Charge accumulation and photochemistry in leaves studied by thermoluminescence and delayed light emission

A major breakthrough in our understanding of how plants oxidize water to molecular O(2) was the discovery by P. Joliot and co-workers that the O(2) yield per flash, in a series of light flashes, oscillates with a periodicity of 4. This led to the concept by B. Kok and co-workers that these reactions involve accumulation of four positive charges in independent "O(2)-evolving centers," which undergo a series of changes in their redox state (the so-called S states). In the present paper, we have applied optical techniques (such as thermoluminescence and delayed light emission, both discovered by W. Arnold and co-workers) to monitor charge storage on the O(2)-evolving system in leaves from higher plants. We observed a period of four oscillations in both thermoluminescence and delayed light emission, with maxima on flashes 2 and 6, establishing a relationship with the charge accumulation process in photosynthesis. These measurements provided additional new information: the deactivation of the "O(2)-evolving centers," which cannot be measured by the O(2) method in the leaves, is in the 20- to 30-s range; and in the dark-adapted leaves, the secondary bound plastoquinone molecule (the so-called secondary electron acceptor Q(B)) is in equal concentration in its reduced and oxidized forms. The origin of thermoluminescence and delayed light emission, in terms of the recombination of charges on the O(2)-evolving and plastoquinone sides, is also discussed.

Site-directed mutagenesis in photosystem II of the cyanobacterium Synechocystis sp. PCC 6803: Donor D is a tyrosine residue in the D2 protein

The chemical nature of electron donor(s) in photosystem II in photosynthetic membranes was analyzed by site-directed mutagenesis of the gene encoding the protein D2 of the photosystem II reaction center. Mutation of the Tyr-160 residue of the D2 protein into phenylalanine results in the disappearance of the electron paramagnetic resonance signal II(S) originating from D(+), the oxidized form of the slow photosystem II electron donor D. Signal II(S) is still present if a neighboring residue in D2, Met-159, is mutated into arginine. Both mutants have normal rereduction kinetics of the oxidized primary electron donor, P680(+), in octyl glucoside-extracted thylakoids, indicating that D is not directly involved in P680(+) reduction. However, overall photosystem II activity appears to be impaired in the Tyr-160-Phe mutant: photosystem II-dependent growth of this mutant is slowed down by a factor of 3-4, whereas photoheterotrophic growth rates in wild type and mutant are essentially identical. Binding studies of diuron, a photosystem II herbicide, show that there is no appreciable decrease in the number of photosystem II centers in the Tyr-160-Phe mutant. The decrease in photosystem II activity in this mutant may be interpreted to indicate a role of D in photoactivation, rather than one as an important redox intermediate in the photosynthetic electron-transport chain.

Genetically engineered mutant of the cyanobacterium Synechocystis 6803 lacks the photosystem II chlorophyll-binding protein CP-47

CP-47 is absent in a genetically engineered mutant of cyanobacterium Synechocystis 6803, in which the psbB gene [encoding the chlorophyll-binding photosystem II (PSII) protein CP-47] was interrupted. Another chlorophyll-binding PSII protein, CP-43, is present in the mutant, and functionally inactive PSII-enriched particles can be isolated from mutant thylakoids. We interpret these data as indicating that the PSII core complex of the mutant still assembles in the absence of CP-47. The mutant lacks a 77 K fluorescence emission maximum at 695 nm, suggesting that the PSII reaction center is not functional. The absence of primary photochemistry was indicated by EPR and optical measurements: no chlorophyll triplet originating from charge recombination between P680(+) and Pheo(-) was observed in the mutant, and there were no flash-induced absorption changes at 820 nm attributable to chlorophyll P680 oxidation. These observations lead us to conclude that CP-47 plays an essential role in the activity of the PSII reaction center.

Radical pair state in photosystem II

A stable light-induced EPR signal is reported in photosystem II particles and in chloroplasts at 5 K. Characteristic spectral features indicate that the signal arises from dipole-dipole interactions of a radical pair triplet state. From its dependence on potential, its relationship to the spin-polarized triplet state, and the redox state of the pheophytin acceptor (Ph) and because it is present in Tris-washed chloroplasts but not in untreated chloroplasts, we conclude that the signal is formed when the reaction center is in the state D(+)P(680)Ph(-) (P(680) is the primary chlorophyll donor and D(+) is an oxidized donor to P(680)). The low-temperature photochemical sequence is thought to occur as follows. (i) Donation from D to the P(680) (+)Ph(-) state occurs at liquid helium temperature in low quantum yield; this reaction is reversible at temperatures above 5 K. (ii) In normal chloroplasts, donation occurs to the D(+)P(680)Ph(-) state, but this does not occur in Tris-washed chloroplasts or in the photosystem II particles at 77 K or lower. (iii) Illumination, at 200 K, of photosystem particles or Tris-washed chloroplasts results in donation to the D(+)P(680)Ph(-) state from another donor. From experiments in the absence of redox mediators and the temperatures dependence of the splitting of the signal, it is suggested that the state D(+)P(680)Ph(-) itself may be the origin of the radical pair triplet signal. The signal has been simulated by assuming the presence of at least two distinct radical pairs that differ slightly in the distance separating the radicals of the pairs. The distance between the radicals of the pair is calculated to be 6-7 A.

