Temperature dependence of energy transfer from the long wavelength antenna BChl-896 to the reaction center in Rhodospirillum rubrum,Rhodobacter sphaeroides (w.t. and M21 mutant) from 77 to 177K,studied by picosecond absorption spectroscopy

Decay of the bacteriochlorophyll excited state was measured in membranes of the purple bacteria Rhodospirillum (R.) rubrum, Rhodobacter (Rb.) sphaeroides wild type and Rb. sphaeroides mutant M21 using low intensity picosecond absorption spectroscopy. The excitation and probing pulses were chosen in the far red wing of the long wavelength absorption band, such that predominantly the minor antenna species B896 was excited. The decay of B896 was studied between 77 and 177K under conditions that the traps were active. In all species the B896 excited state decay is almost temperature independent between 100 and 177K, and probably between 100 and 300 K. In this temperature range the decay rates for the various species are very similar and close to 40 ps. Below 100 K this rate remains temperature independent in Rb. sphaeroides w. t. and M21, while in R. rubrum a steep decrease sets in. An analysis of this data with the theory of nuclear tunneling indicates an activation energy for the final transfer step from B896 to the special pair of 70cm^-1 for R. rubrum and 30cm^-1 or less for Rb. sphaeroides.Abbreviations B880 and B896 the main and long wavelength bacteriochlorophyll's of the LH-1 antenna - RC reaction centre - P special pair in the RC     

Probing the fluorescence emission kinetics of the photosynthetic apparatus of Rhodopseudomonas sphaeroides, strain 1760-1, on a picosecond pulse fluorometer

Using the pulse picosecond fluorometric technique the fluorescence properties of intact cells, isolated chromatophores and photosynthetic reaction centres were studied in bacteria Rhodopseudomonas sphaeroides, strain 1760-1.The fluorescent emission from reduced reaction centres excited by 694.3 nm light has a biphasic character, the lifetimes of the components being τ₁ = 15±8 ps and τ₂ = 250 ps. The faster component, τ₁, contributes to the integral fluorescence in the long wavelength region. It disappears with oxidation of the reaction centres and is attributed to photoactive bacteriochlorophyll P870. The slow component, τ, is apparently due to both bacteriochlorophyll P800 and bacteriopheophytin. The fluorescence from intact cells exhibits a monophasic pattern and decays with τ = 200 ps.The fluorescence emitted by chromatophores comprises two components with τ₃ = 200 ps and τ₄ = 4200 ps. The duration of fluorescence τ₃ increases to its maximum of 500–550 ps, as P870 is oxidized chemically or photochemically, while τ₄ remains unchanged. The fluorescence with a lifetime of 200 ps was ascribed to the photosystem and the 4200-ps fluorescence to bacteriochlorophyll which had lost its functional links with the photosystem.The rise time of the fluorescence emitted by chromatophores varies from 60 or 70 ps to 350 ps depending on the wavelength of the exciting light and the recorded spectral region. On the basis of our findings the rate for energy migration was estimated to be 10⁹ s^?1.     

Picosecond time-resolved energy transfer in Porphyridium cruentum. Part II. In the isolated light harvesting complex (phycobilisomes)

The transfer of excitation energy between phycobiliproteins in isolated phycobilisomes has been observed on a picosecond time scale. The photon density of the excitation pulse has been carefully varied so as to control the level of exciton interactions induced in the pigment bed. The 530 nm light pulse is absorbed predominantly by B-phycoerythrin, and the fluorescence of this component rises within the pulse duration and shows a mean 1/e decay time of 70 ps. The main emission band, centred at 672 nm, is due to allophycocyanin and is prominent because of the absence of energy transfer to chlorophyll. Energy transfer to this pigment from B-phycoerythrin via R-phycocyanin produces a risetime of 120 ps to the fluorescence maximum. The lifetime of the allophycocyanin fluorescence is found to be about 4 ns using excitation pulses of low photon densities (10¹³ photons · cm^?2), but decreases to about 2 ns at higher photon densities. The relative quantum yield of the allophycocyanin fluorescence decreases almost 10 fold over the range of laser pulse intensities, 10¹³–10¹⁶ photons · cm^?2. Fluorescence quenching by exciton-exciton annihilation is only observed in allophycocyanin and could be a consequence of the long lifetime of the single exciton in this pigment.     

