Magnetophotoselection of the triplet state of reaction centers from Rhodopseudomonas sphaeroides R-26

Reaction centers of the photosynthetic bacterium Rhodopseudomonas sphaeroides R-26, give rise to large triplet state EPR signals upon illumination at low temperature (11 K). Utilizing monochromatic polarized light to generate the EPR spectra (magnetophotoselection) we have shown that the intensities of the observed triplet signals are strongly dependent upon the wavelength and polarization direction of the excitation. These data can be used to calculate the orientations of the excited transition moments with respect to each other and with respect to the triplet state principal magnetic axes system. Our quantitative approach is to follow the procedure outlined in a previous publication (Frank, H.A., Friesner, R., Nairn, J.A., Dismukes, G.C. and Sauer, K. (1979) Biochim. Biophys. Acta 547, 484–501) where computer simulations of the observed triplet state spectra were employed.The results presented in the present work indicate that the transition moment at 870 nm which is associated with the bacteriochlorophyll ‘special pair’ lies almost entirely along one of the principal magnetic axes of the triplet state. Also, the 870 nm transition moment makes an angle of approx. 60° with the 546 nm transition moment which is associated with a bacteriopheophytin. This latter result is in agreement with previous photoselection studies on the same bacterial species (Vermeglio, A., Breton, J., Paillotin, G. and Cogdell, R. (1978) Biochim. Biophys. Acta 501, 514–530).     

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.     

Nanosecond fluorescence from isolated photosynthetic reaction centers of Rhodopseudomonas sphaeroides

The time-course of fluorescence from reaction centers isolated from Rhodopseudomonas sphaeroides was measured using single-photon counting techniques. When electron transfer is blocked by the reduction of the electron-accepting quinones, reaction centers exhibit a relatively long-lived (delayed) fluorescence due to back reactions that regenerate the excited state (P*) from the transient radical-pair state, P^F. The delayed fluorescence can be resolved into three components, with lifetimes of 0.7, 3.2 and 11 ns at 295 K. The slowest component decays with the same time-constant as the absorbance changes due to P^F, and it depends on both temperature and magnetic fields in the same way that the absorbance changes do. The time-constants for the two faster components of delayed fluorescence are essentially independent of temperature and magnetic fields. The fluorescence also includes a very fast (prompt) component that is similar in amplitude to that obtained from unreduced reaction centers. The prompt fluorescence presumably is emitted mainly during the period before the initial charge-transfer reaction creates P^F from P*. From the amplitudes of the prompt and delayed fluorescence, we calculate an initial standard free-energy difference between P* and P^F of about 0.16 eV at 295 K, and 0.05 eV at 80 K, depending somewhat on the properties of the solvent. The multiphasic decay of the delayed fluorescence is interpreted in terms of relaxations in the free energy of P^F with time, totalling about 0.05 eV at 295 K, possibly resulting from nuclear movements in the electron-carriers or the protein.     

Binding of carotenoids on reaction centers from Rhodopseudomonas sphaeroides R 26

The carotenoid-less reaction centers isolated from Rhodopseudomonas sphaeroides (strain R 26) bind pure all-trans spheroidene as well as spheroidenone in a nearly 1:1 molar ratio with respect to P-870. Neither β-carotene nor spirilloxanthin, both absent from wild-type Rps. sphaeroides, could be bound in appreciable amounts. Resonance Raman spectra of the carotenoidreaction center complex indicate that the carotenoid is bound as a cis isomer, its conformation being very close, although probably not identical, to that assumed by the carotenoid in the wild-type reaction centers. The electronic absorption spectra of the carotenoid-reaction center complexes are in good agreement with such a interpretation. When bound to the R 26 reaction centers, spheroidene displays light-induced absorbance changes identical in peak wavelengths and comparable in amplitudes to those observed in the wild-type reaction centers. Thus the binding of the carotenoid to the R 26 reaction centers most likely occurs at the same proteic site as in the wild-type reaction centers. This site shows selectivity towards the nature of carotenoids, and has the same sterical requirement as in the wild type, leading to the observed all-trans to cis isomerisation.     

