Turnover kinetics of Photosystem I measured by the electrochromic effect in Chlorella

The rise kinetics of the absorption changes induced at 515 nm and 480 nm by a flash were studied using two types of xenon flashes of different durations. The ‘slow’ rise of the absorption change ($\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 15–20 μ}\text{s}$) observed by Cox and Delosme (1978 C.R. Acad. Sci. (Paris) Sér. D 282, 775–778) and Joliot P., Delosme, R. and Joliot, A. ((1977) Biochim. Biophys. Acta 459, 47–57) was found to be due to double hits occurring in the reaction centers of System I during the flash.The turnover kinetics of the reaction centers of System I after a short flash were studied by a double flash method. They are in agreement with a second order reaction between P⁺-700 and its electron donor.     

Photosystem I charge separation in the absence of center A and B. III. Biochemical characterization of a reaction center particle containing P-700 and FX

The Photosystem I reaction center is a membrane-bound, multiprotein complex containing a primary electron donor (P-700), a primary electron acceptor (A₀), an intermediate electron acceptor (A₁) and three membrane-bound iron-sulfur centers (F_X, F_B, and F_A). We reported in part I of this series (Golbeck, J.H. and Cornelius, J.M. (1986) Biochim. Biophys. Acta 849, 16–24) that in the presence of 1% lithium dodecyl sulfate (LDS), the reaction center becomes dissociated, resulting in charge separation and recombination between P-700 and F_X without the need for prereduction of F_A and F_B. In this paper, we report (i) the LDS-induced onset of the 1.2-ms ‘fast’ phase of the P-700 absorption transient is time-dependent, attaining a maximum 3:1 ratio of ‘fast’ to ‘slow’ kinetic phases; (ii) the ‘fast’ kinetic phase, corresponding to the P-700⁺ F_X⁻ backreaction, is stabilized indefinitely by dilution of the LDS-treated particle followed by ultrafiltration over a YM-100 membrane; (iii) without stabilization, the P-700⁺ F_X⁻ reaction deteriorates, leading to the rise of the long-lived P-700 triplet formed from the P-700⁺A_O⁻ backreaction; (iv) the ‘slow’ kinetic phase correlates with the redox and ESR properties of F_A and/or F_B, which indicates that in a minority of particles the terminal iron-sulfur protein remains attached to the reaction center core; (v) the ultrafiltered reaction center is severely deficient in all of the low molecular-weight polypeptides, particularly the 19-kDa, 18-kDa and 12-kDa polypeptides relative to the 64-kDa polypeptide(s); (vi) the stabilized particle contains 5.8 mol labile sulfide per mol photoactive P-700, reflecting largely the iron-sulfur content of F_x, but also residual F_A and F_B, on the reaction center; and (vii) the apoproteins of F_A and F_B are physically removed from the reaction center particle as indicated by the presence of protein-bound zero-valence sulfur in the YM-100 filtrate. These results are interpreted in terms of a model for Photosystem I in which F_A and F_B are located on a low-molecular-weight polypeptide and F_X is depicted as a [2Fe-2S] cluster shared between the two high-molecular-weight polypeptides Photosystem I-A1 and Photosystem I-A2.     

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.     

Picosecond fluorescence kinetic studies of electron acceptor Q redox heterogeneity

We have investigated the influence of chloroplast organization on the nature of chemical reductive titrations of Photosystem II fluorescence decay kinetics in spinach chloroplasts. Structural changes of the chloroplast membrane system were induced by varying the ionic environment of the thylakoids. A single-photon timing system with picosecond resolution monitored the kinetics of the chlorophyll a fluorescence emission. At all ionic concentrations studied, we have observed biphasic potentiometric titration curves of fluorescence yield; these have been interpreted to be suggestive of electron acceptor Q heterogeneity (Karukstis, K.K. and Sauer, K. (1983) Biochim. Biophys. Acta 722, 364–371; Cramer, W.A. and Butler, W.L. (1969) Biochim. Biophys. Acta 172, 503–510). A direct relation is observed between the E_m value of the low-potential component of Q and the Mg²⁺ concentration of the chloroplast suspending medium. We have attributed these midpoint potential variations to the thylakoid structural rearrangements involved in cation-regulated grana stacking. Ionic effects on the fluorescence decay kinetics at the redox transitions are discussed in terms of the heterogeneity of Photosystem II units (α- and β-centers) and the mechanism of deexcitation at a closed reaction center (fluorescence or nonradiative decay).     