Herbicide-induced changes in charge recombination and redox potential of Q(A) in the T4 mutant of Blastochloris viridis

To gain new insights into the function of photosystem II (PSII) herbicides DCMU (a urea herbicide) and bromoxynil (a phenolic herbicide), we have studied their effects in a better understood system, the bacterial photosynthetic reaction center of the terbutryn-resistant mutant T4 of Blastochloris (Bl.) viridis. This mutant is uniquely sensitive to these herbicides. We have used redox potentiometry and time-resolved absorption spectroscopy in the nanosecond and microsecond time scale. At room temperature the P(+)(*)Q(A)(-)(*) charge recombination in the presence of bromoxynil was faster than in the presence of DCMU. Two phases of P(+)(*)Q(A)(-)(*) recombination were observed. In accordance with the literature, the two phases were attributed to two different populations of reaction centers. Although the herbicides did induce small differences in the activation barriers of the charge recombination reactions, these did not explain the large herbicide-induced differences in the kinetics at ambient temperature. Instead, these were attributed to a change in the relative amplitude of the phases, with the fast:slow ratio being approximately 3:1 with bromoxynil and approximately 1:2 with DCMU at 300 K. Redox titrations of Q(A) were performed with and without herbicides at pH 6.5. The E(m) was shifted by approximately -75 mV by bromoxynil and by approximately +55 mV by DCMU. As the titrations were done over a time range that is assumed to be much longer than that for the transition between the two different populations, the potentials measured are considered to be a weighted average of two potentials for Q(A). The influence of the herbicides can thus be considered to be on the equilibrium of the two reaction center forms. This may also be the case in photosystem II.

Photosystem II: evolutionary perspectives

Based on the current model of its structure and function, photosystem II (PSII) seems to have evolved from an ancestor that was homodimeric in terms of its protein core and contained a special pair of chlorophylls as the photo-oxidizable cofactor. It is proposed that the key event in the evolution of PSII was a mutation that resulted in the separation of the two pigments that made up the special chlorophyll pair, making them into two chlorophylls that were neither special nor paired. These ordinary chlorophylls, along with the two adjacent monomeric chlorophylls, were very oxidizing: a property proposed to be intrinsic to monomeric chlorophylls in the environment provided by reaction centre (RC) proteins. It seems likely that other (mainly electrostatic) changes in the environments of the pigments probably tuned their redox potentials further but these changes would have been minor compared with the redox jump imposed by splitting of the special pair. This sudden increase in redox potential allowed the development of oxygen evolution. The highly oxidizing homodimeric RC would probably have been not only inefficient in terms of photochemistry and charge storage but also wasteful in terms of protein or pigments undergoing damage due to the oxidative chemistry. These problems would have constituted selective pressures in favour of the lop-sided, heterodimeric system that exists as PSII today, in which the highly oxidized species are limited to only one side of the heterodimer: the sacrificial, rapidly turned-over D1 protein. It is also suggested that one reason for maintaining an oxidizable tyrosine, TyrD, on the D2 side of the RC, is that the proton associated with its tyrosyl radical, has an electrostatic role in confining P(+) to the expendable D1 side.

Rapid formation of the stable tyrosyl radical in photosystem II

Two symmetrically positioned redox active tyrosine residues are present in the photosystem II (PSII) reaction center. One of them, TyrZ, is oxidized in the ns-micros time scale by P680+ and reduced rapidly (micros to ms) by electrons from the Mn complex. The other one, TyrD, is stable in its oxidized form and seems to play no direct role in enzyme function. Here, we have studied electron donation from these tyrosines to the chlorophyll cation (P680+) in Mn-depleted PSII from plants and cyanobacteria. In particular, a mutant lacking TyrZ was used to investigate electron donation from TyrD. By using EPR and time-resolved absorption spectroscopy, we show that reduced TyrD is capable of donating an electron to P680+ with t1/2 approximately equal to 190 ns at pH 8.5 in approximately half of the centers. This rate is approximately 10(5) times faster than was previously thought and similar to the TyrZ donation rate in Mn-depleted wild-type PSII (pH 8.5). Some earlier arguments put forward to rationalize the supposedly slow electron donation from TyrD (compared with that from TyrZ) can be reassessed. At pH 6.5, TyrZ (t1/2 = 2-10 micros) donates much faster to P680+ than does TyrD (t1/2 > 150 micros). These different rates may reflect the different fates of the proton released from the respective tyrosines upon oxidation. The rapid rate of electron donation from TyrD requires at least partial localization of P680+ on the chlorophyll (PD2) that is located on the D2 side of the reaction center.

Herbicide-induced oxidative stress in photosystem II

Some herbicides act by binding to the exchangeable quinone site in the photosystem II (PSII) reaction centre, thus blocking electron transfer. In this article, it is hypothesized that the plant is killed by light-induced oxidative stress initiated by damage caused by formation of singlet oxygen in the reaction centre itself. This occurs when light-induced charge pairs in herbicide-inhibited PSII decay by a charge recombination route involving the formation of a chlorophyll triplet state that is able to activate oxygen. The binding of phenolic herbicides favours this pathway, thus increasing the efficiency of photodamage in this class of herbicides.

Electron spin echo envelope modulation spectroscopy in photosystem I

The applications of electron spin echo envelope modulation (ESEEM) spectroscopy to study paramagnetic centers in photosystem I (PSI) are reviewed with special attention to the novel spectroscopic techniques applied and the structural information obtained. We briefly summarize the physical principles and experimental techniques of ESEEM, the spectral shapes and the methods for their analysis. In PSI, ESEEM spectroscopy has been used to the study of the cation radical form of the primary electron donor chlorophyll species, P(700)(+), and the phyllosemiquinone anion radical, A(1)(-), that acts as a low-potential electron carrier. For P(700)(+), ESEEM has contributed to a debate concerning whether the cation is localized on a one or two chlorophyll molecules. This debate is treated in detail and relevant data from other methods, particularly electron nuclear double resonance (ENDOR), are also discussed. It is concluded that the ESEEM and ENDOR data can be explained in terms of five distinct nitrogen couplings, four from the tetrapyrrole ring and a fifth from an axial ligand. Thus the ENDOR and ESEEM data can be fully accounted for based on the spin density being localized on a single chlorophyll molecule. This does not eliminate the possibility that some of the unpaired spin is shared with the other chlorophyll of P(700)(+); so far, however, no unambiguous evidence has been obtained from these electron paramagnetic resonance methods. The ESEEM of the phyllosemiquinone radical A(1)(-) provided the first evidence for a tryptophan molecule pi-stacked over the semiquinone and for a weaker interaction from an additional nitrogen nucleus. Recent site-directed mutagenesis studies verified the presence of the tryptophan close to A(1), while the recent crystal structure showed that the tryptophan was indeed pi-stacked and that a weak potential H-bond from an amide backbone to one of the (semi)quinone carbonyls is probably the origin of the to the second nitrogen coupling seen in the ESEEM. ESEEM has already played an important role in the structural characterization on PSI and since it specifically probes the radical forms of the chromophores and their protein environment, the information obtained is complimentary to the crystallography. ESEEM then will continue to provide structural information that is often unavailable using other methods.

