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.     

Kinetics of luminescence in the 10−6–10−4-s range in Chlorella

The decay of luminescence in the 6–600-μs range following a microsecond flash has been studied in Chlorella. The decay is highly polyphasic; three kinetic components are outlined, in confirmation of the results of K. L. Zankel (1971, Biochim. Biophys. Acta 245, 373–385).Extrapolation of the decay to zero dark time suggests that a unique metastable species C^?₊, resulting from photochemical charge separation in the System II reaction center, is the substrate of the recombination reaction which gives rise to luminescence.The fast (5–10 μs) and medium (50–70 μs) phases of the decay denote different stabilization steps, preceding relaxation of the centers by electron and proton transduction to the photosynthetic chain.NH₂OH specifically inhibits the fast phase and enhances the medium phase. This effect is explained by assuming that the fast phase results from electron transfer from the water splitting system Z to the oxidized primary donor Y.3-(3,4-Dichlorophenyl)-1,1-dimethylurea (DCMU), in the presence of NH₂OH elicits another fast phase. It is believed that DCMU affords a parasitic stabilization of C^?₊ by forming a complex with Q^?.     

Electron transfer in reaction centers of Rhodopseudomonas sphaeroides. I. Determination of the charge recombination pathway of D+QAQ−B and free energy and kinetic relations between Q−AQB and QAQ−B

The electron-transfer reactions and thermodynamic equilibria involving the quinone acceptor complex in bacterial reaction centers from R. sphaeroides were investigated. The reactions are described by the scheme: We found that the charge recombination pathway of D⁺Q_AQ^?_B proceeds via the intermediate state D⁺Q^?_AQ_B, the direct pathway contributing less than approx. 5% to the observed recombination rate. The method used to obtain this result was based on a comparison of the kinetics predicted for the indirect pathway (given by the product k_AD-times the fraction of reaction centers in the Q^?_AQ_B state) with the observed recombination rate, k^obs_{D⁺ →D}. The kinetic measurements were used to obtain the pH dependence (6.1 ? pH ? 11.7) of the free energy difference between the states Q^?_AQ_B and Q_AQ^?_B. At low pH (less than 9) Q_AQ^?_B is stabilized relative to Q^?_AQ_B by 67 meV, whereas at high pH Q^?_AQ_B is energetically favored. Both Q^?_A and Q^?_B associate with a proton, with pK values of 9.8 and 11.3, respectively. The stronger interaction of the proton with Q^?_B provides the driving force for the forward electron transfer.     

Protein Dielectric Environment Modulates the Electron-Transfer Pathway in Photosynthetic Reaction Centers

The replacement of tyrosine by aspartic acid at position M210 in the photosynthetic reaction center of Rhodobacter sphaeroides results in the generation of a fast charge recombination pathway that is not observed in the wild-type. Apparently, the initially formed charge-separated state (cation of the special pair, P, and anion of the A-side bacteriopheophytin, H_A) can decay rapidly via recombination through the neighboring bacteriochlorophyll (B_A) soon after formation. The charge-separated state then relaxes over tens of picoseconds and recombination slows to the hundreds-of-picoseconds or nanosecond timescale. This dielectric relaxation results in a time-dependent blue shift of B_A^– absorption, which can be monitored using transient absorbance measurements. Protein dynamics also appear to modulate the electron transfer between H_A and the next electron carrier, Q_A (a ubiquinone). The kinetics of this reaction are complex in the mutant, requiring two kinetic terms, and the spectra associated with the two terms are distinct; a red shift of the H_A ground-state bleaching is observed between the shorter and longer H_A-to-Q_A electron-transfer phases. The kinetics appears to be pH-independent, suggesting a negligible contribution of static heterogeneity originating from protonation/deprotonation in the ground state. A dynamic model based on the energy levels of the two early charge-separated states, P⁺B_A^– and P⁺H_A^–, has been developed in which the energetics of these states is modulated by fast protein dielectric relaxations and this in turn alters both the kinetic complexity of the reaction and the reaction pathway.     

Picosecond spectroscopy of the charge separation in reaction centers of Chloroflexus aurantiacus with selective excitation of the primary electron donor

Absorbance changes in the picosecond region were studied in isolated reaction centers of the green photosynthetic bacterium Chloroflexus aurantiacus upon selective excitation of the primary electron donor, P, at 870 nm. The results indicate that the first observed state is an excited state of P (P1) which appears to transfer an electron to a bacteriochlorophyll a molecule absorbing at 812 nm (B₁) in 10 ± 2 ps as indicated by a bleaching at this wavelength. This reaction is followed by a rapid electron transfer (3 ± 1 ps) from B₁⁻ to bacteriopheophytin a, so that the fraction of reaction centers in the state P⁺B₁⁻ remains small during the experiment. An apparent bleaching at 925 nm is ascribed to stimulated emission from excited P, which emission disappears upon formation of P⁺. The difference between these time constants for electron transfer and those observed for the same reactions in reaction centers of the purple photosynthetic bacterium Rhodopseudomonas (Rhodobacter) sphaeroides is discussed in terms of the energy difference between P1 and P⁺B₁⁻, which appears to be larger for C. aurantiacus.     

