A picosecond-absorption study on bacteriochlorophyll excitation,trapping and primary-charge separation in chromatophores of Rhodospirillum rubrum

Absorbance-difference spectra and kinetics of absorbance changes were measured of chromatophores of Rhodospirillum rubrum by means of picosecond-absorption spectroscopy. A 35 ps excitation pulse at 532 nm produced absorbance changes due to the formation and decay of excited states of antenna pigments (Nuijs, A.M., Van Grondelle, R., Joppe, H.L.P., Van Bochove, A.C. and Duysens, L.N.M. (1985) Biochim. Biophys. Acta 810, 94–105), and, when open reaction centers were present, also those due to charge separation and primary electron transport. At low excitation energy density the lifetime of singlet-excited antenna bacteriochlorophyll was 80 ± 10 ps when the reaction centers were initially open and 200–400 ps when the primary electron donor was oxidized. Under the former conditions photooxidation of the primary donor occurred with a time constant of 70 ± 10 ps. Reduction of an electron-acceptor complex in the reaction center, probably involving both bacteriochlorophyll and bacteriopheophytin, was observed. Reoxidation of this acceptor occurred with a time constant of 200–300 ps. When the ubiquinone acceptor was reduced chemically, the primary radical pair decayed by recombination with a time constant of about 4 ns at high flash-energy densities, and of about 10 ns at lower energy densities. This dependence of the lifetime of the radical pair on the flash intensity was explained in terms of quenching processes by carotenoid triplet states in the antenna, and indicated a standard free-energy difference between the radical pair and the singlet-excited state of antenna bacteriochlorophyll of about 160 meV.     

Study of the long-wavelength fluorescence band at 920 nm of isolated reaction centers of the photosynthetic bacterium Rhodopseudomonas spaeroides R-26 with fluorescence-detected magnetic resonance in zero field

The triplet state of isolated reaction centers of Rhodopseudomonas sphaeroides R-26 has been studied by fluorescence-detected electron spin resonance in zero magnetic field (FDMR) at 4.2 K. The sign of the FDMR resonance monitored at the long-wavelength fluorescence band is positive (fluorescence increase); this confirms the earlier interpretation (Hoff, A.J. and Gorter de Vries, H. (1978) Biochim. Biophys. Acta 503, 94–106) that the negative sign of the FDMR resonance of the reaction center triplet state in whole bacterial cells is caused by resonant transfer of the singlet excitations from the antenna pigments to the trap. By monitoring the FDMR response as a function of the wavelength of fluorescence, we have recorded microwave-induced fluorescence spectra. In addition to the positive microwave-induced fluorescence band peaking at 935 nm, at 905 nm a negative band was found. The resonant microwave frequencies for these two bands, i.e., the values of the zero-field splitting parameters |D| and |E| of the triplet state being monitored, were different, those of the 905 nm microwave-induced fluorescence band being identical to the resonant microwave frequencies measured with absorption-detected zero-field resonance (Den Blanken, H.J., Van der Zwet, G.P. and Hoff, A.J. (1982) Chem. Phys. Lett. 85, 335–338), a technique that monitors the bulk properties of the sample. From this result and its negative sign, we tentatively attribute the 905 nm microwave-induced fluorescence band to a small (possibly less than 1%) fraction of antenna bacteriochlorophylls that are in close contact with the trap. The positive 935 nm microwave-induced fluorescence band with resonant microwave frequencies deviating from the bulk material is ascribed to a minority of primary donor bacteriochlorophyll dimers, which have a higher than normal fluorescence yield because of a somewhat slower charge-separation reaction. Is it likely that practically all long-wavelength fluorescence of isolated reaction centers stems from such impaired reaction centers.     

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.     

