Preferential binding of equine ferricytochrome c to the bacterial photosynthetic reaction center from Rhodobacter sphaeroides

Redox titration of horse heart cytochrome c (cyt c), in the presence of varying concentrations of detergent-solubilized photosynthetic reaction center (RC) from Rhodobacter sphaeroides, revealed an RC concentration-dependent decrease in the measured cyt c midpoint potential that is indicative of a 3.6 +/- 0.2-fold stronger binding affinity of oxidized cytochrome to a single binding site. This effect was correlated with preferential binding in the functional complex by redox titration of the fraction of RCs exhibiting microsecond, first-order, special pair reduction by cytochrome. A binding affinity ratio of 3.1 +/- 0.4 was determined by this second technique, confirming the result. Redox titration of flash-induced intracomplex electron transfer also showed the association in the electron transfer-active complex to be strong, with a dissociation constant of 0.17 +/- 0.03 microM. The tight binding is associated with a slow off-rate which, in the case of the oxidized form, can influence the kinetics of P(+) reduction. The pitfalls of the common use of xenon flashlamps to photoexcite fast electron-transfer reactions are discussed with relation to the first electron transfer from primary to secondary RC quinone acceptors. The results shed some light on the diversity of kinetic behavior reported for the cytochrome to RC electron-transfer reaction.     

Pressure effects on the photochemistry of bacterial photosynthetic reaction centers from Rhodobacter sphaeroides R-26 and Rhodopseudomonas viridis

Electron-transfer reactions and triplet decay rates have been studied at pressures up to 300 MPa. In reaction centers from Rhodobacter sphaeroides R-26, high pressure hastened the electron transfers from both the primary and secondary quinones (Q_A and Q_B) to the primary electron donor bacteriochlorophyll, P. Motion of Q_A between two sites, one nearer to P and the other nearer to Q_B, could account for these pressure effects. In reaction centers from Rhodopseudomonas viridis, charge recombination was slowed by high pressure. Decay rates were also studied for the triplet state, P^R. In Rb. sphaeroides R-26 with Q_A reduced with Na₂S₂O₄, the decay was hastened by pressure. This could be explained if P^R decays through a charge-transfer triplet state, or if the decay kinetics of P^R are sensitive to the distance between P and Q_A⁻. In Rps. viridis reaction centers, and in Rb. sphaeroides reaction centers that were depleted of Q_A, the lifetime of P^R was not altered by pressure.     

Structure of the membrane-bound protein photosynthetic reaction center from Rhodobacter sphaeroides

The structure of the photosynthetic reaction center (RC) from Rhodobacter sphaeroides was determined at 3.1-A resolution by the molecular replacement method, using the Rhodopseudomonas viridis RC as the search structure. Atomic coordinates were refined with the difference Fourier method and restrained least-squares refinement techniques to a current R factor of 22%. The tertiary structure of the RC complex is stabilized by hydrophobic interactions between the L and M chains, by interactions of the pigments with each other and with the L and M chains, by residues from the L and M chains that coordinate to the Fe2+, by salt bridges that are formed between the L and M chains and the H chain, and possibly by electrostatic forces between the ends of helices. The conserved residues at the N-termini of the L and M chains were identified as recognition sites for the H chain.     

Effects of photosynthetic reaction center H protein domain mutations on photosynthetic properties and reaction center assembly in Rhodobacter sphaeroides

Purple bacterial photosynthetic reaction center (RC) H proteins comprise three cellular domains: an 11 amino acid N-terminal sequence on the periplasmic side of the inner membrane; a single transmembrane alpha-helix; and a large C-terminal, globular cytoplasmic domain. We studied the roles of these domains in Rhodobacter sphaeroides RC function and assembly, using a mutagenesis approach that included domain swapping with Blastochloris viridis RC H segments and a periplasmic domain deletion. All mutations that affected photosynthesis reduced the amount of the RC complex. The RC H periplasmic domain is shown to be involved in the accumulation of the RC H protein in the cell membrane, while the transmembrane domain has an additional role in RC complex assembly, perhaps through interactions with RC M. The RC H cytoplasmic domain also functions in RC complex assembly. There is a correlation between the amounts of membrane-associated RC H and RC L, whereas RC M is found in the cell membrane independently of RC H and RC L. Furthermore, substantial amounts of RC M and RC L are found in the soluble fraction of cells only when RC H is present in the membrane. We suggest that RC M provides a nucleus for RC complex assembly, and that a RC H/M/L assemblage results in a cytoplasmic pool of soluble RC M and RC L proteins to provide precursors for maximal production of the RC complex.     