Beta-carotene redox reactions in photosystem II: electron transfer pathway

A carotenoid (Car), a chlorophyll (Chl(Z)), and cytochrome b(559) (Cyt b(559)) are able to donate electrons with a low quantum yield to the photooxidized chlorophyll, P680(+), when photosystem II (PSII) is illuminated at low temperatures. Three pathways for electron transfer from Cyt b(559) to P680(+) are considered: (a) the "linear pathway" in which Cyt b(559) donates via Chl(Z) to Car, (b) the "branched pathway" in which Cyt b(559) donates via Car and where Chl(Z) is also able to donate to Car, and (c) the "parallel pathway" where Cyt b(559) donates to P680 without intermediate electron carriers and electron donation from Chl(Z) and Car occurs by a competing pathway. Experiments were performed using EPR and spectrophotometry in an attempt to distinguish among these pathways, and the following observations were made. (1) Using PSII with an intact Mn cluster in which Cyt b(559) was preoxidized, Car oxidation was dominant upon illumination at < or =20 K, while electron donation from Chl dominated at >120 K. (2) When Cyt b(559) was prereduced, its light-induced oxidation occurred at < or =20 K in what appeared to be all of the centers and without the formation of a detectable Car(+) intermediate. The small and variable quantity of Car(+) photoinduced in these experiments can be attributed to the residual centers in which Cyt b(559) remained oxidized prior to illumination. (3) The relative rates for irreversible electron donation from Cyt b(559) and Car were determined indirectly at 20 K by monitoring the flash-induced loss of charge separation (i.e., the accumulation of Cyt b(559)(+)Q(A)(-) or Car(+)Q(A)(-)). Similar yields per flash were observed (13% for Cyt b(559) and 8% for Car), indicating similar donation rates. The slightly lower yield with Car as a donor is attributed at least in part to slow charge recombination occurring from the Car(+)Q(A)(-) radical pair in a fraction of centers. (4) Light-induced oxidation of Cyt b(559) and Car at 20 K was monitored directly by EPR, and the rates were found to be indistinguishable. The parallel pathway predicts that when both Cyt b(559) and Car are prereduced, the relative amounts of Cyt b(559)(+) and Car(+) produced upon illumination at 20 K should depend directly on their relative electron donation rates. The measured similarity in the donation rates thus predicts comparable yields of oxidation for both donors. However, what is observed experimentally is that Cyt b(559) oxidation occurs almost exclusively, and this argues strongly against the parallel pathway. The lack of Car(+) as a detectable intermediate is attributed to rapid electron transfer from Cyt b(559) to Car(+). The trapping of Car(+) at low temperature when Cyt b(559) is preoxidized but its absence when Cyt b(559) is prereduced is taken as an argument against the simple linear pathway. Overall, the data reported here and previously favor the branched pathway over the linear pathway, while the parallel pathway is thought to be unlikely. Structural considerations provide further arguments in favor of the branched model.

The heart of photosynthesis in glorious 3D

The input of solar energy into photosynthesis, and thence into the biosphere, occurs via chlorophyll-containing proteins known as reaction centres. There are two kinds of reaction centre in oxygenic photosynthesis: photosystem I (PSI) and photosystem II (PSII). The PSII reaction centre, alias the oxygen-evolving enzyme, the water-oxidizing complex or the water-plastoquinone photo-oxidoreductase, has now been crystallized and its structure solved to a resolution of 3.8 A.

Chlorophyll and carotenoid radicals in photosystem II studied by pulsed ENDOR

The stable carotenoid cation radical (Car(*+)) and chlorophyll cation radical (Chl(Z)(*+)) in photosystem II (PS II) have been studied by pulsed electron nuclear double resonance (ENDOR) spectroscopy. The spectra were essentially the same for oxygen-evolving PS II and Mn-depleted PS II. The radicals were generated by illumination given at low temperatures, and the ENDOR spectra were attributed to Car(*)(+) and Chl(Z)(*+) on the basis of their characteristic behavior with temperature as demonstrated earlier [Hanley et al. (1999) Biochemistry 38, 8189-8195]: i.e., (a) the Car(*)(+) alone was generated by illumination at < or =20 K, while Chl(Z)(*+) alone was generated at 200 K, and (b) warming of the sample containing the Car(*+) to 200 K resulted in the loss of the signal attributable to Car(*+) and its replacement by a spectrum attributable to the Chl(Z)(*+). A map of the hyperfine structure of Car(*+) in PS II and in organic solvent was obtained. The largest observed hyperfine splitting for Car(*+) in either environment was in the order of 8-9 MHz. Thus, the spin density on the cation is proposed to be delocalized over the carotenoid molecule. The pulsed ENDOR spectrum of Chl(Z)(*)(+) was compared to that obtained from a Chl a cation in frozen organic solvent. The hyperfine coupling constants attributed to the beta-protons at position 17 and 18 are well resolved from Chl(Z)(*+) in PS II (10. 8 and 14.9 MHz) but not in Chl a(*+) in organic solvent (12.5 MHz). This suggests a more defined conformation of ring IV with respect to the rest of the tetrapyrrole ring plane of Chl(Z)(*+) than Chl a(*+) probably induced by the protein matrix.