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.     

Effects of electron donors and acceptors on the kinetics of the photoelectric responses in Rhodospirillum rubrum and Rhodopseudomonas sphaeroides chromatophores

Chromatophores of Rhodospirillum rubrum and Rhodopseudomonas sphaeroides were adhered to one side of a collodion film impregnated with a phospholipid solution in decane and 20 ns laser flashes were delivered to produce an electrical potential difference generated across the collodion film in less than 0.2 μs (resolution time of the apparatus). The kinetics of Δψ decay in the dark was studied. In the absence of additions there occurs a ‘rapid’ decay of photoelectric potential (τ ≈ 70 ms) corresponding to charge recombination within the primary dipole P-870⁺-Q^-_A. The rapid decay of Δψ is prevented by ascorbate in the presence of permeable redox dyes which can reduce the photooxidized P-870⁺ rapidly. Under these conditions, Δψ dissipates with τ > 0.5 s typical of a passive discharge of the chromatophore membrane. Prevention of the rapid decay of Δψ by 70–75% can be observed upon addition of excess ubiquinone-10 to the solution of phospholipids used to impregnate the collodion film, and to a lesser extent by addition of some other quinones. The effect of quinones is inhibited by o-phenanthroline. The data obtained show that upon association of chromatophores with the collodion film, the secondary quinone acceptor is extracted from its binding site into a hydrophobic volume of the macroscopic membrane, and this effect can be reversed by exogenous ubiquinone. About 4-times less Q-10 is required to reconstitute Q_B function in chromatophores from Rps. sphaeroides than in those from R. rubrum, which points to a tighter binding of the secondary acceptor in the former. No evidence for electrogenic nature of Q⁻_A → Q_B electron transfer could be obtained in experiments with Q_B-replenished chromatophores.     

Formation and decay of radical-pair state P+I− in Chloroflexus aurantiacus reaction centers

We have examined the room temperature kinetics of the absorption changes associated with the formation of state P⁺I⁻ (P⁺BPh⁻) and its subsequent decay to state P⁺Q⁻_A in reaction centers from Chloroflexus aurantiacus. Our data, acquired using 30-ps excitation flashes, strongly suggest that formation of P⁺I⁻ (P⁺BPh⁻) takes longer in Chloroflexus than in reaction centers from Rhodopseudomonas sphaeroides. The reduction of the photoactive bacteriopheophytin (BPh) could take as long as 13 ps. Absorption changes different from those due to P⁺I⁻ are observed early in the excitation flash, but the detailed identity of the transient remains unclear. We also find that the kinetics observed subsequent to P⁺I⁻ formation differ with detection wavelength. The time constant measured in the anion band (I⁻) at 655 nm is 324 ± 20 ps and probably reflects the rate of electron transfer from I⁻ (BPh⁻) to Q_A. However, the kinetics measured in the BPh ground-state absorption bands are slightly longer: 365 ± 19 and 367 ± 21 ps at 538 and 760 nm, respectively. At 810 nm, a wavelength normally associated with the monomeric bacteriochlorophyll (BChl) in the Chloroflexus reaction center, a slightly faster (281 ± 19 ps) time constant is observed. This detection-wavelength dependence of the kinetics is similar to that observed recently in Rps. sphaeroides reaction centers. Comparison of these results suggests that the kinetics observed in the ground-state absorption bands of the BPhs and BChls in Chloroflexus may contain contributions from readjustments of the pigments and/or protein in response to the charge separation process.     

Properties of photochemical reaction centers purified from Rhodopseudomonas gelatinosa

Reaction centers were isolated from a carotenoidless mutant of Rhodopseudomonas gelatinosa by hydroxyapatite chromatography of purified chromatophores treated with lauryl dimethyl amine oxide. Absorption spectra and spectra of light-induced absorbance changes are similar to those of reaction centers from Rhodopseudomonas sphaeroides. The ratio of absorbance at 280 nm to that at 799 nm was 1.8 in the purest preparations. The extinction coefficient at the 799 nm absorption maximum was estimated to be 305 ± 20 mM^?1 · cm^?1. The molecular weight based on protein and chromophore assays was found to be 1.5 · 10⁵; the reaction center protein accounted for 6% of the total membrane protein. These reaction centers contained no cytochrome and showed just two components of apparent molecular weights 33 000 and 25 000 in polyacrylamide gel electrophoresis. The chromatophores contained 42 molecules of antenna bacteriochlorophyll for each reaction center.     