Kinetic analysis of the thermal stability of the photosynthetic reaction center from Rhodobacter sphaeroides

The temperature-induced denaturation of the photosynthetic reaction center from Rhodobacter sphaeroides has been studied through the changes that occur in the absorption spectrum of the bound chromophores on heating. At elevated temperatures, the characteristic absorbance bands of the bacteriochlorins bound to the polypeptides within the reaction center are lost, and are replaced by features typical of unbound bacteriochlorophyll and bacteriopheophytin. The kinetics of the spectral changes cannot be explained by a direct conversion from the functional to the denatured form of the protein, and require the presence of at least one intermediate. Possible mechanisms for the transformation via an intermediate are examined using a global analysis of the kinetic data, and the most likely mechanism is shown to involve a reversible transformation between the native state and an off-pathway intermediate, coupled to an irreversible transformation to the denatured state. The activation energies for the transformations between the three components are calculated from the effect of temperature on the individual rate constants, and the likely structural changes of the protein during the temperature-induced transformation are discussed.     

Interactions between cytochrome c2 and the photosynthetic reaction center from Rhodobacter sphaeroides: the cation-pi interaction

The cation-pi interaction between positively charged and aromatic groups is a common feature of many proteins and protein complexes. The structure of the complex between cytochrome c(2) (cyt c(2)) and the photosynthetic reaction center (RC) from Rhodobacter sphaeroides exhibits a cation-pi complex formed between Arg-C32 on cyt c(2) and Tyr-M295 on the RC [Axelrod, H. L., et al. (2002) J. Mol. Biol. 319, 501-515]. The importance of the cation-pi interaction for binding and electron transfer was studied by mutating Tyr-M295 and Arg-C32. The first- and second-order rates for electron transfer were not affected by mutating Tyr-M295 to Ala, indicating that the cation-pi complex does not greatly affect the association process or structure of the state active in electron transfer. The dissociation constant K(D) showed a greater increase when Try-M295 was replaced with nonaromatic Ala (3-fold) as opposed to aromatic Phe (1.2-fold), which is characteristic of a cation-pi interaction. Replacement of Arg-C32 with Ala increased K(D) (80-fold) largely due to removal of electrostatic interactions with negatively charged residues on the RC. Replacement with Lys increased K(D) (6-fold), indicating that Lys does not form a cation-pi complex. This specificity for Arg may be due to a solvation effect. Double mutant analysis indicates an interaction energy between Tyr-M295 and Arg-C32 of approximately -24 meV (-0.6 kcal/mol). This energy is surprisingly small considering the widespread occurrence of cation-pi complexes and may be due to the tradeoff between the favorable cation-pi binding energy and the unfavorable desolvation energy needed to bury Arg-C32 in the short-range contact region between the two proteins.     

Continuum electrostatic model for the binding of cytochrome c2 to the photosynthetic reaction center from Rhodobacter sphaeroides

Electrostatic interactions are important for protein-protein association. In this study, we examined the electrostatic interactions between two proteins, cytochrome c(2) (cyt c(2)) and the reaction center (RC) from the photosynthetic bacterium Rhodobacter sphaeroides, that function in intermolecular electron transfer in photosynthesis. Electrostatic contributions to the binding energy for the cyt c(2)-RC complex were calculated using continuum electrostatic methods based on the recent cocrystal structure [Axelrod, H. L., et al. (2002) J. Mol. Biol. 319, 501-515]. Calculated changes in binding energy due to mutations of charged interface residues agreed with experimental results for a protein dielectric constant epsilon(in) of 10. However, the electrostatic contribution to the binding energy for the complex was close to zero due to unfavorable desolvation energies that compensate for the favorable Coulomb attraction. The electrostatic energy calculated as a function of displacement of the cyt c(2) from the bound position showed a shallow minimum at a position near but displaced from the cocrystal configuration. These results show that although electrostatic steering is present, other short-range interactions must be present to contribute to the binding energy and to determine the structure of the complex. Calculations made to model the experimental data on association rates indicate a solvent-separated transition state for binding in which the cyt c(2) is displaced approximately 8 A above its position in the bound complex. These results are consistent with a two-step model for protein association: electrostatic docking of the cyt c(2) followed by desolvation to form short-range van der Waals contacts for rapid electron transfer.     