Electron-spin resonance studies of the bound iron-sulfur centers in Photosystem I. II. Correlation of P-700 triplet production with urea/ferricyanide inactivation of the iron-sulfur clusters

Photosystem I charge separation in a subchloroplast particle isolated from spinach was investigated by electron spin resonance (ESR) spectroscopy following graduated inactivation of the bound iron-sulfur centers by urea-ferricyanide treatment. Previous work demonstrated a differential decrease in iron-sulfur centers A, B and X which indicated that center X serves as a branch point for parallel electron flow through centers A and B (Golbeck, J.H. and Warden, J.T. (1982) Biochim. Biophys. Acta 681, 77-84). We now show that during inactivation the disappearance of iron-sulfur centers A, B, and X correlates with the appearance of a spin-polarized triplet ESR signal with [D] = 279 X 10(-4) cm-1 and [E] = 39 X 10(-4) cm-1. The triplet resonances titrate with a midpoint potential of +380 +/- 10 mV. Illumination of the inactivated particles results in the generation of an asymmetric ESR signal with g = 2.0031 and delta Hpp = 1.0 mT. Deconvolution of the P-700+ contribution to this composite resonance reveals the spectrum of the putative primary acceptor species A0, which is characterized by g = 2.0033 +/- 0.0004 and delta Hpp = 1.0 +/- 0.2 mT. The data presented in this report do not substantiate the participation of the electron acceptor A1 in PS I electron transport, following destruction of the iron-sulfur cluster corresponding to center X. We suggest that A1 is closely associated with center X and that this component is decoupled from the electron-transport path upon destruction of center X. The inability to photoreduce A1 in reaction centers lacking a functional center X may result from alteration of the reaction center tertiary structure by the urea-ferricyanide treatment or from displacement of A1 from its binding site.     

Supramolecular organization of the photosynthetic chain in chromatophores and cells of Rhodobacter sphaeroides

Flash-induced kinetics of the membrane potential increase related to electron transfer within the cytochrome (cyt) b/c₁ complex (Phase III) and that of cyt c₁+c₂ reduction have been measured as a function of myxothiazol concentration in isolated chromatophores and whole cells of Rhodobacter sphaeroides. Upon addition of nonsaturating concentrations of myxothiazol, kinetics of Phase III display two phases, Phase IIIa and Phase IIIb. The amplitude of Phase IIIa, completed in about 10 ms, is proportional to the fraction of non-inhibited cyt b/c₁ complexes, while its half-time is independent of the myxothiazol concentration. A fast cyt c₁+c₂ reduction phase is correlated to Phase IIIa. These experiments demonstrate that, in a range of time of several ms, diffusion of cyt c₂ is restricted to domains formed by a supercomplex including two reaction centers (RCs) and a single cyt b/c₁ complex, as proposed by Joliot et al. (Biochim Biophys Acta 975: 336–345, 1989). Phase IIIb, completed in about 100 ms, shows that positive charges or inhibitor molecules are exchanged between supercomplexes in this range of time. These exchanges occur within domains including 2 to 3 supercomplexes, i.e. in membrane domains smaller than a single chromatophore. These conclusions apply to both isolated chromatophores and whole cells.Abbreviations cyt cytochrome - MOPS 3-(N-morpholino)propane sulfonic acid - PMS phenazine methosulfate - P primary donor - Rb. Rhodobacter - RC reaction center     

Energy requirement for biosynthesis of DNA in Escherichia coli: Role of membrane-bound energy-transducing ATPase (coupling factor)

A mutant of Escherichia coli missing energy-transducing ATPase and known to be defective in a variety of membrane functions from earlier studies (Yamamoto, T. H., Mével-Ninio, M. and Valentine, R. C. (1973) Biochim. Biophys. Acta 314, 267–275; Thipayathasana, P. and Valentine, R. C. (1974) Biochim. Biophys. Acta 347, 464–468; Mével-Ninio, M. and Yamamoto, T. (1974) Biochim. Biophys. Acta 357, 63–66) has been found to be blocked for anaerobic DNA synthesis. The rate of anaerobic DNA synthesis in the mutant, measured as radioactive adenine incorporation into the alkali-resistant fraction of whole cells, is about 1/6 the rate of DNA synthesis in the wild type culture under similar conditions. Addition of NO₃^- or O₂ restores DNA biosynthesis in the mutant. The entry of radioactive adenine is not appreciably affected in the mutant by anaerobiosis. It is concluded that coupling factor plays a role in some step(s) of DNA biosynthesis.     