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.     

Spectroscopic characterization of a semi-stable, charge-separated state in Cu-substituted reaction centers from Rhodobacter sphaeroides

In reaction centers from Rhodobacter sphaeroides exposed to continuous illumination in the presence of an inhibitor of the Q_A⁻ to Q_B electron transfer, a semi-stable, charge-separated state was formed with halftimes of formation and decay of several minutes. When the non-heme iron was replaced by Cu²⁺, the decay of the semi-stable, charge-separated state became much slower than in centers with bound Fe²⁺ with about the same rate constant for formation. In Cu²⁺-substituted reaction centers, the semi-stable state was associated with an EPR signal, significantly different from that observed after chemical reduction of the acceptor-side quinone or after illumination at low temperature, but similar to that of an isolated Cu²⁺ in the absence of magnetic interaction. The EPR results, obtained with Cu²⁺-substituted reaction centers, suggest that the slow kinetics of formation and decay of the charge-separated, semi-stable state is associated with a structural rearrangement of the acceptor side and the immediate environment of the metal-binding site.     

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.     

Resistance of reaction centers from Rhodobacter sphaeroides against UV-B radiation. Effects on protein structure and electron transport

Inhibition of electron transport and damage to the protein subunits by ultraviolet-B (UV-B, 280–320 nm) radiation have been studied in isolated reaction centers of the non-sulfur purple bacterium Rhodobacter sphaeroides R26. UV-B irradiation results in the inhibition of charge separation as detected by the loss of the initial amplitude of absorbance change at 430 nm reflecting the formation of the P⁺(Q_AQ_B)^– state. In addition to this effect, the charge recombination accelerates and the damping of the semiquinone oscillation increases in the UV-B irradiated reaction centers. A further effect of UV-B is a 2 fold increase in the half- inhibitory concentration of o-phenanthroline. Some damage to the protein subunits of the RC is also observed as a consequence of UV-B irradiation. This effect is manifested as loss of the L, M and H subunits on Coomassie stained gels, but not accompanied with specific degradation products. The damaging effects of UV-B radiation enhanced in reaction centers where the quinone was semireduced (Q_B ^–) during UV-B irradiation, but decreased in reaction centers which lacked quinone at the Q_B binding site. In comparison with Photosystem II of green plant photosynthesis, the bacterial reaction center shows about 40 times lower sensitivity to UV-B radiation concerning the activity loss and 10 times lower sensitivity concerning the extent of reaction center protein damage. It is concluded that the main effect of UV-B radiation in the purple bacterial reaction center occurs at the Q_AQ_B quinone acceptor complex by decreasing the binding affinity of Q_B and shifting the electron equilibration from Q_AQ_B ^– to Q_A ^–Q_B. The inhibitory effect is likely to be caused by modification of the protein environment around the Q_B binding pocket and mediated by the semiquinone form of Q_B. The UV-resistance of the bacterial reaction center compared to Photosystem II indicates that either the Q_AQ_B acceptor complex, which is present in both types of reaction centers with similar structure and function, is much less susceptible to UV damage in purple bacteria, or, more likely, that Photosystem II contains UV-B targets which are more sensitive than its quinone complex.Abbreviations Bchl bacteriochlorophyll - P Bchl dimer - Q_A primary quinone electron acceptor - Q_B secondary quinone electron acceptor - RC reaction center - UV-B ultraviolet-B     

Kinetic and Energetic Model for the Primary Processes in Photosystem II

A detailed model for the kinetics and energetics of the exciton trapping, charge separation, charge recombination, and charge stabilization processes in photosystem (PS) II is presented. The rate constants describing these processes in open and closed reaction centers (RC) are calculated on the basis of picosecond data (Schatz, G. H., H. Brock, and A. R. Holzwarth. 1987. Proc. Natl. Acad. Sci. USA. 84:8414-8418) obtained for oxygen-evolving PS II particles from Synechococcus sp. with ~80 chlorophylls/P₆₈₀. The analysis gives the following results. (a) The PS II reaction center donor chlorophyll P₆₈₀ constitutes a shallow trap, and charge separation is overall trap limited. (b) The rate constant of charge separation drops by a factor of ~6 when going from open (Q-oxidized) to closed (Q-reduced) reaction centers. Thus the redox state of Q controls the yield of radical pair formation and the exciton lifetime in the Chl antenna. (c) The intrinsic rate constant of charge separation in open PS II reaction centers is calculated to be ~2.7 ps^-1. (d) In particles with open RC the charge separation step is exergonic with a decrease in standard free energy of ~38 meV. (e) In particles with closed RC the radical pair formation is endergonic by ~12 meV. We conclude on the basis of these results that the long-lived (nanoseconds) fluorescence generally observed with closed PS II reaction centers is prompt fluorescence and that the amount of primary radical pair formation is decreased significantly upon closing of the RC.     