EPR study of the oxygen evolving complex in His-tagged photosystem II from the cyanobacterium Synechococcus elongatus

The Mn(4)-cluster and the cytochrome c(550) in histidine-tagged photosystem II (PSII) from Synechococcus elongatus were studied using electron paramagnetic resonance (EPR) spectroscopy. The EPR signals associated with the S(0)-state (spin = 1/2) and the S(2)-state (spin = 1/2 and IR-induced spin = 5/2 state) were essentially identical to those detected in the non-His-tagged strain. The EPR signals from the S(3)-state, not previously reported in cyanobacteria, were detectable both using perpendicular (at g = 10) and parallel (at g = 14) polarization EPR, and these signals are similar to those found in plant PSII. In the S(3)-state, near-infrared illumination at 50 K induced a 176-G-wide split signal at g = 2 and signals at g = 5.20 and g = 1.51. These signals differ slightly from those reported in plant PSII [Ioannidis, N., and Petrouleas, V. (2000) Biochemistry 39, 5246-5254]. In accordance with the cited work, the split signal presumably reflects a radical interacting with the Mn(4)-cluster in a fraction of centers, while the g = 5.20 and g = 1.51 signals are tentatively attributed to a high-spin state of the Mn(4)-cluster with zero field splitting parameters different from those in plant PSII, reflecting minor changes in the environment of the Mn(4)-cluster. Biochemical modifications (Sr(2+)/Ca(2+) substitution, acetate and NH(3) treatments) were also investigated. In Sr(2+)-reconstituted PSII, in addition to the expected modified S(2) multiline signal, a signal at g = 5.2 was present instead of the g approximately 4 signal seen in plant PSII. In NH(3)-treated samples, in addition to the expected modified S(2)-multiline signal, a g approximately 4 signal was detected in a small proportion of the reaction centers. This is of note since g approximately 4 spectra arising from the Mn(4)-cluster in the S(2) state have not yet been published in cyanobacterial PSII. The detection of modified S(3)-signals in both perpendicular (at g = 7.5) and parallel (at g = 12) polarization EPR from NH(3)-treated PSII indicate that NH(3) is still bound in the S(3)-state. The acetate-treated PSII behaves essentially as in plant PSII. A study using oriented samples indicated that the heme plane of the oxidized low spin Cytc(550) was perpendicular to the plane of the membrane.

Orientation of the tyrosyl D, pheophytin anion, and semiquinone Q(A)(*)(-) radicals in photosystem II determined by high-field electron paramagnetic resonance

The radical forms of two cofactors and an amino acid in the photosystem II (PS II) reaction center were studied by using high-field EPR both in frozen solution and in oriented multilayers. Their orientation with respect to the membrane was determined by using one-dimensionally oriented samples. The ring plane of the stable tyrosyl radical, Y(D)(*), makes an angle of 64 degrees +/- 5 degrees with the membrane plane, and the C-O direction is tilted by 72 degrees +/- 5 degrees in the plane of the radical compared to the membrane plane. The semiquinone, Q(A)(*)(-), generated by chemical reduction in samples lacking the non-heme iron, has its ring plane at an angle of 72 degrees +/- 5 degrees to the membrane plane, and the O-O axis is tilted by 21 degrees +/- 5 degrees in the plane of the quinone compared to the membrane plane. This orientation is similar to that of Q(A)(*)(-) in purple bacteria reaction centers except for the tilt angle which is slightly bigger. The pheophytin anion was generated by photoaccumulation under reducing conditions. Its ring plane is almost perpendicular to the membrane with an angle of 70 degrees +/- 5 degrees with respect to the membrane plane. This is very similar to the orientation of the pheophytin in purple bacteria reaction centers. The position of the g tensor with respect to the molecule is tentatively assigned for the anion radical on the basis of this comparison. In this work, the treatment of orientation data from EPR spectroscopy applied to one-dimensionally oriented multilayers is examined in detail, and improvements over previous approaches are given.

Calcium binding to the photosystem II subunit CP29

We have identified a Ca(2+)-binding site of the 29-kDa chlorophyll a/b-binding protein CP29, a light harvesting protein of photosystem II most likely involved in photoregulation. (45)Ca(2+) binding studies and dot blot analyses of CP29 demonstrate that CP29 is a Ca(2+)-binding protein. The primary sequence of CP29 does not exhibit an obvious Ca(2+)-binding site therefore we have used Yb(3+) replacement to analyze this site. Near-infrared Yb(3+) vibronic side band fluorescence spectroscopy (Roselli, C., Boussac, A., and Mattioli, T. A. (1994) Proc. Natl. Acad. Sci. U. S. A. 91, 12897-12901) of Yb(3+)-reconstituted CP29 indicated a single population of Yb(3+)-binding sites rich in carboxylic acids, characteristic of Ca(2+)-binding sites. A structural model of CP29 presents two purported extra-membranar loops which are relatively rich in carboxylic acids, one on the stromae side and one on the lumenal side. The loop on the lumenal side is adjacent to glutamic acid 166 in helix C of CP29, which is known to be the binding site for dicyclohexylcarbodiimide (Pesaresi, P., Sandonà, D., Giuffra, E. , and Bassi, R. (1997) FEBS Lett. 402, 151-156). Dicyclohexylcarbodiimide binding prevented Ca(2+) binding, therefore we propose that the Ca(2+) in CP29 is bound in the domain including the lumenal loop between helices B and C.

Comparative study of the g=4.1 EPR signals in the S(2) state of photosystem II

The Mn(4) complex which is involved in water oxidation in photosystem II is known to exhibit three types of EPR signals in the S(2) state, one of the five redox states of the enzyme cycle: a multiline signal (spin 1/2), signals at g5 (spin 5/2) and a signal at g=4.1 (or g=4.25). The g=4.1 signal could be generated under two distinct sets of conditions: either by illumination at room temperature or at 200 K in certain experimental conditions (g4(S) signal) or by near-infrared illumination between approximately 77 and approximately 160 K of the S(2)-multiline state (g4(IR) signal). The two g=4.1 signals arise from states which have quite different stability in terms of temperature. In the present work we have compared these two signals in order to test if they originate from the same or from different chemical origins. The microwave power saturation properties of the two signals measured at 4.2 K were found to be virtually identical. Their temperature dependencies measured at non-saturating powers were also identical. The presence of Curie law behavior for the g4(S) and g4(IR) signals indicates that the states responsible for both signals are ground states. The orientation dependence, anisotropy and resolved hyperfine structure of the two g4 signals were also found to be virtually indistinguishable. We have been unable to confirm the behavior reported earlier indicating that the g4(S) signal is an excited state, nor were we able to confirm the presence of signal from a higher excited state in samples containing the g4(S), nor a radical signal in samples containing the g4(IR). These findings are best interpreted assuming that the two signals have a common origin i.e. a spin 5/2 ground state arising from a magnetically coupled Mn-cluster of 4 Mn ions.