Influence of temperature on Photosystem II electron transfer reactions

The influence of temperature on the rate of reduction of P-680⁺, the primary donor of Photosystem II, has been studied in the range 5–294 K, in chloroplasts and subchloroplasts particles. P-680 was oxidized by a short laser flash. Its oxidation state was followed by the absorption level at 820 nm, and its reduction attributed to two mechanisms: electron donation from electron donor D₁ and electron return from the primary plastoquinone (back-reaction).Between 294 and approx. 200 K, the rate of the back-reaction, on a logarithmic scale, is a linear function of the reciprocal of the absolute temperature, corresponding to an activation energy between 3.3 and 3.7 kcal · mol^?1, in all of the materials examined (chloroplasts treated at low pH or with Tris; particles prepared with digitonin). Between approx. 200 K and 5 K the rate of the back-reaction is temperature independent, with $\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 1.6}\text{ms}$. In untreated chloroplasts we measured a $\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$ of 1.7 ms for the back-reaction at 77 and 5 K.The rate of electron donation from the donor D₁ has been measured in darkadapted Tris-treated chloroplasts, in the range 294–260 K. This rate is strongly affected by temperature. An activation energy of 11 kcal · mol^?1 was determined for this reaction.In subchloroplast particles prepared with Triton X-100 the signals due to P-680 were contaminated by absorption changes due to the triplet state of chlorophyll a. This triplet state has been examined with pure chlorophyll a in Triton X-100. An Arrhenius plot of its rate of decay shows a temperature-dependent region (292–220 K) with an activation energy of 9 kcal · mol^?1, and a temperature-independent region (below 200 K) with $\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 1.1}\text{ms}$.     

Evidence for a new early acceptor in Photosystem I of plants. An ESR investigation of reaction center triplet yield and of the reduced intermediary acceptors

The yield of the triplet state of the primary electron donor of Photosystem I of photosynthesis (P^T-700) and the characteristic parameters (g value, line shape, saturation behavior) of the ESR signal of the photoaccumulated intermediary acceptor A have been measured for two types of Photosystem I subchloroplast particles: Triton particles (TSF 1, about 100 chlorophyll molecules per P-700) that contain the iron-sulfur acceptors F_X, F_B and F_A, and lithium dodecyl sulfate (LDS) particles (about 40 chlorophyll molecules per P-700) that lack these iron-sulfur acceptors. The results are: (i) In Triton particles the yield of P^T-700 upon illumination is independent of the redox state of A and of F_X,B,A and is maximally about 5% of the active reaction centers at 5 K. The molecular sublevel decay rates are k_x = 1100 s^?1 ± 10%, k_y = 1300 s^?1 ± 10% and k_z = 83 s^?1 ± 20%. In LDS particles the triplet yield decreases linearly with concentration of reduced intermediary acceptors, the maximal yield being about 4% at 5 K assuming full P-700 activity. (ii) In Triton particles the acceptor complex A consists of two acceptors A₀ and A₁, with A₀ preceding A₁. In LDS particles at temperatures below ?30°C only A₀ is photoactive. (iii) The spin-polarized ESR signal found in the time-resolved ESR experiments with Triton particles is attributed to a polarized P-700-A^?₁ spectrum. The decay kinetics are complex and are influenced by transient nutation effects, even at low microwave power. It is concluded that the lifetime at 5 K of P-700A₀A^?₁ must exceed 5 ms. We conclude that P^T-700 originates from charge recombination of P-700A^?₀, and that in Triton particles A₀ and A₁ are both photoaccumulated upon cooling at low redox potential in the light. Since the state P-700AF^?_X does not give rise to triplet formation the 5% triplet yield in Triton particles is probably due to centers with damaged electron transport.     