Impairment of the photosynthetic apparatus by oxidative stress induced by photosensitization reaction of protoporphyrin IX

Treatment with the herbicide acifluorfen-sodium (AF-Na), an inhibitor of protoporphyrinogen oxidase, caused an accumulation of protoporphyrin IX (Proto IX) , light-induced necrotic spots on the cucumber cotyledon within 12-24 h, and photobleaching after 48-72 h of light exposure. Proto IX-sensitized and singlet oxygen (¹O₂)-mediated oxidative stress caused by AF-Na treatment impaired photosystem I (PSI), photosystem II (PSII) and whole chain electron transport reactions. As compared to controls, the F_v/F_m (variable to maximal chlorophyll a fluorescence) ratio of treated samples was reduced. The PSII electron donor NH₂OH failed to restore the F_v/F_m ratio suggesting that the reduction of F_v/F_m reflects the loss of reaction center functions. This explanation is further supported by the practically near-similar loss of PSI and PSII activities. As revealed from the light saturation curve (rate of oxygen evolution as a function of light intensity), the reduction of PSII activity was both due to the reduction in the quantum yield at limiting light intensities and impairment of light-saturated electron transport. In treated cotyledons both the Q (due to recombination of Q_A⁻ with S₂) and B (due to recombination of Q_B⁻ with S₂/S₃) band of thermoluminescence decreased by 50% suggesting a loss of active PSII reaction centers. In both the control and treated samples, the thermoluminescence yield of B band exhibited a periodicity of 4 suggesting normal functioning of the S states in centers that were still active. The low temperature (77 K) fluorescence emission spectra revealed that the F₆₉₅ band (that originates in CP-47) increased probably due to reduced energy transfer from the CP47 to the reaction center. These demonstrated an overall damage to the PSI and PSII reaction centers by ¹O₂ produced in response to photosensitization reaction of protoporphyrin IX in AF-Na-treated cucumber seedlings.     

Chlorophyll fluorescence phenomena in chloroplasts on subnanosecond time-scales probed by picosecond pulse pairs

Fluorescence enhancement phenomena and quenching by exciton-exciton annihilation on subnanosecond and nanosecond time-scales were investigated in spinach chloroplasts utilizing picosecond laser pulse pairs (530 nm, 30 ps wide) of equal intensity, spaced apart in time by variable delays of Δt = 0−6 ns. This new method was devised to study the effect of pulse energies (1·10¹⁰–2·10¹⁵ photons per cm²) on the overall fluorescence yield in order to deduce the degree of correlation between the two pulses as a function of Δt. In the case of open reaction centers (F₀ state) in Photosystem II (PS II), it is shown that the quenching effect of excitons generated by the first pulse on the fluorescence yield of the second pulse diminishes with increasing Δt with a characteristic decorrelation time of 140 ± 60 ps. This effect is attributed to either (1) the decay of mobile excitons in the light-harvesting antenna pigment bed as these excitons migrate towards the PS II reaction centers and the associated smaller core antenna pigment pools, or (2) the decay of a quenching state of the reaction center (and/or core antenna) which appears following a rapid (less than 140 ps) trapping of the excitons initially created in the antenna pigment bed. The absence of a significant decay component of exciton quenchers with a lifetime comparable to the 300–600 ps intermediate phase of fluorescence decay kinetics suggests that this phase, although contributing to more than half of the integrated fluorescence emission signal, is not caused by freely mobile exitons migrating in a lake of pigments, but originates instead from smaller pigment pools to which the excitons have migrated. It is proposed that bimolecular exciton-exciton annihilation in these smaller domains dominates annihilation in the larger antenna pigment bed. In the case of closed reaction centers (F_max state), the decorrelation time between the two pulses is increased to 400 ± 100 ps, which is also attributed to either a mobile exciton component or to the decay of a quenching state of the reaction center. At low pulse intensities (below approx. 2 · 10¹² photons per cm²) anomalous fluorescence enhancement effects are noted, which are clearly linked to the existence of initially open PS II reaction centers. These enhancement effects are different from the well-known fluorescence induction phenomena which occur on longer time-scales, and are tentatively attributed to variations in the quenching efficiencies of transitory photochemical states of PS II reaction centers.     