Effect of pH on the semiquinone radical Q(A)- in CN-treated photosystem II: study by hyperfine sublevel correlation spectroscopy

The semiquinone radical Q(A)- has been studied by electron spin echo envelope modulation (ESEEM) spectroscopy in Photosystem II membranes treated with CN- at various pH values. Two protein 14N nuclei (N(I) and N(II)) were found to be magnetically coupled with the Q(A)- spin. N(I) is assigned to an amide nitrogen from the protein backbone while N(II) is assigned to the amino nitrogen, N(epsilon), of an imidazole. Above pH 8.5 only the N(I) coupling is present while both N(I) and N(II) couplings are present at lower pH values. These results are interpreted in terms of a model based on the structure of the bacterial reaction center and involving two determining factors. First, the non-heme iron, when present, is ligated to the imidazole that H-bonds to one of the Q(A)- carbonyls. This physical attachment of the imidazole to the iron limits the strength of the H-bond to Q(A)-. Second, a pH-dependent group on the protein controls the strength of the H-bonds to Q(A)-. The pKa of this group is around pH 7.5 in CN(-)-treated PSII.

Inhibition of Photosystem II activity by saturating single turnover flashes in calcium-depleted and active Photosystem II

Inhibition of Photosystem II (PS II) activity induced by continuous light or by saturating single turnover flashes was investigated in Ca(2+)-depleted, Mn-depleted and active PS II enriched membrane fragments. While Ca(2+)- and Mn-depleted PS II were more damaged under continuous illumination, active PS II was more susceptible to flash-induced photoinhibition. The extent of photoinactivation as a function of the duration of the dark interval between the saturating single turnover flashes was investigated. The active centres showed the most photodamage when the time interval between the flashes was long enough (32 s) to allow for charge recombination between the S(2) or S(3) and Q(B) (-) to occur. Illumination with groups of consecutive flashes (spacing between the flashes 0.1 s followed by 32 s dark interval) resulted in a binary oscillation of the loss of PS II-activity in active samples as has been shown previously (Keren N, Gong H, Ohad I (1995), J Biol Chem 270: 806-814). Ca(2+)- and Mn-depleted PS II did not show this effect. The data are explained by assuming that charge recombination in active PS II results in a back reaction that generates P(680) triplet and thence singlet oxygen, while in Ca(2+)- and Mn-depleted PS II charge recombination occurs through a different pathway, that does not involve triplet generation. This correlates with an up-shift of the midpoint potential of Q(A) in samples lacking Ca(2+) or Mn that, in term, is predicted to result in the triplet generating pathway becoming thermodynamically less favourable (G.N. Johnson, A.W. Rutherford, A. Krieger, 1995, Biochim. Biophys. Acta 1229, 201-207). The diminished susceptibility to flash-induced photoinhibition in Ca(2+)- and Mn-depleted PS II is attributed at least in part to this mechanism.

Effects of copper and zinc ions on photosystem II studied by EPR spectroscopy

The effect of Zn(2+) or Cu(2+) ions on Mn-depleted photosystem II (PS II) has been investigated using EPR spectroscopy. In Zn(2+)-treated and Cu(2+)-treated PS II, chemical reduction with sodium dithionite gives rise to a signal attributed to the plastosemiquinone, Q(A)(*)(-), the usual interaction with the non-heme iron being lost. The signal was identified by Q-band EPR spectroscopy which partially resolves the typical g-anisotropy of the semiquinone anion radical. Illumination at 200 K of the unreduced samples gives rise to a single organic free radical in Cu(2+)-treated PS II, and this is assigned to a monomeric chlorophyll cation radical, Chl a(*)(+), based on its (1)H-ENDOR spectrum. The Zn(2+)-treated PS II under the same conditions gives rise to two radical signals present in equal amounts and attributed to the Chl a(*)(+) and the Q(A)(*)(-) formed by light-induced charge separation. When the Cu(2+)-treated PS II is reduced by sodium ascorbate, at >/=77 K electron donation eliminates the donor-side radical leaving the Q(A)(*)(-) EPR signal. The data are explained as follows: (1) Cu(2+) and Zn(2+) have similar effects on PS II (although higher concentrations of Zn(2+) are required) causing the displacement of the non-heme Fe(2+). (2) In both cases chlorophyll is the electron donor at 200 K. It is proposed that the lack of a light-induced Q(A)(*)(-) signal in the unreduced Cu(2+)-treated sample is due to Cu(2+) acting as an electron acceptor from Q(A)(*)(-) at low temperature, forming the Cu(+) state and leaving the electron donor radical Chl a(*)(+) detectable by EPR. (3) The Cu(2+) in PS II is chemically reducible by ascorbate prior to illumination, and the metal can therefore no longer act as an electron acceptor; thus Q(A)(*)(-) is generated by illumination in such samples. (4) With dithionite, both the Cu(2+) and the quinone are reduced resulting in the presence of Q(A)(*)(-) in the dark. The suggested high redox potential of Cu(2+) when in the Fe(2+) site in PS II is in contrast to the situation in the bacterial reaction center where it has been shown in earlier work that the Cu(2+) is unreduced by dithionite. It cannot be ruled out however that Q(A)-Cu(2+) is formed and a magnetic interaction is responsible for the lack of the Q(A)(-) signal when no exogenous reductant is present. With this alternative possibility, the effects of reductants would be explained as the loss of Cu(2+) (due to formation of Cu(+)) leading to loss of the Cu(2+) from the Fe(2+) site due to the binding equilibrium. The quite different binding and redox behavior of the metal in the iron site in PS II compared to that of the bacterial reaction center is presumably a further reflection of the differences in the coordination of the iron in the two systems.