Similarity of EPR Signal IIf rise and P-680+ decay kinetics in Tris-washed chloroplast Photosystem II preparations as a function of pH

The rise time, of Signal II_f and the decay time of P-680⁺ have been measured kinetically as a function of pH by using EPR. The Photosystem II-enriched preparations which were used as samples were derived from spinach chloroplasts, and they evolved oxygen before Tris washing. The onset kinetics of Signal II_f are in agreement, within experimental error, with the fast component of the decay of an EPR signal attributable to P-680⁺. The signal II_f rise kinetics also show good agreement with published values of the pH dependence of the decay of P-680⁺ measured optically (Conjeaud, H. and Mathis, P. (1980) Biochim. Biophys. Acta 590, 353–359). These results are consistent with a model where the species Z (or D₁) responsible for Signal II_f is the immediate electron donor to P-680⁺ in tris-washed Photosystem II fragments.     

Inhibition of the binding of cytochrome b5 to phosphatidylcholine vesicles by cholesterol

The binding of cytochrome b₅ to single-walled liposomes of egg phosphatidylcholine was inhibited by the presence of cholesterol in the lipid bilayer under conditions where a limited amount of liposomes was incubated with the cytochrome. Since similar conditions seem to apply for the binding of cytochrome b₅ to erythrocyte ghosts, this observation supports the conclusion of Enomoto and Sato (Enomoto, K. and Sato, R. (1977) Biochim. Biophys. Acta 466, 136–147) that the localization of cholesterol on the outer surface of the ghost membrane prevents the binding of cytochrome b₅ to this surface. The finding reported by Roseman et al. (Roseman, M.A., Holloway, P.W. and Calabro, M.A. (1978) Biochim. Biophys. Acta 507, 552–556) that cholesterol did not prevent the cytochrome binding to phosphatidylcholine liposomes in the presence of a large excess of liposomes could be confirmed in the present study, but this does not contradict the abovementioned conclusion.     

Precursors to microsecond delayed luminescence in oxygenevolving and inhibited chloroplasts

We have investigated submillisecond delayed luminescence in spinach chloroplasts under a variety of conditions. In Tris-washed chloroplasts, which are inhibited on the oxidizing side of P-680, the delayed light emission in the 7–200 μs time-range decayed with biphasic behavior. In fully dark-adapted samples illuminated by a single saturating laser pulse, the fast phase of delayed luminescence followed a nearly identical pH-dependent time-course as that observed optically and by ESR for P⁺-680 reduction, thus verifying the recombination hypothesis for the origin of delayed light. The observed slower phase of delayed luminescence was also pH dependent, but unlike the fast phase, could not be ascribed to specific electron transfer events of PS II. This phase could be rationalized by a heterogeneity in the population of P-680. While kinetic parameters were found to be insensitive to changes in ionic strength, the overall luminescence intensity was quite sensitive to the electrical parameters, thus indicating the role of ionic strength and local charges in delayed luminescence modulation. A similar series of experiments was performed on untreated chloroplasts. The pH-dependent delayed luminescence behavior in both untreated chloroplasts and Tris-washed chloroplasts was similar despite significantly faster kinetics associated with the reduction of P⁺-680 by the secondary PS II electron donor, Z, in the former preparation (e.g., Van Best, J.A. and Mathis, P. (1978) Biochim. Biophys. Acta 503, 178–188). Thus, it was concluded that, in untreated samples, microsecond delayed luminescence emanates primarily from centers which are not competent in oxygen evolution. The nearly identical delayed luminescence intensity in untreated chloroplasts and in Tris-washed chloroplasts was rationalized by a model which predicts modulations in delayed luminescence yield by the exciton-quenching effect of P⁺-680. Computer simulations demonstrate the feasibility of this model. The previously documented flash oscillations in microsecond delayed luminescence intensity in untreated chloroplasts (Bowes, J.M. and Crofts, A.R. (1979) Biochim. Biophys. Acta 547, 336–346), which we readily observed, were attributed to alterations in delayed luminescence yield (in nonfunctional centers) by variations in charge density stored at the oxygen-evolving complex of functional centers. Taken together, our results emphasize the dependence of delayed luminescence kinetics upon electron-transfer kinetics and the dependence of delayed luminescence amplitude upon the photochemical parameters, the exciton yield and the emission yield.     

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.     