Magnetic field-induced increase of the yield of (bacterio)chlorophyll emission of some photosynthetic bacteria and of Chlorella vulgaris.

In photosynthetic bacteria, in which the iron-ubiquinone complex X is prereduced, a magnetic field induces an increase of the emmission yield, which is correlated with the decrease in reaction center triplet yield reported previously (Hoff, A.J., Rademaker, H., van Grondelle, R. and Duysens, L.N.M. (1977) Biochim. Biophys. Acta 460, 547--554). Our results support the hypothesis that under these conditions charge recombination of the oxidized primary donor and the reduced primary acceptor predominantly generates the excited singlet state of the reaction center bacteriochlorophyll. In Chlorella vulgaris and spinach chloroplasts, at 120 K, the magnetic field has an effect similar to that found in bacteria, which suggests that an intermediary electron acceptor between P-680 and Q is present in Photosystem II also.     

Orientation of chromophores in reaction centers of Rhodopseudomonas sphaeroides. Evidence for two absorption bands of the dimeric primary electron donor

Chromatophores from Rhodopseudomonas sphaeroides were oriented by allowing aqueous suspensions to dry on glass plates. Orientation of reaction center pigments was investigated by studying the linear dichroism of chromatophores in which the absorption by antenna bacteriochlorophyll had been attenuated through selective oxidation. Alternatively the light-induced absorbance changes, in the ranges 550–650 and 700–950 nm, were studied in untreated chromatophores. The long wave transition moment of reaction center bacteriochlorophyll (P-870) was found to be nearly parallel to the plane of the membrane, whereas the long wave transition moments of bacteriopheophytin are polarized out of this plane. For light-induced changes the linear dichroic ratios, defined as Δa_v/Δa_h, are nearly the same for untreated and for oxidized chromatophores. Typical values are 1.60 at 870 nm, 0.80 at 810 nm, 1.20 at 790 nm, 0.70 at 765 nm, 0.30 at 745 nm, and 0.50 at 600 nm. The different values for the absorbance decrease at 810 nm (0.80) and the increase at 790 nm (1.20) are incompatible with the hypothesis that these changes are due to the blue-shift of a single band. We propose that the decreases at 870 and 810 nm reflect bleaching of the two components of a bacteriochlorophyll dimer, the “special pair” that shares in the photochemical donation of a single electron. The increase at 790 nm then represents the appearance of a monomer band in place of the dimer spectrum, as a result of electron donation. This hypothesis is consistent with available data on circular dichroism. It is confirmed by the presence of a shoulder at 810 nm in the absorption spectrum of reaction centers at low temperature; this band disappears upon photooxidation of the reaction centers. For the changes near 760 nm, associated with bacteriopheophytin, the polarization and the shape of the “light-dark” difference spectrum (identical to the first derivative of the absorption spectrum) show that the 760 nm band undergoes a light-induced shift to greater wavelengths.     

Antenna and reaction-center processes upon picosecond-flash excitation of membranes of the green photosynthetic bacterium Chloroflexus aurantiacus