Detection of an electron paramagnetic resonance signal in the S0 state of the manganese complex of photosystem II from Synechococcus elongatus

The Mn(4)-cluster of photosystem II (PSII) from Synechococcus elongatus was studied by electron paramagnetic resonance (EPR) spectroscopy after a series of saturating laser flashes given in the presence of either methanol or ethanol. Results were compared to those obtained in similar experiments done on PSII isolated from plants. The flash-dependent changes in amplitude of the EPR multiline signals were virtually identical in all samples. In agreement with earlier work [Messinger, J., Nugent, J. H. A., and Evans, M. C. W. (1997) Biochemistry 36, 11055-11060; Ahrling, K. A., Peterson, S., and Styring, S. (1997) Biochemistry 36, 13148-13152], detection of an EPR multiline signal from the S(0) state in PSII from plants was only possible with methanol present. In PSII from S. elongatus, it is shown that the S(0) state exhibits an EPR multiline signal in the absence of methanol (however, ethanol was present as a solvent for the artificial electron acceptor). The hyperfine lines are better resolved when methanol is present. The S(0) multiline signals detected in plant PSII and in S. elongatus were similar but not identical. Unlike the situation seen in plant PSII, the S(2) state in S. elongatus is not affected by the addition of methanol in that (i) the S(2) multiline EPR signal is not modified by methanol and (ii) the spin state of the S(2) state is affected by infrared light when methanol is present. It is also shown that the magnetic relaxation properties of an oxidized low-spin heme, attributed to cytochrome c(550), vary with the S states. This heme then is in the magnetic environment of the Mn(4) cluster.

Carotenoid oxidation in photosystem II

The oxidation of carotenoid upon illumination at low temperature has been studied in Mn-depleted photosystem II (PSII) using EPR and electronic absorption spectroscopy. Illumination of PSII at 20 K results in carotenoid cation radical (Car+*) formation in essentially all of the centers. When a sample which was preilluminated at 20 K was warmed in darkness to 120 K, Car+* was replaced by a chlorophyll cation radical. This suggests that carotenoid functions as an electron carrier between P680, the photooxidizable chlorophyll in PSII, and ChlZ, the monomeric chlorophyll which acts as a secondary electron donor under some conditions. By correlating with the absorption spectra at different temperatures, specific EPR signals from Car+* and ChlZ+* are distinguished in terms of their g-values and widths. When cytochrome b559 (Cyt b559) is prereduced, illumination at 20 K results in the oxidation of Cyt b559 without the prior formation of a stable Car+*. Although these results can be reconciled with a linear pathway, they are more straightforwardly explained in terms of a branched electron-transfer pathway, where Car is a direct electron donor to P680(+), while Cyt b559 and ChlZ are both capable of donating electrons to Car+*, and where the ChlZ donates electrons when Cyt b559 is oxidized prior to illumination. These results have significant repercussions on the current thinking concerning the protective role of the Cyt b559/ChlZ electron-transfer pathways and on structural models of PSII.

Influence of herbicide binding on the redox potential of the quinone acceptor in photosystem II: relevance to photodamage and phytotoxicity

Here we show that herbicide binding influences the redox potential (Em) of the plastoquinone QA/QA- redox couple in Photosystem II (PSII). Phenolic herbicides lower the Em by approximately 45 mV, while DCMU raises the Em by 50 mV. These shifts are reflected in changes in the peak temperature of thermoluminescence bands arising from the recombination of charge pairs involving QA-. The herbicide-induced changes in the Em of QA/QA- correlate with earlier work showing that phenolic herbicides increase the sensitivity of PSII to light, while DCMU protects against photodamage. This correlation is explained in terms of the following hypothesis which is based on reactions occurring in the bacterial reaction center. The back-reaction pathway for P680+QA- is assumed to be modulated by the free-energy gap between the P680+QA- and the P680+Ph- radical pairs. When this gap is small (i.e., when the Em of QA/QA- is lowered), a true back-reaction is favored in which P680+Ph- is formed, a state which decays forming a significant yield of P680 triplet. This triplet state of chlorophyll reacts with oxygen, forming singlet oxygen, a species likely to be responsible for photodamage. When the free-energy gap is increased (i.e., when the Em of QA/QA- is raised), the yield of the P680+Ph- is diminished and a greater proportion of the P680+QA- radical pair decays by an alternative, less damaging, route. We propose that at least some of the phytotoxic properties of phenolic herbicides may be explained by the fact that they render PSII ultrasensitive to light due to this mechanism.

Relationship between activity, D1 loss, and Mn binding in photoinhibition of photosystem II

Photoinhibition of photosystem II (PSII) activity and loss of the D1 reaction center protein were studied in PSII-enriched membrane fragments in which the water-splitting complex was inhibited by depletion of either calcium or chloride or by removing manganese. The Ca2+-depleted PSII was found to be the least susceptible to inhibition by light as reported previously (Krieger, A., and Rutherford, A. W. (1997) Biochim. Biophys. Acta 1319, 91-98). This different susceptibility to light was not reflected in the extent of D1 protein loss. In Mn-depleted PSII the loss of activity and the loss of the D1 protein were correlated, while in Cl-- and Ca2+-depleted PSII, there was very little loss of the D1 protein. The production of free radicals and singlet oxygen was measured by EPR spin-trapping techniques in the different samples. 1O2 and carbon-centered radicals could be detected after photoinhibition of active PSII, while hydroxyl radical formation dominated in all of the other samples. In addition, photoinhibition of PSII was investigated in which the functional Mn cluster was reconstituted (i. e., photoactivated). As expected this led to a protection against photoinhibition. When the photoactivation procedure was done in the absence of Ca2+ no activity was obtained although a nonfunctional Mn cluster was formed. Despite the lack of activity the binding of Mn partially protected against the loss of D1. These data demonstrate that, during photoinhibition, the extent of D1 loss is neither affected by the water-splitting activity of the sample nor correlated to the kinetics of PSII activity loss. D1 loss seems to be independent of the chemical nature of the reactive oxygen species formed during photoinhibition and seems to occur only in the absence of Mn. It is proposed that Mn binding protects against D1 loss by maintaining a protein structure which is not accessible to cleavage.