Short-lived delayed luminescence of photosynthesizing organisms II. The ratio between delayed and prompt fluorescence as studied by the modulation method

The ratio between the intensities of delayed and prompt fluorescence was studied for different photosynthetic objects under different conditions by a modulation method. The method is based on excitation of luminescing objects by light, modulated harmonically, and on a combined study of phase shifts and demodulation coefficients of the luminescence as related to excitation light. The presence of intense delayed emissions was revealed in purple bacteria, Ectothiorhodospira shaposhinokovii, Rhodospirillum rubrum and Rhodopseudomonas sphaeroides, in the micro- and nanosecond range. Under conditions of saturating light, their proportion was several percent of the total emission.The most striking phenomenon was observed under reducing conditions (addition of 1 · 10^?2 M Na₂S₂O₄ to whole-cell suspensions of purple bacteria) where the intensity of the delayed emissions grew dramatically and became comparable to that of prompt fluorescence.The data obtained indicate that, at room temperature, reversal of some early stages of charge separation in bacterial reaction centres may proceed largely via the channel that includes generation of the reaction-centre bacteriochlorophyll in the excited singlet state, followed by excitation-energy migration to antenna bacteriochlorophyll.The relation of these phenomena to the efficiency of solar energy utilization in photosynthetic apparatus is discussed.     

Energy trapping and detrapping by wild type and mutant reaction centers of purple non-sulfur bacteria

Time-correlated single photon counting was used to study energy trapping and detrapping kinetics at 295 K in Rhodobacter sphaeroides chromatophore membranes containing mutant reaction centers. The mutant reaction centers were expressed in a background strain of Rb. sphaeroides which contained only B880 antenna complexes and no B800-850 antenna complexes. The excited state decay times in the isolated reaction centers from these strains were previously shown to vary by roughly 15-fold, from 3.4 to 52 ps, due to differences in the charge separation rates in the different mutants (Allen and Williams (1995) J Bioenerg Biomembr 27: 275–283). In this study, measurements were also performed on wild type Rhodospirillum rubrum and Rb. sphaeroides B880 antenna-only mutant chromatophores for comparison. The emission kinetics in membranes containing mutant reaction centers was complex. The experimental data were analyzed in terms of a kinetic model that involved fast excitation migration between antenna complexes followed by reversible energy transfer to the reaction center and charge separation. Three emission time constants were identified by fitting the data to a sum of exponential decay components. They were assigned to trapping/quenching of antenna excitations by the reaction center, recombination of the P⁺H^– charge-separated state of the reaction center reforming an emitting state, and emission from uncoupled antenna pigment-protein complexes. The first varied from 60 to 160 ps, depending on the reaction center mutation; the second was 200–300 ps, and the third was about 700 ps. The observed weak linear dependence of the trapping time on the primary charge separation time, together with the known sub-picosecond exciton migration time within the antenna, supports the concept that it is energy transfer from the antenna to the reaction center, rather than charge separation, that limits the overall energy trapping time in wild type chromatophores. The component due to charge recombination reforming the excited state is minor in wild type membranes, but increases substantially in mutants due to the decreasing free energy gap between the states P^* and P⁺H^–.Abbreviations PSU photosynthetic unit - Bchl bacteriochlorophyll - Bphe bacteriopheophytin - P reaction center primary electron donor - RC reaction center - Rb. Rhodobacter - Rs. Rhodospirillum - EDTA (ethylenediamine)tetraacetic acid - Tris tris(hydroxymethyl)aminomethane Author for correspondence     

Comparison of the fluorescence kinetics of detergent-solubilized and membrane-reconstituted LH2 complexes from Rps. acidophila and Rb. sphaeroides