Hexane-solubilised reaction centre proteolipid complexes of Rhodopseudomonas sphaeroides

Reaction centres from Rhodopseudomonas sphaeroides, strain R-26, have been solubilised in hexane by the use of phospholipids and cations. Two procedures have been developed: (I) a two-step technique involving the formation of detergent-free proteoliposomes from detergent solubilised reaction centres and phospholipids and mixing these with hexane in the presence of cations; (II) directly sonicating detergent-solubilised reaction centres with phosopholipids before mixing with hexane and cations.The yield of the extracted complex varied with the ratios of protein, phospholipid and cations, species of phospholipid, and sonication time. The spectral characteristics of the complex in the organic phase were similar to those of detergent-solubilised reaction centres. The stability of the reaction centres appeared to be dependent on the presence of phospholipid and water in the hexane. The usefulness of the hexane solution as a model membrane system is discussed and its possible future applications are considered.     

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.     

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.     

Size and shape of detergent-solubilized photochemical reaction centers from two strains of Rhodopseudomonas sphaeroides. A solution X-ray scattering study

Solubilized reaction centers purified from Rhodopseudomonas sphaeroides (wild type and R26 strains) were studied in a nondenaturing detergent, dodecyldimethylamine N-oxide, by solution X-ray scattering. Some thermodynamic parameters were also obtained by coupling the results of this study with sedimentation equilibrium data previously obtained (Rivas, E., Reiss-Husson, F and le Maire, M. (1980) Biochemistry 19, 2943–2950). The particle weight of both types of reaction centers was found to be about 160 000 Da, corresponding to a protein molecular weight close to 90 000. Both hydrodynamic and solution X-ray scattering experiments suggest that the complexes have a globular shape, with a maximal chord of about 90 Å as indicated by the autocorrelation function. This maximal dimension is probably created by the binding of detergent to the solubilized complex. The approach followed in this study to investigate the shape of detergent-protein complexes involved a comparison of the Stokes' radii and the radii of gyration of various proteins.     

On the mechanism of photosynthetic electron transfer in Rhodopseudomonas capsulata and Rhodopseudomonas sphaeroides

(1) Current models for the mechanism of cyclic electron transport in Rhodopseudomonas sphaeroides and Rhodopseudomonas capsulata have been investigated by observing the kinetics of electron transport in the presence of inhibitors, or in photosynthetically incompetent mutant strains. (2) In addition to its well-characterized effect on the Rieske-type iron sulfur center, 5-(n-undecyl)-6-hydroxy-4,7-dioxobenzothiazole (UHDBT) inhibits both cytochrome b₅₀ and cytochrome b_?90 reduction induced by flash excitation in Rps. sphaeroides and Rps. capsulata. The concentration dependency of the inhibition in the presence of antimycin (approx. 2.7 mol UHDBT/mol reaction center for 50% inhibition of extent) is very similar to that of its inhibition of the antimycin-insensitive phase of ferricytochrome c re-reduction. UHDBT did not inhibit electron transfer between the reduced primary acceptor ubiquinone (Q^?_I) and the secondary acceptor ubiquinone (Q_II) of the reaction center acceptor complex. A mutant of Rps. capsulata, strain R126, lacked both the UHDBT and antimycin-sensitive phases of cytochrome c re-reduction, and ferricytochrome b₅₀ reduction on flash excitation. (3) In the presence of antimycin, the initial rate of cytochrome b₅₀ reduction increased about 10-fold as the E_h(7.0) was lowered below 180 mV. A plot of the rate at the fastest point in each trace against redox potential resembles the Nernst plot for a two-electron carrier with E_m(7.0) ≈ 125 ± 15 mV. Following flash excitation there was a lag of 100–500 μs before cytochrome b₅₀ reduction began. However, there was a considerably longer lag before significant reduction of cytochrome c by the antimycin-sensitive pathway occurred. (4) The herbicide ametryne inhibited electron transfer between Q^?_I and Q_II. It was an effective inhibitor of cytochrome b₅₀ photoreduction at E_h(7.0) 390 mV, but not at E_h(7.0) 100 mV. At the latter E_h, low concentrations of ametryne inhibited turnover after one flash in only half of the photochemical reaction centers. By analogy with the response to o-phenanthroline, it is suggested that ametryne is ineffective at inhibiting electron transfer from Q^?_I to the secondary acceptor ubiquinone when the latter is reduced to the semiquinone form before excitation. (5) At E_h(7.0) > 200 mV, antimycin had a marked effect on the cytochrome b₅₀ reduction-oxidation kinetics but not on the cytochrome c and reaction center changes or the slow phase III of the electrochromic carotenoid change on a 10-ms time scale. This observation appears to rule out a mechanism in which cytochrome b₅₀ oxidation is obligatorily and kinetically linked to the antimycin-sensitive phase of cytochrome c reduction in a reaction involving transmembrane charge transfer at high E_h values. However, at lower redox potentials, cytochrome b₅₀ oxidation is more rapid, and may be linked to the antimycin-sensitive reduction of cytochrome c. (6) It is concluded that neither a simple linear scheme nor a simple Q-cycle model can account adequately for all the observations. Future models will have to take account of a possible heterogeneity of redox chains resulting from the two-electron gate at the level of the secondary quinone, and of the involvement of cytochrome b_?90 in the rapid reactions of the cyclic electron transfer chain     