Reaction centre photochemistry in cyanide-treated photosystem II

EPR was used to study the triplet state of chlorophyll generated by radical pair recombination in the photosystem II (PSII) reaction centre. The spin state of the non-haem Fe2+ was varied using the CN--binding method (Y. Sanakis, V. Petrouleas, B.A. Diner, Biochemistry 33 (1994) 9922-9928) and the redox state of the quinone acceptor (QA) was changed from semi-reduced to fully reduced (F.J.E. van Mieghem, W. Nitschke, P. Mathis, A.W. Rutherford, Biochim. Biophys. Acta 977 (1989) 207-214). It was found that the triplet was not detectable using continuous wave EPR when QA- was present irrespective of the spin-state of the Fe2+. It was also found that the triplet state became detectable by EPR when the semiquinone was removed (by reduction to the quinol) and that the triplet observed was not influenced by the spin state of the Fe2+. Since it is known from earlier work that the EPR detection of the triplet reflects a change in the triplet lifetime, it is concluded that the redox state of the quinone determines the triplet lifetime (at least in terms of its detectability by continuous wave EPR) and that the magnetic state of the iron, (through the weakly exchange-coupled QA- Fe2+ complex) is not a determining factor. In addition, we looked for polarisation transfer from the radical pair to QA- in PSII where the Fe2+ was low spin. Such polarisation is seen in bacterial reaction centres under comparable conditions. In PSII, however, we were unable to find evidence for such polarisation of the semiquinone. It is suggested that both the short triplet lifetime in the presence of QA- and the lack of polarised QA- might be explained in terms of the electron transfer mechanism for triplet quenching involving the semiquinone which was proposed previously (F.J.E. van Mieghem, K. Brettel, B. Hillmann, A. Kamlowski, A.W. Rutherford, E. Schlodder, Biochemistry 34 (1995) 4798-4813). It is suggested that this mechanism may occur in PSII (but not in purple bacterial reaction centres) due the triplet-bearing chlorophyll being adjacent to the pheophytin at low temperature as suggested from structural studies (F.J.E. van Mieghem, K. Satoh, A.W. Rutherford, Biochim. Biophys. Acta 1058 (1992) 379-385).

Effect of near-infrared light on the S2-state of the manganese complex of photosystem II from Synechococcus elongatus

The Mn cluster of Photosystem II (PSII) from Synechococcus elongatus was studied using EPR. A signal with features between g = 5 and g = 9 is reported from the S2-state. The signal is attributed to the manganese cluster in a state with a spin 5/2 state. Spectral simulations of the signal indicate zero field splitting parameters where the |E/D| was 0.13. The new signal is formed by irradiating PSII samples which contain the spin = 1/2 S2-state using 813 nm light below 200 K. This effect is attributed to a spin-state change in the manganese cluster due to absorption of the IR light by the Mn-cluster itself. The signal is similar to that reported recently in PSII of plants [Boussac, A., Un, S., Horner, O., and Rutherford, A. W. (1998) Biochemistry 37, 4001-4007]. In plant PSII the comparable signal is formed at a lower temperature (optimally below 77 K), and gradual warming of the sample in the dark leads to the formation of the state responsible for the well-known g = 4.1 signal prior to formation of the spin 1/2 multiline signal. In the present work using cyanobacterial PSII, warming of the sample in the dark leads to the formation of the spin 1/2 multiline signal without formation of the g = 4 type signal as an intermediate. These observations provide a partial explanation for the long-standing "mystery of the missing g = 4 state" in cyanobacterial PSII. The observations are rationalized in terms of three possible states which can exist for S2: (i) the spin 1/2 multiline signal, (ii) the state responsible for the g = 4.1 signal, and (iii) the new spin 5/2 state. The relative stability of these states differs between plants and cyanobacteria.

The 18 kDa cytochrome c553 from Heliobacterium gestii: gene sequence and characterization of the mature protein

The 18 kDa cytochrome c553 is the dominant c-type cytochrome in cell membranes of Heliobacterium gestii. After solubilization, this cytochrome was purified in three steps as a complex with two other proteins of 32 and 42 kDa. The redox midpoint potential of the cytochrome c553 was determined to be +215 mV. The EPR spectra clearly show the presence of an ascorbate-reducible low-spin heme with gz = 3.048 and gy = 2.238. The gx = trough could not be detected. In addition, a Cu(II) signal with g = 2.058 was observed, indicating that one component of the cytochrome c553 complex contains a bound copper ion. The gene for the 18 kDa cytochrome c553, cyhA, consists of 429 bp coding for a protein of 142 amino acids. The association of the cytochrome with the cytoplasmic membrane is mediated by two fatty acid molecules, one palmitate and one stearate, that could be identified by mass spectrometry. Both fatty acids are most likely bound to the cysteine residue of the N-terminally processed protein via a glycerol moiety. The amino acid sequence deduced from the DNA sequence exhibits partial identity to the membrane-bound cytochrome c551 from Bacillus PS3 [Fujiwara, Y., Oka, M., Hamamoto, T., and Sone, N. (1993) Biochem. Biophys. Res. Commun. 1144, 213-219] and to the cytochrome c subunit (NorC) of the nitrous reductase from Pseudomonas stutzeri [Zumft, W. G., Braun, C., and Cuypers, H. (1994) Eur. J. Biochem. 219, 481-490].