Cu2+ site in photosynthetic bacterial reaction centers from Rhodobacter sphaeroides, Rhodobacter capsulatus, and Rhodopseudomonas viridis

The interaction of metal ions with isolated photosynthetic reaction centers (RCs) from the purple bacteria Rhodobacter sphaeroides, Rhodobacter capsulatus, and Rhodopseudomonas viridis has been investigated with transient optical and magnetic resonance techniques. In RCs from all species, the electrochromic response of the bacteriopheophytin cofactors associated with Q(A)(-)Q(B) --> Q(A)Q(B)(-) electron transfer is slowed in the presence of Cu(2+). This slowing is similar to the metal ion effect observed for RCs from Rb. sphaeroides where Zn(2+) was bound to a specific site on the surface of the RC [Utschig et al. (1998) Biochemistry 37, 8278]. The coordination environments of the Cu(2+) sites were probed with electron paramagnetic resonance (EPR) spectroscopy, providing the first direct spectroscopic evidence for the existence of a second metal site in RCs from Rb. capsulatus and Rps. viridis. In the dark, RCs with Cu(2+) bound to the surface exhibit axially symmetric EPR spectra. Electron spin echo envelope modulation (ESEEM) spectral results indicate multiple weakly hyperfine coupled (14)N nuclei in close proximity to Cu(2+). These ESEEM spectra resemble those observed for Cu(2+) RCs from Rb. sphaeroides [Utschig et al. (2000) Biochemistry 39, 2961] and indicate that two or more histidines ligate the Cu(2+) at the surface site in each RC. Thus, RCs from Rb. sphaeroides, Rb. capsulatus, and Rps. viridis each have a structurally analogous Cu(2+) binding site that is involved in modulating the Q(A)(-)Q(B) --> Q(A)Q(B)(-) electron-transfer process. Inspection of the Rps. viridis crystal structure reveals four potential histidine ligands from three different subunits (M16, H178, H72, and L211) located beneath the Q(B) binding pocket. The location of these histidines is surprisingly similar to the grouping of four histidine residues (H68, H126, H128, and L211) observed in the Rb. sphaeroides RC crystal structure. Further elucidation of these Cu(2+) sites will provide a means to investigate localized proton entry into the RCs of Rb. capsulatus and Rps. viridis as well as locate a site of protein motions coupled with electron transfer.     

Effects of ionizable residues on the absorption spectrum and initial electron-transfer kinetics in the photosynthetic reaction center of Rhodobacter sphaeroides

Effects of ionizable amino acids on spectroscopic properties and electron-transfer kinetics in the photosynthetic reaction center (RC) of Rhodobacter sphaeroides are investigated by site-directed mutations designed to alter the electrostatic environment of the bacteriochlorophyll dimer that serves as the photochemical electron donor (P). Arginine residues at homologous positions in the L and M subunits (L135 and M164) are changed independently: Arg L135 is replaced by Lys, Leu, Glu, and Gln and Arg M164 by Leu and Glu. Asp L155 also is mutated to Asn, Tyr L164 to Phe, and Cys L247 to Lys and Asp. The mutations at L155, L164, and M164 have little effect on the absorption spectrum, whereas those at L135 and L247 shift the long-wavelength absorption band of P to higher energies. Fits to the ground-state absorption and hole-burned spectra indicate that the blue shift and increased width of the absorption band in the L135 mutants are due partly to changes in the distribution of energies for the zero-phonon absorption line and partly to stronger electron-phonon coupling. The initial electron-transfer kinetics are not changed significantly in most of the mutants, but the time constant increases from 3.0 +/- 0.2 in wild-type RCs to 4.7 +/- 0.2 in C(L247)D and 7.0 +/- 0.3 ps in C(L247)K. The effects of the mutations on the solvation free energies of the product of the initial electron-transfer reaction (P(+)) and the charge-transfer states that contribute to the absorption spectrum ( and ) were calculated by using a distance-dependent electrostatic screening factor. The results are qualitatively in accord with the view that electrostatic interactions of the bacteriochlorophylls with ionized residues of the protein are strongly screened and make only minor contributions to the energetics and dynamics of charge separation. However, the slowing of electron transfer in the Cys L247 mutants and the blue shift of the spectrum in some of the Arg L135 and Cys L247 mutants cannot be explained consistently by electrostatic interactions of the mutated residues with P and B(L); we ascribe these effects tentatively to structural changes caused by the mutations.     