Magnetic field affects the fluorescence yield in reaction center preparations from Rhodopseudomonas sphaeroides R-26

Purified photochemical reaction centers from Rhodopseudomonas sphaeroides R-26 were reduced with Na₂S₂O₄ so as to block their photochemical electron-transfer reactions. The magnetic field induced an increase in the emission yield. Our results support the hypothesis that under these conditions, charge recombination in the singlet radical pair composed of the oxidized primary donor and reduced primary acceptor predominantly generates the excited singlet state of the reaction center bacteriochlorophyll.The maximum relative fluorescence change and the value of the magnetic field at which half-saturation of the effect is achieved ($\text{B}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$) at room temperature are 5.5% and 75 G, respectively. For the whole cells of Rps. sphaeroides R-26 these parameters are 1.2% and 120 G.The relative fluorescence change at 600 G, $\text{ΔF}\text{F(600)}$, and $\text{B}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$ are studied as functions of temperature. The temperature dependencies of $\text{ΔF}\text{F(600)}$ for reaction centers and whole cells of Rps. sphaeroides R-26 are qualitatively the same, with the maximum effect (8% for reaction centers) occurring at 230 K. However, the $\text{B}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$ curves for the two preparations are different.     

Resolved difference spectra of redox centers involved in photosynthetic electron flow in Rhodopseudomonas capsulata and rhodopseudomonas sphaeroides

1. In Rhodopseudomonas sphaeroides the Q_x absorption band of the reaction center bacteriochlorophyll dimer which bleaches on photo-oxidation is both blue-shifted and has an increased extinction coefficient on solubilisation of the chromatophore membrane with lauryldimethylamine-N-oxide. These effects may be attributable in part to the particle flattening effect.2. The difference spectrum of photo-oxidisable c type cytochrome in the chromatophore was found to have a slightly variable peak position in the α-band (λ_max at 551–551.25 nm); this position was always red-shifted in comparison to that of isolated cytochrome c₂ (λ_max at 549.5 ± 0.5 nm). The shift in wavelength maximum was not due to association with the reaction center protein. A possible heterogeneity in the c-type cytochromes of chromatophores is discussed.3. Flash-induced difference spectra attributed to cytochrome b were resolved at several different redox potentials and in the presence and absence of antimycin. Under most conditions, one major component, cytochrome b₅₀ appeared to be involved. However, in some circumstances, reduction of a component with the spectral characteristics of cytochrome b_?90 was observed.4. Difference spectra attributed to (BChl)₂, Q^?_II, c type cytochrome and cytochrome b₅₀ were resolved in the Soret region for Rhodopseudomonas capsulata.5. A computer-linked kinetic spectrophotometer for obtaining automatically the difference spectra of components functioning in photosynthetic electron transfer chains is described. The system incorporates a novel method for automatically adjusting and holding the photomultiplier supply voltage.     

Linear dichroism of light harvesting bacteriochlorophyll proteins from Rhodopseudomonas sphaeroides in stretched polyvinyl alcohol films

Light-harvesting bacteriochlorophyll-protein complexes from Rhodopseudomonas sphaeroides 2.4.1 and R-26 mutant are solubilized in sodium dodecyl sulfate and imbedded in polyvinyl alcohol. Stretching induces orientation, and the linear dichroism of visible and near infrared absorption is analyzed. Based on a simple model, angles between the particle axis and the transition dipole moments are found. In the near infrared absorption band of the R-26 light-harvesting protein the dichroic ratio varies from 1.30 to 1.57. Using the absorption curves the band is resolved into two exciton components. In the visible absorption band the dichroic ratio has a constant value of 0.43 for the R-26 protein but varies with wavelength for the wild type light-harvesting protein. This variation is attributed to an additional bacteriochlorophyll not present in the R-26 protein.     