The formation and decay of antenna-excited states and the primary charge separation in membranes of the green photosynthetic bacterium Chloroflexus aurantiacus were studied by means of picosecond absorbance difference spectroscopy. After chemical oxidation of the primary electron donor, a 35 ps excitation pulse at 532 nm produced singlet- and triplet-excited states of carotenoid and of bacteriochlorophyll a. Excitation of bacteriochlorophyll a caused a bleaching of its Q_y absorption band and induced a blue shift of several neighboring bacteriochlorophyll molecules. The singlet-excited state decayed biphasically with lifetimes of about 200 ps and 1.2 ns. A decrease in the lifetime at increasing flash intensity was attributed to singlet-singlet annihilation. In the presence of active reaction centers also the primary-charge separation and secondary electron transfer were observed. The charge separation consisted of the transfer of an electron from the primary donor, P-865, to the primary-acceptor complex of bacteriopheophytin a and bacteriochlorophyll a. Electron transfer to a secondary acceptor occurred with a time constant of 400 ± 50 ps, which is about 30% longer than had been observed with isolated reaction centers (Kirmaier, C., Holten, D., Mancino, L.J. and Blankenship, R.E. (1984) Biochim. Biophys. Acta 765, 138–146). When this secondary acceptor was prereduced chemically, the lifetime of the primary radical pair increased to 10 ns or more.     

Singlet-triplet fusion in Rhodopseudomonas sphaeroides chromatophores. A probe of the organization of the photosynthetic apparatus

Chromatophores from various strains of Rhodopseudomonas sphaeroides were excited with laser flashes lasting about 20 ns. Fluorescence from the antenna bacteriochlorophyll of the photosynthetic apparatus was measured both during the laser flash, and during a weak Xe flash following the laser flash. Strong laser flashes caused severe quenching of the fluorescence, which could be correlated with the formation of triplet states of the antenna pigments. Triplet states of both BChl and carotenoids acted as quenchers, but bacteriochlorophyll triplets were the more effective of the two. In the double-flash experiments, the reciprocal of the fluorescence yield was proportional to the concentration of triplet quenchers remaining at the time of the second flash. This relationship indicates that singlet excitations can migrate over large domains in the antenna, rather than being restricted by boundaries separating individual reaction centers. Comparisons of chromatophores from different strains and from cells grown under different conditions showed that excitations are concentrated rapidly in the antenna complexes with the longest wavelength absorption bands (B870), and that the migration of excitations to trapping sites is relatively insensitive to the amount of antenna bacteriochlorophyll absorbing at shorter wavelengths (B800–B850). This suggests that the B870 complexes are organized in the membrane so as to interconnect many reaction centers, and that the B800–B850 complexes are arranged peripherally.     

Magnetic field-induced increase of the yield of (bacterio)chlorophyll emission of some photosynthetic bacteria and of Chlorella vulgaris

In photosynthetic bacteria, in which the iron-ubiquinone complex X is prereduced, a magnetic field induces an increase of the emission yield, which is correlated with the decrease in reaction center triplet yield reported previously (Hoff, A.J., Rademaker, H., van Grondelle, R. and Duysens, L.N.M. (1977) Biochim. Biophys. Acta 460, 547–554). Our results support the hypothesis that under these conditions charge recombination of the oxidized primary donor and the reduced primary acceptor predominantly generates the excited singlet state of the reaction center bacteriochlorophyll.In Chlorella vulgaris and spinach chloroplasts, at 120 K, the magnetic field has an effect similar to that found in bacteria, which suggests that an intermediary electron acceptor between P-680 and Q is present in Photosystem II also.     

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. Aso, the 870 nm transition moment makes an angle of approx. 60 degrees 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).     

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).     

Identification of the 120 μs phase in the decay of delayed fluorescence in spinach chloroplasts and subchloroplast particles as the intrinsic back reaction. The dependence of the level of this phase on the thylakoids internal pH

After a 500 μs laser flash a 120 μs phase in the decay of delayed fluorescence is visible under a variety of circumstances in spinach chloroplasts and subchloroplast particles enriched in Photosystem II prepared by means of digitonin. The level of this phase is high in the case of inhibition of oxygen evolution at the donor side of Photosystem II. Comparison with the results of Babcock and Sauer (1975) Biochim. Biophys. Acta 376, 329–344, indicates that their EPR signal II_f which they suppose to be due to Z⁺, the oxidized first secondary donor of Photosystem II, is well correlated with a large amplitude of our 120 μs phase. We explain our 120 μs phase by the intrinsic back reaction of the excited reaction center in the presence of Z⁺, as predicted by Van Gorkom and Donze (1973) Photochem. Photobiol. 17, 333–342. The redox state of Z⁺ is dependent on the internal pH of the thylakoids. The results on the effect of pH in the μs region are compared with those obtained in the ms region.     