Unbinding of oxidized cytochrome c from photosynthetic reaction center of Rhodobacter sphaeroides is the bottleneck of fast turnover

To understand the details of rate limitation of turnover of the photosynthetic reaction center, photooxidation of horse heart cytochrome c by reaction center from Rhodobacter spheroides in detergent dispersion has been examined by intense continuous illumination under a wide variety of conditions of cytochrome concentration, ionic strength, viscosity, temperature, light intensity, and pH. The observed steady-state turnover rate of the cytochrome was not light intensity limited. In accordance with recent findings [Larson, J. W., Wells, T. A., and Wraight, C. A. (1998) Biophys. J. 74 (2), A76], the turnover rate increased with increasing bulk ionic strength in the range of 0-40 mM NaCl from 1000 up to 2300 s(-)(1) and then decreased at high ionic strength under conditions of excess cytochrome and ubiquinone and a photochemical rate constant of 4500 s(-)(1). Furthermore, we found the following: (i) The contribution of donor (cytochrome c) and acceptor (ubiquinone) sides as well as the binding of reduced and the release of oxidized cytochrome c could be separated in the observed kinetics. At neutral and acidic pH (when the proton transfer is not rate limiting) and at low or moderate ionic strength, the turnover rate of the reaction center was limited primarily by the low release rate of the photooxidized cytochrome c (product inhibition). At high ionic strength, however, the binding rate of the reduced cytochrome c decreased dramatically and became the bottleneck. The observed activation energy of the steady-state turnover rate reflected the changes in limiting mechanisms: 1.5 kcal/mol at 4 mM and 5.7 kcal/mol at 100 mM ionic strength. A similar distinction was observed in the viscosity dependence of the turnover rate: the decrease was steep (eta(-)(1)) at 40 and 100 mM ionic strengths and moderate (eta(-)(0.2)) under low-salt (4 mM) conditions. (ii) The rate of quinone exchange at the acceptor side with excess ubiquinone-30 or ubiquinone-50 was higher than the cytochrome exchange at the donor side and did not limit the observed rate of cytochrome turnover. (iii) Multivalent cations exerted effects not only through ionic strength (screening) but also by direct interaction with surface charge groups (ion-pair production). Heavy metal ion Cd(2+) bound to the RC with apparent dissociation constant of 14 microM. (iv) A two-state model of collisional interaction between reaction center and cytochrome c together with simple electrostatic considerations in the calculation of rate constants was generally sufficient to describe the kinetics of photooxidation of dimer and cytochrome c. (v) The pH dependence of cytochrome turnover rate indicated that the steady-state turnover rate of the cytochrome under high light conditions was not determined by the isoelectric point of the reaction center (pI = 6. 1) but by the carboxyl residues near the docking site.     

Theoretical studies on the mechanism of primary electron transfer in the photosynthetic reaction center of Rhodobacter sphaeroides

The mechanism of the primary electron transfer (ET) process in the photosynthetic reaction center (PRC) of Rhodobacter sphaeroides has been studied with quantum chemistry method of ab initio density functional theory (DFT) (B3LYP/6-31G) based on the optimized X-ray crystallographic structure. The calculation was carried out on different structural levels. The electronic structure of pigment molecules was first studied, and then the influence of the neighboring protein was taken into account at three approximation levels: (a) the surrounding proteins were treated as a homogeneous medium with a uniform dielectric constant (SCRF); (b) both the influence of axial coordination of His to the special pair P and ABChl as, and the hydrogen bonds between related residues and P and also BPhas were included; and (c) the influence of the electronic structure of the protein subunit chains as a whole was studied. The results suggest that: (1) according to the composition of the HOMO and LUMO of P, there might be a charge-separated state of (BChl_L ⁺BChl_M ⁻) for the excited state of P; (2) to treat the protein surroundings as a homogeneous medium is not sufficient. Different interactions between pigment molecules and related residues play different roles in the ET process; (3) the axial coordination of His to P raises the E _LUMO of P greatly, and it is very important for the ET process to occur in the PRC of wild-type bacterium; the axial coordination of His to ABChl as also raises their E _LUMO significantly; (4) the hydrogen-bonds between amino acid residues and P and also BPh as depress the E _LUMO of the pigment molecules to some extent, which makes the E _LUMO of P lower than those of ABChlas, and the E _LUMO of BPh a _L lower than that of BPh a _M. Consequently, the ET process from P to BPh a _L does not, according to our calculation model, occur via ABChl a _L. The possibility of the ET pathway from P to BPh a _L via ABChl a _L was discussed; (5) the frontier orbitals of protein subunit chains L and M are localized at the random coil area and the α–helix areas, respectively. Results mentioned above support the fact that the ET process proceeds in favourable circumstances along the branch L. This revised version was published online in June 2006 with corrections to the Cover Date.     