Picosecond time-resolved fluorescence spectroscopy has been used in order to compare the fluorescence kinetics of detergent-solubilized and membrane-reconstituted light-harvesting 2 (LH2) complexes from the purple bacteria Rhodopseudomonas (Rps.) acidophila and Rhodobacter (Rb.) sphaeroides. LH2 complexes were reconstituted in phospholipid model membranes at different lipid:protein-ratios and all samples were studied exciting with a wide range of excitation densities. While the detergent-solubilized LH2 complexes from Rps. acidophila showed monoexponential decay kinetics (τ_f = 980 ps) for excitation densities of up to 3·10¹³ photons/(pulse·cm²), the membrane-reconstituted LH2 complexes showed multiexponential kinetics even at low excitation densities and high lipid:protein-ratios. The latter finding indicates an efficient clustering of LH2 complexes in the phospholipid membranes. Similar results were obtained for the LH2 complexes from Rb. sphaeroides. Guest editor: Dr. Conrad Mullineaux.     

Electrogenic reduction of the secondary quinone acceptor in chromatophores of Rhodospirillum rubrum: Rapid kinetics measurements

Electron transfer Q_A → Q_B has been reconstituted with added Q-10 in Rhodospirillum rubrum chromatophores associated with a phospholipid-impregnated collodion film. Rapid kinetics measurements of laser flash-induced ΔΨ generated in the chromatophores show that whereas electron transfer from Q_a⁻ to Q_B upon the first flash is not electrogenic in dark-adapted chromatophores, reduction of Q⁻_B to Q_bh₂ induced by the second flash gives rise to an electrogenic phase with τ = 250 μs at pH 7.5 which contributes about 10% to the total ΔΨ generated upon the flash. The electrogenic phase is ascribed to vectorial protonation of Q²⁻_B.     

Singlet and triplet excited carotenoid and antenna bacteriochlorophyll of the photosynthetic purple bacterium Rhodospirillum rubrum as studied by picosecond absorbance difference spectroscopy

Picosecond absorbance difference spectra at a number of delay times after a 35 ps excitation pulse and kinetics of absorbance changes were measured in chromatophores of the photosynthetic purple bacterium Rhodospirillum rubrum after chemical oxidation of the primary electron donor P-875. Kinetics and spectra were measured of the excited singlet states of carotenoid and bacteriochlorophyll a and also of the triplet state of the carotenoid. The excited singlet state of carotenoid, produced by direct excitation at 532 nm, is characterized by a bleaching of the ground state absorption bands in the region 450–490 nm and by an absorbance increase with a maximum near 570 nm. Its lifetime was calculated to be 0.6 ± 0.1 ps in vitro and less than 1 ps in vivo. The triplet state of carotenoid in vivo is formed within 100 ps after direct carotenoid excitation via a pathway that does not involve excited states of bacteriochlorophyll. Singlet excitation of a bacteriochlorophyll a molecule causes the bleaching of its Q_x and Q_y absorption bands, and is probably associated with blue shifts of the Q_y absorption band of about six neighboring bacteriochlorophyll molecules. Upon increasing the excitation density, the average lifetime of the singlet excitations on bacteriochlorophyll decreased from about 350 ps to about 10 ps or less. The results are in quantitative agreement with the known effect of singlet-singlet annihilation upon the fluorescence yield, and furthermore show that no bacteriochlorophyll or carotenoid triplet formation is associated with this annihilation.     

Surface potential on the periplasmic side of the photosynthetic membrane of Rhodopseudomonas sphaeroides