Electron Transfer in the Photosynthetic Membrane: Influence of PH and Surface Potential on the P-680 Reduction Kinetics

The primary electron donor P-680 of the Photosystem-II reaction center was photoxidized by a short flash given after dark adaptation of photosynthetic membranes in which oxygen evolution was inhibited. The P-680⁺ reduction rate was measured under different conditions of pH and salt concentration by following the recovery of the absorption change at 820 nm. As previously reported for Tris-washed chloroplasts (Conjeaud, H., and P. Mathis, 1980, Biochim. Biophys. Acta, 590:353-359) a fast phase of P-680⁺ reduction slows down as the bulk pH decreases. When salt concentration increases, this fast phase becomes faster for pH above 4.5-5 and slower below. A quantitative interpretation is proposed in which the P-680⁺ reduction kinetics by the secondary electron donor Z are controlled by the local pH. This pH, at the membrane level, can be calculated using the Gouy-Chapman theory. A good fit of the results requires to assume that the surface charge density of the inside of the membrane, near the Photosystem-II reaction center, is positive at low pH values and becomes negative as the pH increases, with a local isoelectric point ~4.8. These results lead us to propose a functional scheme in which a pH-dependent proton release is coupled to the electron transfer between secondary and primary donors of Photosystem-II. The H⁺/e ratio varies from 1 at low pH to 0 at high pH, with a real pK ~6.5 for the protonatable species.     

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).     

Studies on the mechanism of ADRY agents (agents accelerating the deactivation reactions of water-splitting enzyme system Y) on thermoluminescence emission

The effect of 2-(3-chloro-4-trifluoromethyl)anilino-3,5-dinitrothiophene (ANT-2p), known to be the most powerful ADRY agent (Renger, G. (1972) Biochim. Biophys. Acta 256, 428–439), on thermoluminescence has been investigated. Two thermoluminescence bands were analyzed: (a) the emission peaking at about 20–30°C caused by warming up of untreated chloroplasts, illuminated with a single 5 μs flash at room temperature and frozen rapidly to 77 K; and (b) the band emitted in the range of ?10 up 10°C after warming of chloroplast suspensions containing 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU) which were illuminated with a single 5 μs flash at ?15°C and frozen rapidly at 77 K. These bands were attributed to the recombination of the B ^?S₂(S₃) and X-320 ^?S₂ states, respectively (Rutherford, A.W., Crofts, A.R. and Inoue, Y. (1982) Biochim. Biophys. Acta 682, 457–465). It was found that: (1) The B ^?S₂(S₃) band is markedly diminished at very low ANT-2p concentrations of less than one molecule per 2000 chlorophylls. (2) The inhibition of the X-320 ^?S₂ band requires significantly higher concentrations of ANT-2p (50% peak reduction at one ANT-2p molecule per 100 chlorophylls). (3) Preflashing at room temperature before cooling to ?15°C diminishes the X-320 ^?S₂ band significantly in the presence of ANT-2p, while almost no effect is observed in its absence. (4) The state X-320 ^?S₂ decays monoexponentially with a half-lifetime of 2 min at ?15°C in the absence of ANT-2p. In the presence of one ANT-2p molecule per 800 chlorophylls the decay becomes biphasic with half-lifetimes of 0.5 and 2 min and an amplitude ratio of 2:3, respectively. The results obtained can be explained consistently by the function of ANT-2p as an ADRY agent acting as a mobile species within the thylakoid membrane at room temperature. At subzero temperatures, a ‘fixed-place’ mechanism appears to be operative. The implications for the ADRY effect and thermoluminescence are discussed.     

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.     

Reactions between primary and secondary acceptors of Photosystem II in Chlorella Pyrenoidosa under anaerobic conditions as studied by chlorophyll a fluorescence