Excited states and primary charge separation in the pigment system of the green photosynthetic bacterium Prosthecochloris aestuarii as studied by picosecond absorbance difference spectroscopy

Picosecond absorbance difference spectra at a number of delay times after a 35 ps excitation flash and kinetics of absorbance changes were measured of the membrane vesicle preparation Complex I from the photosynthetic green sulfur bacterium Prosthecochloris aestuarii. After chemical oxidation of the primary donor the excitation pulse produced singlet and triplet excited states of carotenoid and bacteriochlorophyll a. With active reaction centers present also the flash-induced primary charge separation and subsequent electron transfer were observed. The singlet excited state of the carotenoid, formed by direct excitation at 532 nm, is characterized by an absorbance band peaking at 590 nm. Its average lifetime was calculated to be about 1 ps. Excited singlet states of bacteriochlorophyll a were characterized by a bleaching of their ground state Q_y absorption bands. Singlet excited states, localized on the so-called core complex, were produced by energy transfer from excited carotenoid. Their lifetime was about 70 ps. A decay component of about 280 ps was ascribed to singlet excited bacteriochlorophyll a in the bacteriochlorophyll a protein. These singlet excitations were partly converted to the triplet state. With active reaction centers, oxidation of the primary donor, P-840, characterized by the bleaching of its Q_y and Q_x absorption bands, was observed. This oxidation was accompanied by a bleaching between 650 and 680 nm and an absorbance increase between 680 and 750 nm. These changes, presumably due to reduction of bacteriopheophytin c (Van Bochove, A.C., Swarthoff, T., Kingma, H., Hof, R.M., Van Grondelle, R., Duysens, L.N.M. and Amesz, J. (1984) Biochim. Biophys. Acta 764, 343–346), were attributed to the reduction of the primary electron acceptor. Electron transfer to a secondary acceptor occurred with a time-constant of 550 ± 50 ps. Since no absorbance changes due to reduction of this acceptor were observed in the red or infrared region, we tentatively assume that this acceptor is an iron-sulfur center.     

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.     

Thermoluminescence properties of the isolated photosystem two reaction centre

Formation of thermoluminescence signals is characteristics of energy- and charge storage in Photosystem II. In isolated D1/D2/cytochrome b-559 Photosystem II reaction centre preparation four thermoluminescence components were found. These appear at -180 (Z band), between -80 and -50 (Z_v band), at -30 and at +35°C. The Z band arises from pigment molecules but not correlated with photosynthetic activity. The Z_v and -30°C bands arise from the recombination of charge pairs stabilized in the Photosystem II reaction centre complex. The +35°C band probably corresponds to the artefact glow peak resulting from a pigment-protein-detergent interaction in subchloroplast preparations (Rózsa Zs, Droppa M and Horváth G (1989) Biochim Biophys Acta 973, 350–353).Abbreviations Chl chlorophyll - Cyt cytochrome - DCMU 3-(3,4-dichlorophenyl)-1,1-dimethylurea - D1 psbA gene product - D2 psbD gene product - P680 primary electron donor of PS II - Pheo pheophytin - PS II Photosystem II - Q_A primary quinone acceptor of PS II - Q_B secondary quinone acceptor of PS II - RC reaction centre of PS II - TL thermoluminescence     

Trapping, loss and annihilation of excitations in a photosynthetic system: II. Experiments with the purple bacteria Rhodospirillum rubrum and Rhodopseudomonas capsulata