Membrane surface potential on the periplasmic side of the photosynthetic membrane was estimated in cells, spheroplasts and chromatophores of Rhodopseudomonas sphaeroides. When the membrane potential (potential difference between bulk aqueous phases) was kept constant in the presence of carbonylcyanide m-chlorophenylhydrazone, addition of salt to a suspension of cells or spheroplasts induced a red shift in the carotenoid absorption spectrum which indicated a change in the intramembrane electrical field. The spectral shift is explained by a rise in electrical potential at the outside surface of the photosynthetic membrane due to a decrease in extent of the negative surface potential.The spectral shift occurred in the direction opposite to that in chromatophores, indicating that the sidedness of the membrane of cells or spheroplasts is opposite to that of chromatophores. The dependences of the extent of the potential change on concentration and valence of cations of salts agreed with the Gouy-Chapman relationship on the electrical diffuse double layer. The charge density on the periplasmic surface of the photosynthetic membrane was estimated to be ?2.9 · 10^?3 elementary charge per Ų, while that on the cytoplasmic side surface was calculated as ?1.9 · 10^?3 elementary charge per Ų (Matsuura, K., Masamoto, K., Itoh, S. and Nishimura, M. (1979) Biochim. Biophys. Acta 547, 91–102). Surface potential on the periplasmic side of the photosynthetic membrane was estimated to be about ?50 mV at pH 7.8 in the presence of 0.1 M monovalent salt.     

Time-resolved fluorescence spectroscopy of spinach chloroplast

Picosecond fluorescent kinetics and time-resolved spectra of spinach chloroplast were measured at room temperature and low temperatures. The measurement is conducted with 530 nm excitation at an average intensity of 2 · 10¹⁴ photons/cm², pulse and at a pulse separation of 6 ns for the 100 pulses used. The 685 nm fluorescent kinetics was found to decay with two components, a fast component with a 56 ps lifetime, and a slow component with a 220 ps lifetime. The 730 nm fluorescent kinetics at room temperature is a single exponential decay with a 100 ps lifetime. The 730 nm fluorescence lifetime was found to increase by a factor of 6 when the temperature was lowered from room temperature to 90 K, while the 685 and 695 nm fluorescent kinetics were unchanged. The time-resolved spectra data obtained within 10 ps after excitation is consistent with the kinetic data reported here. A two-level fluorescence scheme is proposed to explain the kinetics. The effect of excitation with high light intensity and multiple pulses is discussed.     

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.     

Time-resolved picosecond fluorescence spectra of the antenna chlorophylls in Chlorella vulgaris. Resolution of Photosystem I fluorescence

The time-resolved fluorescence emission and excitation spectra of Chlorella vulgaris cells have been measured by single-photon timing with picosecond resolution. In a three-exponential analysis the time-resolved excitation spectra recorded at 685 and 706 nm emission wavelength with closed PS II reaction centers show large variations of the preexponential factors of the different decay components as a function of wavelength. At λ_em = 685 nm the major contribution to the fluorescence decay originates from two components with life-times of 2.1–2.4 and 1.2–1.3 ns. A short-lived component with life-times of 0.1–0.16 ns of relatively small amplitude is also found. When the emission is detected at 706 nm, the short-lived component with a life-time of less than 0.1 ns predominates. Time-resolved emission spectra using λ_exc = 630 or λ_exc = 652 nm show a spectral peak of the two longer-lived components at about 680–685 nm, whereas the fast component is red-shifted as compared to the others and shows a maximum at about 690 nm. The emission spectrum observed upon excitation at 696 nm with closed PS II reaction centers shows a large increase in the amplitude of the fast component with a lifetime of 80–100 ps as compared to that at 630 nm excitation. At almost open Photosystem II (PS II) reaction centers (F₀), the life-time of the fast component decreased from 150–160 ps at 682 nm to less than 100 ps at 720 nm emission wavelength. We conclude that at least two pigment pools contribute to the fast component. One is attributed to PS II and the other to Photosystem I (PS I). They have life-times of approx. 180 ps and 80 ps, respectively. The 80 ps (PS I) contribution has a spectral maximum slightly below 700 nm, whereas the 180 ps (PS II) spectrum peaks at 680–685 nm. The spectra of the middle decay component τ_m and its sensitivity to inhibitors of PS II suggest that this component is not preferentially related to LHC II but arises mainly from Chl a pigments probably associated with a second type of PS II centers. The amplitudes of the fast (180 ps, PS II) component and the long-lived decay show an opposite dependence on the state of the PS II centers and confirm our earlier conclusion that the contribution of PS II to the fast component probably disappears at the F_max state (Haehnel W., Holzwarth, A.R. and Wendler, J. (1983) Photochem. Photobiol. 34, 435–443). Our data are discussed in terms of α,β-heterogeneity in PS II centers.     