Photoinhibition of carotenoidless reaction centers from Rhodobacter sphaeroides by visible light. Effects on protein structure and electron transport

Inhibition of electron transport and damage to the protein subunits by visible light has been studied in isolated reaction centers of the non-sulfur purple bacterium Rhodobacter sphaeroides. Illumination by 1100 μEm⁻² s⁻¹ light induced only a slight effect in wild type, carotenoid containing 2.4.1. reaction centers. In contrast, illumination of reaction centers isolated from the carotenoidless R26 strain resulted in the inhibition of charge separation as detected by the loss of the initial amplitude of absorbance change at 430 nm arising from the P⁺Q_B ⁻ → PQ_B recombination. In addition to this effect, the L, M and H protein subunits of the R26 reaction center were damaged as shown by their loss on Coomassie stained gels, which was however not accompanied by specific degradation products. Both the loss of photochemical activity and of protein subunits were suppressed in the absence of oxygen. By applying EPR spin trapping with 2,2,6,6-tetramethylpiperidine we could detect light-induced generation of singlet oxygen in the R26, but not in the 2.4.1. reaction centers. Moreover, artificial generation of singlet oxygen, also led to the loss of the L, M and H subunits. Our results provide evidence for the common hypothesis that strong illumination by visible light damages the carotenoidless reaction center via formation of singlet oxygen. This mechanism most likely proceeds through the interaction of the triplet state of reaction center chlorophyll with the ground state triplet oxygen in a similar way as occurs in Photosystem II. This revised version was published online in August 2006 with corrections to the Cover Date.     

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.     

Magnetic field effects on radical pair intermediates in bacterial photosynthesis

We have investigated the effects of magnetic fields on the formation and decay of excited states in the photochemical reaction centers of Rhodopseudomonas sphaeroides. In chemically reduced reaction centers, a magnetic field decreases the fraction of the transient state P^F that decays by way of the bacteriochlorophyll triplet state P^R. At room temperature, a 2-kG field decreases the quantum yield of P^R by about 40%. In carotenoid-containing reaction centers, the yield of the carotenoid triplet state which forms via P^R is reduced similarly. The effect of the field depends monotonically on field-strength, saturating at about 1 kG. The effect decreases at lower temperatures, when the yield of P^R is higher. Magnetic fields do not significantly affect the formation of the triplet state of bacteriochlorophyll in vitro, the photooxidation of P-870 in reaction centers at moderate redox potential, or the decay kinetics of states P^F and P^R.The effects of magnetic fields support the view that state P^F is a radical pair which is born in a singlet state but undergoes a rapid transformation into a mixture of singlet and triplet states. A simple kinetic model can account for the effects of the field and relate them to the temperature dependence of the yield of P^R.     

Effects of hydroxylamine and silicomolybdate on the decay in delayed light emission in the 6–100 μs range after a single 10 ns flash in pea thylakoids

Measurements are reported on μs delayed light emission, following a single 10 ns excitation flash, in Alaska pea thylakoids treated with hydroxylamine (NH₂OH) or with silicomolybdate.

1. In thylakoids treated with 2 mM NH₂OH in the light, or in the dark, the quantum yield of delayed light emission is considerably enhanced. A 10 μs lifetime component of delayed light emission is not significantly changed, whereas a 50–70 μs lifetime component is increased. MnCl₂ and diphenylcarbazide are unable to reverse the above effects of NH₂OH treatment. Thus Mn²⁺ and diphenylcarbazide must not donate electrons directly to reaction center II but on the oxygen-evolution side of the NH₂OH block.
2. When the closed form of photosystem II reaction centers (P₆₈₀Q^-), where P₆₈₀ is the reaction center chlorophyll and Q is a ‘stable’ electron acceptor, is generated by preillumination of NH₂OH-treated thylakoids with diuron present, the μs delayed light emission is inhibited, but a low level residual delayed light emission remains. Possible origins of this emission are discussed. It is believed that the best explanation for residual DLE is the existence of another acceptor besides Q that partakes in charge separation and rapid dissipative recombination when the reaction center is in the P₆₈₀Q^- state.
3. The quantum yield of delayed light emission from ‘closed’ reaction centers (P₆₈₀ ⁺Q^-) that have all charge stabilization reactions (i.e., flow of electrons to P₆₈₀ ⁺ and out of Q^-) blocked by NH₂OH treatment and addition of diuron is 1.1×10^-3 for components measured in a range from 6 to 400 μs and extrapolated to zero time.
4. The addition of silicomolybdate, which accepts electron from Q^-, causes delayed light emission in the μs range to be greatly inhibited.