The orientations of reaction center transition moments in the chromatophore membrane of Rhodopseudomonas sphaeroides, based on new linear dichroism and photoselection measurements

Chromatophore membranes from Rhodopseudomonas sphaeroides were oriented by drying suspensions on the surfaces of glass slides. Polarized spectra of light-induced absorption changes were obtained between 500 and 1000 nm. As observed earlier, these spectra showed negative bands, reflecting photooxidation of the bacteriochlorophyll ‘special pair’ in the reaction centers, centered near 870, 810, 630 and 600 nm. These bands have been designated BY₁, BY₂, BX₁ and BX₂, respectively, corresponding to two Q_y transitions and two Q_x transitions of the dimeric special pair. We found the BY₁ and BX₁ transition moments to be parallel (within 20°) to the plane of the membrane, whereas the BX₂ moment makes an angle of 55–63° with the plane.Using the photoselection technique we found that the angle between the BY₁ and BX₁ transition moments is 30°, while that between BY₁ and BX₂ is 75°. The BX₁ and BX₂ moments were found to be orthogonal, consistent with the prediction of molecular exciton theory for a dimer.By combining these data, we have calculated the orientations of the transition moments of the bacteriochlorophyll dimer in spherical polar coordinates, with the pole of the coordinate system normal to the plane of the membrane. The orientations of the Q_y and Q_x transition moments of the two bacteriopheophytin molecules in the reaction center were also computed in this coordinate system by transforming the data reported by Clayton, C.N., Rafferty, R.K. and Vermeglio, A. ((1979) Biochim. Biophys. Acta 545, 58–68). We have derived the transformation equations for two polar coordinate systems: in one, the pole is an axis of symmetry as defined by the orientations of purified reaction centers in stretched gelatin films (Rafferty, C.N. and Clayton, R.K. (1979) Biochim. Biophys. Acta 545, 106–121). In the other, the pole is normal to the plane of the chromatophore membrane. These two polar axes are approximately orthogonal.     

High-resolution optical absorption-difference spectra of the triplet state of the primary donor in isolated reaction centers of the photosynthetic bacteria Rhodopseudomonas sphaeroides R-26 and Rhodopseudomonas viridis measured with optically detected magnetic resonance at 1.2 K

We have recorded triplet optical absorption-difference spectra of the reaction center triplet state of isolated reaction centers from Rhodopseudomonas sphaeroides R-26 and Rps. viridis with optical absorption-detected electron spin resonance in zero magnetic field (ADMR) at 1.2 K. This technique is one to two orders of magnitude more sensitive than conventional flash absorption spectroscopy, and consequently allows a much higher spectral resolution. Besides the relatively broad bleachings and appearances found previously (see, e.g., Shuvalov V.A. and Parson W.W. (1981) Biochim. Biophys. Acta 638, 50–59) we have found strong, sharp oscillations in the wavelength regions 790–830 nm (Rps. sphaeroides) and 810–890 nm (Rps. viridis). For Rps. viridis these features are resolved into two band shifts (a blue shift at about 830 nm and a red shift at about 855 nm) and a strong, narrow absorption band at 838 nm. For Rps. sphaeroides R-26 the features are resolved into a red shift at about 810 nm and a strong absorption band at 807 nm. We conclude that the appearance of the absorption bands at 807 and 838 nm, respectively, is due to monomeric bacteriochlorophyll. Apparently, the exciton interaction between the pigments constituting the primary donor is much weaker in the triplet state than in the singlet state, and at low temperature the triplet is localized on one of the bacteriochlorophylls on an optical time scale. The fact that for Rps. sphaeroides the strong band shift and the monomeric band found at 1.2 K are absent at 293 K and very weak at 77 K indicates that these features are strongly temperature dependent. It seems, therefore, premature to ascribe the temperature dependence between 293 and 77 K of the intensity of the triplet absorption-difference spectrum at 810 nm (solely) to a delocalization of the triplet state on one of the accessory bacteriochlorophyll pigments.     