Free-energy change accompanying the reduction of the reaction center secondary quinone in Rhodopseudomonas sphaeroides chromatophores

The standard free-energy change accompanying the electron transfer from Q_A to Q_B was estimated from the intensity of the delayed fluorescence in chromatophores of Rhodopseudomonas sphaeroides. The value of 120 meV (at pH 8) suggests that Q_B⁻ is more stable in the chromatophore membrane than in the isolated reaction center.     

Picosecond processes in chromatophores at various excitation intensities

The aim of this paper is to review and discuss the results obtained by fluorescence and absorption spectroscopy of bacterial chromatophores excited with picosecond pulses of varying power and intensity. It was inferred that spectral and kinetic characteristics depend essentially on the intensity, the repetition rate of the picosecond excitation pulses as well as on the optical density of the samples used. Taking the different experimental conditions properly into account, most of the discrepancies between the fluorescence and absorption measurements can be solved. At high pulse repetition rate (>10⁶ Hz), even at moderate excitation intensities (10¹⁰–10¹¹ photons/cm² per pulse), relatively long-lived triplet states start accumulating in the system. These are efficient (as compared to the reaction centers) quenchers of mobile singlet excitations due to singlet-triplet annihilation. The singlet-triplet annihilation rate constant in Rhodospirillum rubrum was determined to be equal to 10^-9 cm³ s^-1. At fluences >10¹² photons/cm² per pulse singlet-singlet annihilation must be taken into account. Furthermore, in the case of high pulse repetition rates, triplet-triplet annihilation must be considered as well. From an analysis of experimental data it was inferred that the singlet-singlet annihilation process is probably migration-limited. If this is the case, one has to conclude that the rate of excitation decay in light-harvesting antenna at low pumping intensities is limited by the efficiency of excitation trapping by the reaction center. The influence of annihilation processes on spectral changes is also discussed as is the potential of a local heating caused by annihilation processes. The manifestation of spectral inhomogeneity of light-harvesting antenna in picosecond fluorescence and absorption kinetics is analyzed.Abbreviations LHA light-harvesting antenna - RC reaction center     

High-precision determination of quantum yields of photoelectric excitation conversion in reaction centers of purple bacteria <Emphasis Type="Italic">Rhodospirillum rubrum</Emphasis> and <Emphasis Type="Italic">Rhodobacter sphaeroides</Emphasis> R-26

Using an original model of primary events in bacterial photosynthetic reaction centers (RCs), a complete set of kinetic and energy characteristics, and temperature dependences of nanosecond luminescence component(s) emitted by the RCs, upper limits to the quantum yield of primary transmembrane charge separation in RCs of the purple bacterium Rhodospirillum rubrum and the carotenoidless mutant Rhodobacter sphaeroides R-26 have been estimated. The calculations have given the values of 0.915 ± 0.045 and 0.978 ± 0.006, respectively. In the case of Rb. sphaeroides R-26, the quantum yield partly overlapped with that reported earlier (1.02 ± 0.04) by Wraight and Clayton (BBA, 1974. vol. 333, pp. 246–260).     

Two regimens of electrogenic cyclic redox chain operation in chromatophores of non-sulfur purple bacteria A study using antimycin A

Antimycin A causes a biphasic suppression of the light-induced membrane potential generation in Rhodospirillum rubrum and Rhodopseudomonas sphaeroides chromatophores incubated anaerobically. The first phase is observed at low antibiotic concentrations and is apparently due to its action as a cyclic electron transfer inhibitor. The second phase is manifested at concentrations which are greater than 1–2 μM and is due to uncoupling that may be connected with an antibiotic-induced dissipation of the electrochemical H⁺ gradient across the chromatophore membrane. The inhibitory effect of anti-mycin added at low concentrations under aerobic conditions is removed by succinate to a large extent. It is expected that the electrogenic cyclic redox chain in the bacterial chromatophores incubated under conditions of continuous illumination may function at two regimes: (1) as a complete chain involving all the redox components, and (2) as a shortened chain involving only the P-870 photoreaction center, ubiquinone and cytochrome c₂.