Identification of proton transfer pathways in the X-ray crystal structure of the bacterial reaction center from Rhodobacter sphaeroides

Structural features that have important implications for the fundamental process of transmembrane proton transfer are examined in the recently published high resolution atomic structures of the reaction center (RC) from Rhodobacter sphaeroides in the dark adapted state (DQ_AQ_B) and the charged separated state (D⁺Q_AQ_B ^–); the latter is the active state for proton transfer to the semiquinone. The structures have been determined at 2.2 Å and 2.6 Å resolution, respectively, as reported by Stowell et al. (1997) [Science 276: 812–816]. Three possible proton transfer pathways (P1, P2, P3) consisting of water molecules and/or protonatable residues were identified which connect the Q_B binding region with the cytoplasmic exposed surface at Asp H224 & Asp M240 (P1), Tyr M3 (P2) and Asp M17 (P3). All three represent possible pathways for proton transfer into the RC. P1 contains an uninterrupted chain of water molecules. This path could, in addition, facilitate the exchange of quinone for quinol during the photocycle by allowing water to move into and out of the binding pocket. Located near these pathways is a cluster of electrostatically interacting acid residues (Asp-L213, Glu-H173, Asp-M17, Asp H124, Asp-L210 and Asp H170) each being within 4.5 Å of a neighboring carboxylic acid or a bridging water molecule. This cluster could serve as an internal proton reservoir facilitating fast protonation of Q_B ^– that could occur at a rate greater than that attainable by proton uptake from solution.     

Characterization of bacterial photosynthetic reaction center crystals from Rhodopseudomonas sphaeroides R-26 by X-ray diffraction

An orthorhombic crystal form (P2(1)2(1)2(1)) of the reaction center from the photosynthetic bacterium Rhodopseudomonas sphaeroides R-26 has been characterized. The crystals were grown from polyethylene glycol; the unit cell dimensions are a = 142.2 A, b = 139.6 A, and c = 78.7 A; and they contain one reaction center in each crystallographic asymmetric unit. The crystals diffract to at least 3.0 A resolution, and are suitable for detailed structural studies.     

A picosecond circular dichroism study of photosynthetic reaction centers from Rhodobacter sphaeroides

Picosecond transient circular dichroism spectra are reported for the primary intermediates in the photocycle of reaction centers isolated from Rhodobacter sphaeroides. The time-resolved circular dichroism spectra of the two electron transfer intermediates (BChl2) +BPh-LQA and (BChl2) +BPhLQ-A reveal a large, nonconservative, and fairly stationary CD band at 800 nm. These results suggests that mechanisms other than exciton interactions need to be included in order to explain the optical activity of this biological system.     

Energy trapping and detrapping in reaction center mutants from Rhodobacter sphaeroides

Time-resolved fluorescence of chromatophores isolated from strains of Rhodobacter sphaeroides containing light harvesting complex I (LHI) and reaction center (RC) (no light harvesting complex II) was measured at several temperatures between 295 K and 10 K. Measurements were performed to investigate energy trapping from LHI to the RC in RC mutants that have a P/P(+) midpoint potential either above or below wild-type (WT). Six different strains were investigated: WT + LHI, four mutants with altered RC P/P(+) midpoint potentials, and an LHI-only strain. In the mutants with the highest P/P(+) midpoint potentials, the electron transfer rate decreases significantly, and at low temperatures it is possible to directly observe energy transfer from LHI to the RC by detecting the fluorescence kinetics from both complexes. In all mutants, fluorescence kinetics are multiexponential. To explain this, RC + LHI fluorescence kinetics were analyzed using target analysis in which specific kinetic models were compared. The kinetics at all temperatures can be well described with a model which accounts for the energy transfer between LHI and the RC and also includes the relaxation of the charge separated state P(+)H(A)(-), created in the RC as a result of the primary charge separation.     