The kinetics of flash-induced electron flow in bacteriochlorophyll-less membranes of Rhodopseudomonas sphaeroides reconstituted with reaction centres

Membranes isolated from aerobically grown mutants 01 and PM8bg II-15 of Rhodopseudomonas sphaeroides lack reaction centres. Incorporation of purified reaction centres into these membranes can be achieved by mixing the protein and membranes in 1% sodium cholate with added soybean phospholipid and removing the cholate by dialysis.The kinetics of light-stimulated electron flow in these reconstituted membranes have been examined and compared with those observed in chromatophore membranes isolated from photosynthetically grown R. sphaeroides. Following a single saturating flash, reconstituted reaction centres become photo-oxidised, and about 60% are re-reduced within about 200 ms by cytochrome c2 in the 01 membrane. Cytochrome c2 photo-oxidation is biphasic, the half-time of the first fase being faster than 20 μs. The second phase is variable and can be as slow as 60 ms. A cytochrome b in the membrane becomes photoreduced with a half-time of 27 ms. Electron flow between cytochromes b and c2 is slow and appears only partially sensitive to antimycin A.Using membranes from the reaction centre-less mutant PM8bg II-15 similar reconstitution measurements were performed. The resulting kinetic measurements showed that fast cytochrome b photoreduction and cytochrome c2 photo-oxidation occurred.The absorbance change at 560 minus 570 nm induced by steady-state illumination of 01 membranes reconstituted with reaction centres was measured at a range of ambient potentials; the reaction was abolished at oxidation-reduction potentials below 0 mV. The change was approximately halved at +50 mV, indicating that cytochrome b₊₅₀ is the recipient of electrons from the reconstituted reaction centres.     

Spectroscopic and kinetic properties of the transient intermediate acceptor in reaction centers of Rhodopseudomonas sphaeroides.

The photoreductive trapping of the transient, intermediate acceptor, I-, in purified reaction centers of Rhodopseudomonas sphaeroides R-26 was investigated for different external conditions. The optical spectrum of I- was found to be similar to that reported for other systems by Shuvalov and Klimov ((1976) Biochim. Biophys. Acta 400, 587--599) and Tiede et al. (P.M. Tiede, R.C. Prince, G.H. Reed and P.L. Dutton (1976) FEBS Lett. 65, 301--304). The optical changes of I- showed characteristics of both bacteriopheophytin (e.g. bleaching at 762, 542 nm and red shift at 400 nm) and bacteriochlorophyll (bleaching at 802 and 590 nm). Two types of EPR signals of I- were observed: one was a narrow singlet at g = 2.0035, deltaH = 13.5 G, the other a doublet with a splitting of 60 G centered around g = 2.00, which was only seen after short illumination times in reaction centers reconstituted with menaquinone. The optical and EPR kinetics of I- on illumination in the presence of reduced cytochrome c and dithionite strongly support the following three-step scheme in which the doublet EPR signal is due to the unstable state DI-Q-Fe2+ and the singlet EPR signal is due to DI-Q2-Fe2+. : formula: (see text), where D is the primary donor (BChl)2+. The above model was supported by the following observations: (1) During the first illumination, sigmoidal kinetics of the formation of I- was observed. This is a direct consequence of the three-sequential reactions. (2) During the second and subsequent illuminations first-order (exponential) kinetics were observed for the formation of I-. This is due to the dark decay, k4, to the state DIQ2-Fe2+ formed after the first illumination. (3) Removal of the quinone resulted in first-order kinetics. In this case, only the first step, k1, is operative. (4) The observation of the doublet signal in reaction centers containing menaquinone but not ubiquinone is explained by the longer lifetime of the doublet species I-(Q-Fe2%) in reaction centers containing menaquinone. The value of tau2 was determined from kinetic measurements to be 0.01 s for ubiquinone and 4 s for menaquinone (T = 20 degrees C). The temperature and pH dependence of the dark electron transfer reaction I-(Q-Fe2+) yields I(Q2-Fe2+) was studied in detail. The activation energy for this process was found to be 0.42 eV for reaction centers containing ubiquinone and 0.67 eV for reaction centers with menaquinone. The activation energy and the doublet splitting were used to calculate the rate of electron transfer from I- to MQ-Fe2+ using Hopfield's theory for thermally activated electron tunneling. The calculated rate agrees well with the experimentally determined rate which provides support for electron tunneling as the mechanism for electron transfer in this reaction. Using the EPR doublet splitting and the activation energy for electron transfer, the tunneling matrix element was calculated to be 10(-3) eV. From this value the distance between I- and MQ- was estimated to be 7.5--10 A.     