The kinetics of the fluorescence yield Ф of chlorophyll a in Chlorella pyrenoidosa were studied under anaerobic conditions in the time range from 50 μs to several minutes after short ($\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 30}\text{ns}$ or 5 μs) saturating flashes. The fluorescence yield “in the dark” increased from $\text{Ф = 1}$ at the beginning to $\text{Ф ≈ 5}$ in about 3 h when single flashes separated by dark intervals of about 3 min were given.After one saturating flash, Ф increased to a maximum value (4–5) at 50 μs, then Ф decreased to about 3 with a half time of about 10 ms and to the initial value with a half time of about 2 s. When two flashes separated by 0.2 s were given, the first phase of the decrease after the second flash occurred within 2 ms. After one flash given at high initial fluorescence yield, the 10-ms decay was followed by a 10 s increase to the initial value. After the two flashes 0.2 s apart, the rapid decay was not follewed by a slow increase.These and other experiments provided additional evidence for and extend an earlier hypothesis concerning the acceptor complex of Photosystem II (Bouges-Bocquet, B. (1973) Biochim. Biophys. Acta 314, 250–256; Velthuys, B. R. and Amesz, J. (1974) Biochim. Biophys. Acta 333, 85–94): reaction center 2 contains an acceptor complex QR consisting of an electron-transferring primary acceptor molecule Q, and a secondary electron acceptor R, which can accept two electrons in succession, but transfers two electrons simultaneously to a molecule of the tertiary acceptor pool, containing plastoquinone (A). Furthermore, the kinetics indicate that 2 reactions centers of System I, excited by a short flash, cooperate directly or indirectly in oxidizing a plastohydroquinone molecule (A^2?). If initially all components between photoreaction 1 and 2 are in the reduced state the following sequence of reactions occurs after a flash has oxidised A^2? via System I: Q^?R^2? + A → Q^?R + A^2? → QR^? + A^2?. During anaerobiosis two slow reactions manifest themselves: the reduction of R (and A) within 1 s, presumably by an endogenous electron donor D₁, and the reduction of Q in about 10 s when R is in the state R^? and A in the state A^2?. An endogenous electron donor, D₂, and Q^? compete in reducing the photooxidized donor complex of System II in reactions with half times of the order of 1 s.     

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| = 279·10⁻⁴ cm⁻¹ and |E| = 39·10⁻⁴ 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 ΔH_pp = 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 ΔH_pp = 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.     

On the State 1-State 2 phenomenon in photosynthesis

The State 1-State 2 phenomenon of photosynthesis was studied in Chlorella by measuring the flash yield (Y) and the modulated rate (v) of oxygen evolution induced by weak modulated 650-nm light. From light intensity curves, intensities of 650 and 710 nm background and preilluminations were chosen to give maximum values of Y and v. Following long preilluminations in 710 nm (State 1) or in 650 nm (State 2), Y and v were measured in background light of chosen wavelength. The resulting plots of v vs Y show a discontinuity between State 1 and State 2. They confirm the predictions of Bonaventura and Myers [(1969) Biochim. Biophys. Acta 189, 366–383] and are consistent with changes in α (fraction of absorbed light captured by System II) as explanation of the State 1–State 2 phenomenon. When the intensity of 710 nm preillumination was too low, the characteristics of State 1 were not fully developed and the results then were similar to those of Delrieu [(1972) Biochim. Biophys. Acta 256, 293–299].     

Absorption and structure of an LM unit isolated with sodium dodecyl sulfate from reaction centers of Rhodopseudomonas sphaeroides

Low-temperature absorption, circular dichroism and resonance Raman spectra of the LM units isolated with sodium dodecyl sulfate from wild-type Rhodopseudomonas sphaeroides reaction centers (Agalidis, I. and Reiss-Husson, F. (1983) Biochim. Biophys. Acta 724, 340–351) are described in comparison with those of intact reaction centers. In LM unit, the Q_y absorption band of P-870 at 77 K shifted from 890 nm (in reaction center) to 870 nm and was broadened by about 30%. In contrast, the 800 nm bacteriochlorophyll absorption band including the 810 species remained unmodified. It was concluded that the 810 nm transition is not the higher excitonic component of P-870. The Q_x band of P-870 shifted from 602 nm (in reaction center) to 598 nm in LM, whereas the Q_x band of the other bacteriochlorophylls was the same in reaction center and LM and had two components at about 605 and 598 nm. The Q_xII band of bacteriopheophytin was upshifted to 538 nm and a slight blue shift of the Q_y band of bacteriopheophytin was observed. Resonance Raman spectra of spheroidene in LM showed that its native cis-conformation was preserved. Resonance Raman spectroscopy also demonstrated that in LM the molecular interactions assumed by the conjugated carbonyls of bacteriochlorophyll molecules were altered, but not those assumed by the bacteriopheophytins carbonyls. In particular at least one Keto group of bacteriochlorophyll free in reaction center, becomes intermolecularly bounded in LM (possibly with extraneous water). This group may belong to the primary donor molecules.