added. Triton X-100 (but not dodecyl maltoside) detergent was found to significantly affect the absorption and persistent hole spectra and to disrupt energy transfer from the accessory chlorophyll a to the active pheophytin a. However, Triton X-100 does not significantly affect the transient hole spectrum and lifetime (1.9 ps at 4.2 K) of the primary donor state, P680^*. Data are presented which indicate that the disruptive effects of Triton X-100 are not due to extraction of pigments from the reaction center, leaving structural perturbations as the most plausible explanation. In the absence of detergent the high resolution persistent hole spectra yield an energy transfer decay time for the accessory Chl a Q_Y-state at 1.6 K of 12 ps, which is about three orders of magnitude longer than the corresponding time for the bacterial RC. In the presence of Triton X-100 the Chl a Q_Y-state decay time is increased by at least a factor of 50.Abbreviations PS I photosystem I - PS II photosystem II - RC reaction center - P680, P870, P960 the primary electron donor absorption bands of photosystem II, Rhodobacter sphaeroides, Rhodopseudomonas viridis - NPHB nonphotochemical hole burning - TX Triton X-100 - DM Dodecyl Maltoside - Chl chlorophyll - Pheo pheophytin - ZPH ero phonon hole     

Localization of the secondary quinone-binding site in reaction centers from Rhodopseudomonas sphaeroides R-26 by antibody inhibition of electron transfer

Inhibition of the electron transfer from Q_A to Q_B was measured in the presence of Fab fragments of antibodies directed against the subunits of reaction centers of Rhodopseudomonas sphaeroides R-26. Anti-M Fab inhibited the electron transfer, whereas anti-L Fab and anti-H Fab did not. From these experiments, we conclude that the binding site for Q_B is located on the M-subunit.     

Influence of magnetic fields on the P-870 triplet state in Rps. sphaeroides reaction centers

Magnetic fields influence two properties of the P-870 triplet state observed in Rps. sphaeroides reaction centers: the yield of formation and the kinetics of decay. These effects have been studied in reaction centers which were prepared in three different states: state Q_A ^–, state Q_A ^2– and state (– Q_A) (Q_A depleted). The triplet yields decrease with increasing magnetic fields, with B1/2's of about 140, 41 and 57 Gauss, respectively. The half-time of ³P-870 decay is not influenced by the field in state Q_A ^–; it increases at increasing fields, in state Q_A ^2– and state (– Q_A), with the same B1/2 as the triplet yield. These results are discussed in the framework of current theories of the radical-pair dynamics and of the mechanism of triplet decay.Abbreviations I primary electron acceptor - LDAO lauryldimethylamine oxide - P-870 primary electron donor - Q_A first quinone acceptor - SDS sodium dodecylsulfate - YAG Yttrium Aluminum Garnet     

Electron transfer in deuterated reaction centers of Rhodobacter sphaeroides at 90 K according to femtosecond spectroscopy data

The primary act of charge separation was studied in P⁺B_A ^– and P⁺H_A ^– states (P, primary electron donor; B_A and H_A, primary and secondary electron acceptor) of native reaction centers (RCs) of Rhodobacter sphaeroides R-26 using femtosecond absorption spectroscopy at low (90 K) and room temperature. Coherent oscillations were studied in the kinetics of the stimulated emission band of P* (935 nm), of absorption band of B_A ^– (1020 nm) and of absorption band of H_A (760 nm). It was found that in native RCs kept in heavy water (D₂O) buffer the isotopic decreasing of basic oscillation frequency 32 cm ^–1 and its overtones takes place by the same factor 1.3 in the 935, 1020, and 760 nm bands in comparison with the samples in ordinary water H₂O. This suggests that the femtosecond oscillations in RC kinetics with 32 cm ^–1 frequency may be caused by rotation of hydrogen-containing groups, in particular the water molecule which may be placed between primary electron donor P_B and primary electron acceptor B_A. This rotation may appear also as high harmonics up to sixth in the stimulated emission of P*. The rotation of the water molecule may modulate electron transfer from P* to B_A. The results allow for tracing of the possible pathway of electron transfer from P* to B_A along a chain consisting of polar atoms according to the Brookhaven Protein Data Bank (1PRC): Mg(P_B)-N-C-N(His M200)-HOH-O = B_A. We assume that the role of 32-cm ^–1 modulation in electron transfer along this chain consists of a fixation of electron density at B_A ^– during a reversible electron transfer, when populations of P* and P⁺B_A ^– states are approximately equal.