The interaction of the reaction center secondary quinone with the ubiquinone-cytochrome c2 oxidoreductase in Rhodopseudomonas sphaeroides chromatophores

(1) Two populations of reaction centers in the chromatophore membrane can be distinguished under some conditions of initial redox poise (300 mV < E_h < 400 mV): those which transfer a reducing equivalent after the first flash from the secondary quinone (Q_II) of the reaction center to cytochrome b of the ubiquinone-cytochrome c₂ oxidoreductase; and those which retain the reducing equivalent on Q^?_II until a second flash is given. These two populations do not exchange on a time scale of tens of seconds. (2) At redox potentials higher than 400 mV, Q^?_II generated after the first flash is no longer able to reduce cytochrome b-560 even in those reaction centers associated with an oxidoreductase. Under these conditions, doubly reduced Q_II generated by a second flash is required for cytochrome b reduction, so that the Q_II effectively functions as a two-electron gate into the oxidoreductase at these high potentials. (3) At redox potentials below 300 mV, although the two populations of Q_II are no longer distinguishable, cytochrome b reduction is still dependent on only part of the reaction center population. (4) Proton binding does not oscillate under any condition tested.     

Structural and kinetic properties of Rhodobacter sphaeroides photosynthetic reaction centers containing exclusively Zn-coordinated bacteriochlorophyll as bacteriochlorin cofactors

The Zn-BChl-containing reaction center (RC) produced in a bchD (magnesium chelatase) mutant of Rhodobacter sphaeroides assembles with six Zn-bacteriochlorophylls (Zn-BChls) in place of four Mg-containing bacteriochlorophylls (BChls) and two bacteriopheophytins (BPhes). This protein presents unique opportunities for studying biological electron transfer, as Zn-containing chlorins can exist in 4-, 5-, and (theoretically) 6-coordinate states within the RC. In this paper, the electron transfer perturbations attributed exclusively to coordination state effects are separated from those attributed to the presence, absence, or type of metal in the bacteriochlorin at the H_A pocket of the RC. The presence of a 4-coordinate Zn^2 + ion in the H_A bacteriochlorin instead of BPhe results in a small decrease in the rates of the P* → P⁺H_A⁻ → P⁺Q_A⁻ electron transfer, and the charge separation yield is not greatly perturbed; however coordination of the Zn^2 + by a fifth ligand provided by a histidine residue results in a larger rate decrease and yield loss. We also report the first crystal structure of a Zn-BChl-containing RC, confirming that the H_A Zn-BChl was either 4- or 5-coordinate in the two types of Zn-BChl-containing RCs studied here. Interestingly, a large degree of disorder, in combination with a relatively weak anomalous difference electron density was found in the H_B pocket. These data, in combination with spectroscopic results, indicate partial occupancy of this binding pocket. These findings provide insights into the use of BPhe as the bacteriochlorin pigment of choice at H_A in both BChl- and Zn-BChl-containing RCs found in nature.     

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.     

Fast oxidation of the primary electron acceptor under anaerobic conditions requires the organization of the photosynthetic chain of Rhodobacter sphaeroides in supercomplexes

The kinetics of reoxidation of the primary acceptor Q_a has been followed by measuring the changes in the fluorescence yield induced by a series of saturating flashes in intact cells of Rhodobacter sphaeroides in anaerobic conditions. At 0 °C, about half of Q_a⁻ is reoxidized in about 200 ms while reoxidation of the remaining fraction is completed in several seconds to minutes. The fast phase is associated with the transfer of ubiquinone formed at site Q_o of the cytochrome bc₁ complex while the slowest phase is associated with the diffusion of ubiquinone present in the membrane prior to the flash excitation. The biphasic kinetics of Q_a⁻ oxidation is interpreted assuming that the electron chain is organized in supercomplexes that associate two RCs and one cyt bc₁ complex, which allows a fast transfer of quinone formed at the level of cyt bc₁ complex to the RCs. In agreement with this model, the fast phase of Q_a⁻ reoxidation is inhibited by myxothiazol, a specific inhibitor of cyt bc₁. The PufX-deleted mutant displays only the slowest phase of Q_a⁻ oxidation; it is interpreted by the lack of supramolecular organization of the photosynthetic chain that leads to a larger average distance between cyt bc₁ and RCs.