Effect of high pressure on the photochemical reaction center from Rhodobacter sphaeroides R26.1

High-pressure studies on the photochemical reaction center from the photosynthetic bacterium Rhodobacter sphaeroides, strain R26.1, shows that, up to 0.6 GPa, this carotenoid-less membrane protein does not loose its three-dimensional structure at room temperature. However, as evidenced by Fourier-transform preresonance Raman and electronic absorption spectra, between the atmospheric pressure and 0.2 GPa, the structure of the bacterial reaction center experiences a number of local reorganizations in the binding site of the primary electron donor. Above that value, the apparent compressibility of this membrane protein is inhomogeneous, being most noticeable in proximity to the bacteriopheophytin molecules. In this elevated pressure range, no more structural reorganization of the primary electron donor binding site can be observed. However, its electronic structure becomes dramatically perturbed, and the oscillator strength of its Q(y) electronic transition drops by nearly one order of magnitude. This effect is likely due to very small, pressure-induced changes in its dimeric structure.     

pH modulates the quinone position in the photosynthetic reaction center from Rhodobacter sphaeroides in the neutral and charge separated states

The structure of the photosynthetic reaction-center from Rhodobacter sphaeroides has been determined at four different pH values (6.5, 8.0, 9.0, 10.0) in the neutral and in charge separated states. At pH 8.0, in the neutral state, we obtain a resolution of 1.87 A, which is the best ever reported for the bacterial reaction center protein. Our crystallographic data confirm the existence of two different binding positions of the secondary quinone (QB). We observe a new orientation of QB in its distal position, which shows no ring-flip compared to the orientation in the proximal position. Datasets collected for the different pH values show a pH-dependence of the population of the proximal position. The new orientation of QB in the distal position and the pH-dependence could be confirmed by continuum electrostatics calculations. Our calculations are in agreement with the experimentally observed proton uptake upon charge separation. The high resolution of our crystallographic data allows us to identify new water molecules and external residues being involved in two previously described hydrogen bond proton channels. These extended proton-transfer pathways, ending at either of the two oxo-groups of QB in its proximal position, provide additional evidence that ring-flipping is not required for complete protonation of QB upon reduction.     

Crystallization of the reaction center from Rhodobacter sphaeroides in a new tetragonal form

The reaction center from the nonsulfur purple bacteriumRhodobacter sphaeroideshas been crystallized in a new form. The crystals grew in the presence of polyethylene glycol 4000, the detergent β-octyl glucoside, and the amphiphiles heptane triol and benzamidine hydrochloride, using the sitting drop method. The space group of these crystals is tetragonal, P4₁(4₃)2₁2, and the cell constants are a = b = 141.5 Å and c = 276.7 Å with probably 2 proteins per asymmetric unit. A native data set has been set collected to a resolution of 2.8 Å consisting of 56,332 unique reflections (50,731 with F > 2σ) with anR_sym of 9.5%. Analysis of the diffraction data is underway using molecular and isomorphous replacement. © 1994 Wiley-Liss, Inc.     

Long-lived charge-separated states in bacterial reaction centers isolated from Rhodobacter sphaeroides

We studied the accumulation of long-lived charge-separated states in reaction centers isolated from Rhodobacter sphaeroides, using continuous illumination, or trains of single-turnover flashes. We found that under both conditions a long-lived state was produced with a quantum yield of about 1%. This long-lived species resembles the normal P(+)Q(-) state in all respects, but has a lifetime of several minutes. Under continuous illumination the long-lived state can be accumulated, leading to close to full conversion of the reaction centers into this state. The lifetime of this accumulated state varies from a few minutes up to more than 20 min, and depends on the illumination history. Surprisingly, the lifetime and quantum yield do not depend on the presence of the secondary quinone, Q(B). Under oxygen-free conditions the accumulation was reversible, no changes in the normal recombination times were observed due to the intense illumination. The long-lived state is responsible for most of the dark adaptation and hysteresis effects observed in room temperature experiments. A simple method for quinone extraction and reconstitution was developed.