In this paper a number of experiments with the purple bacteria Rhodospirillum rubrum and Rhodopseudomonas capsulata is described in which the total fluorescence yield and/or the total fraction of reaction centers closed after a picosecond laser pulse were measured as a function of the pulse intensity. The conditions were such that the reaction centers were either all in the open or all in the closed state before the pulse arrived. These experiments are analysed using the theoretical formalism discussed in the preceding paper (Den Hollander, W.T.F., Bakker J.G.C., and Van Grondelle, R., Biochim. Biophys. Acta 725, 492–507). From the experimental results the number of connected photosynthetic units, λ, the rate of energy transfer between neighboring antenna molecules, k_h, and the rate of trapping by an open reaction center, k^o_t, can be estimated. For R. rubrum it is found that λ = 14−17, k_h = (1−2)·10¹² s⁻¹ and k^o_t = (4−6)·10¹¹ s⁻¹, for Rps. capsulata λ ≈ 30, k_h ≈ 4·10¹¹ s⁻¹ and k^o_t ≈ 3·10¹¹ s⁻¹. The findings are discussed in terms of current models for the structure of the antenna and the kinetic properties of the decay processes occurring in these purple bacteria.     

Electron transfer between primary and secondary donors in Rhodospirillum rubrum: evidence for a dimeric association of reaction centers

Light-induced oxidation of the primary electron donor P and of the secondary donor cytochrome c2 was studied in whole cells of Rhodospirillum rubrum in the presence of myxothiazole to slow down their reduction. 1. The primary and secondary electron donors are close to thermodynamic equilibrium during continuous illumination when the rate of the electron transfer is light-limited. This implies a long-range thermodynamic equilibration involving the diffusible cytochrome c2. A different behavior is observed with Rhodobacter sphaeroides R26 whole cells, in which the cytochrome c2 remains trapped within a supercomplex including reaction centers and the cytochrome b/c complex [Joliot, P., et al. (1989) Biochim. Biophys. Acta 975, 336-345]. 2. Under weak flash excitation, the reduction kinetics of the photooxidized primary donor are nearly exponential with a half-time in the hundred microseconds time range. 3. Under strong flash excitation, the reduction of the photooxidized primary donor follows a second-order kinetics. About half of the photooxidized primary donor is reduced in a few milliseconds while the remainder stays oxidized for hundreds of milliseconds despite an excess of secondary donors in their reduced form. The flash intensity dependence of the amplitude of the slow phase of P+ reduction is proportional to the square of the fraction of reaction centers that have undergone a charge separation.(ABSTRACT TRUNCATED AT 250 WORDS)     

Orientation of chromophores in reaction centers of Rhodopseudomonas sphaeroides: a photoselection study.

The relative orientation of the pigments of reaction centers from Rhodopseudomonas sphaeroides has been studied by the photoselection technique. A high value (+0.45) of p=(delta AV--delta AH)/(delta AV + delta AH) is obtained when exciting and observing within the 870 nm band which is contradictory to the results of Mar and Gingras (Mar, T. and Gringras, G. (1976) Biochim. Biophys. Acta 440, 609-621) and Shuvalov et al. (Shuvalov, V.A., Asadov, A.A. and Krakhmaleva, I.N. (1977) FEBS Lett. 16, 240-245). It is shown that the low values of p obtained by both groups were erroneous due to excitation conditions. Analysis of the polarization of light-induced changes when exciting with polarized light in single transitions (spheroiden band and bacteriopheophytin Qx bands) enable us to propose a possible arrangement of the pigments within the reaction center. It is concluded that the 870 nm band corresponds to a single transition and is one of the two bands of the primary electron donor (P-870). The second band of the bacteriochlorophyll dimer is centered at 805 nm. The Qx transitions of the molecules constituting the bacteriochlorophyll dimer are nearly parallel (angle less than 25 degrees). The two bacteriopheophytin molecules present slightly different absorption spectra in the near infra-red. Both bacteriopheophytin absorption bands are subject to a small shift under illumination. The angle between the Qy bacteriopheophytin transitions is 55 degrees or 125 degrees. Both Qy transitions are nearly perpendicular to the 870 nm absorption band. Finally, the carotenoid molecules makes an angle greater than 70 degrees with the 870 nm band and the other bacteriochlorophyll molecules.