High-spin states (S >/= 5/2) of the photosystem II manganese complex

The Mn4 complex which is involved in water oxidation in photosystem II (PSII) is known to exhibit two types of EPR signals in the S2 state, one of the five redox states of the enzyme cycle: either a multiline signal (S = 1/2) or a signal at g = 4.1 (S = 3/2 or S= 5/2). The S = 1/2 state can be converted to that responsible for the g = 4.1 signal upon the absorption of near-infrared (IR) light [Boussac, A., Girerd, J.-J., and Rutherford, A.W. (1996) Biochemistry 35, 6984-6989]. It is shown here that a third state gives rise to signals at g = 10 and 6. This state is formed by IR illumination of the S = 1/2 state at 65 K, a temperature where IR illumination leads to the loss of the S = 1/2 signal but to no formation of the g = 4.1 state. On the basis of the corresponding decrease of the S = 1/2 state, the new state can be trapped in approximately 40% of the PSII centers. Warming of the sample above 65 K, in the dark, leads to the loss of the g = 10 and 6 resonances with the corresponding appearance of the g = 4.1 signal. It is suggested that the IR-induced conversion of the S = 1/2 state into the g = 4.1 state at 150 K involves the transient formation of the new state. The new state is attributed to a S = 5/2 state of the Mn4 complex (although a S value > 5/2 is also a possibility). Spectral simulations indicate an E/D ratio of -0.05 with D </= 1 cm-1. The resonances at g = 10 and 6 correspond to the gz of the +/-5/2 and +/-3/2 transition, respectively. The temperature-dependent conversion of this S = 5/2 state into the g = 4.1 state is proposed to be due to relaxation of the ligand environment around the Mn4 cluster that leads to a change in the zero field splitting parameters, assuming an S = 5/2 value for the g = 4.1 state. The new form of the S2 state reported here may explain some earlier data where the S2 state was present and yet not detectable as either a S = 1/2 or a g = 4.1 EPR signal.

Spin-lattice relaxation of the phyllosemiquinone radical of photosystem I

The spin-lattice relaxation time (T1) of the phyllosemiquinone anion radical, A1-, of the photosystem I (PSI) reaction center, were measured between 4.5 and 85 K by electron spin-echo spectroscopy. The selective removal of the iron-sulfur centers, FA, FB, and FX, from PSI allowed the measurement of the intrinsic T1 of the A1- radical. The temperature dependence of the intrinsic (T1)-1 for A1- was found to be approximately T1.3 +/- 0.1. The spin-lattice relaxation of the reduced form of iron-sulfur center FX was also measured at low temperatures, in FA/FB-depleted PSI membranes. It was found that the fast-relaxing FX center enhances the spin-lattice relaxation of the phyllosemiquinone due to dipolar coupling. The effect of the reduced forms of FA/FB on the T1 of the phyllosemiquinone was minor compared to the effect of FX. By analyzing the data with a dipolar model in the light of limitations imposed by other information present in the literature, the distance between the phyllosemiquinone and FX in PSI is estimated to be 14.8 +/- 4 A.

A systematic survey of conserved histidines in the core subunits of Photosystem I by site-directed mutagenesis reveals the likely axial ligands of P700

The Photosystem I complex catalyses the transfer of an electron from lumenal plastocyanin to stromal ferredoxin, using the energy of an absorbed photon. The initial photochemical event is the transfer of an electron from the excited state of P700, a pair of chlorophylls, to a monomer chlorophyll serving as the primary electron acceptor. We have performed a systematic survey of conserved histidines in the last six transmembrane segments of the related polytopic membrane proteins PsaA and PsaB in the green alga Chlamydomonas reinhardtii. These histidines, which are present in analogous positions in both proteins, were changed to glutamine or leucine by site-directed mutagenesis. Double mutants in which both histidines had been changed to glutamine were screened for changes in the characteristics of P700 using electron paramagnetic resonance, Fourier transform infrared and visible spectroscopy. Only mutations in the histidines of helix 10 (PsaA-His676 and PsaB-His656) resulted in changes in spectroscopic properties of P700, leading us to conclude that these histidines are most likely the axial ligands to the P700 chlorophylls.

ESEEM study of the phyllosemiquinone radical A1.- in 14N- and 15N-labeled photosystem I

The phyllosemiquinone radical of the photosystem I reaction center has been studied by electron spin echo envelope modulation (ESEEM) spectroscopy. A comparative analysis of ESEEM data of the semiquinone in 14N- and 15N-labeled PSI and numerical simulations demonstrate the existence of two protein nitrogen nuclei coupled to the semiquinone. One of the 14N couplings is characterized by a quadrupolar coupling constant e2qQ/4h of 0.77 MHz, an asymmetry parameter eta of 0.18, and a hyperfine coupling tensor with an almost pure isotropic hyperfine coupling, i.e. (Axx, Ayy, Azz) = (1.3, 1.3, 1.5 MHz). The second nitrogen coupling is characterized by a quadrupolar coupling constant e2qQ/4h of 0.45 MHz, an asymmetry parameter eta of 0.85, and a weak hyperfine coupling tensor with a dominant anisotropic part, i.e. (Axx, Ayy, Azz) = (-0.2, -0.2, 1.5 MHz). On the basis of a comparison of the 14N-ESEEM data with 14N-NQR and 14N-ESEEM data from the literature, the first coupled nitrogen is assigned to the indole nitrogen of a tryptophan residue. The coupling of the second nitrogen is much weaker and therefore more difficult to assign. However, the simulated spectrum best describes an amino nitrogen of a histidine, although the amide group of an asparagine or glutamine cannot be ruled out. The possible origins of teh nitrogen hyperfine coupling are discussed in terms of the amino acid residues thought to be close to the semiquinone in PSI.

Orientation of the phylloquinone electron acceptor anion radical in photosystem I

The photosynthetic reaction center of photosystem I (PS I) contains a phylloquinone molecule (A1) which acts as a transient electron acceptor. In PS I form the cyanobacterium Synechocystis PCC 6803 under reducing conditions, we have photoaccumulated an EPR signal assigned to the phylloquinone radical anion. The phylloquinone EPR spectrum has been studied in oriented multilayers of PS I using EPR at 9 GHz. In addition, the phyllosemiquinone spectrum has been obtained at 283 GHz using high-field, high-frequency EPR spectroscopy. From the orientation dependence of the spectrum at 9 GHz and the resolved g values obtained at 283 GHz, the phyllosemiquinone ring plane was determined to be almost perpendicular to the membrane (76 degrees) while the oxygen-oxygen (O-O) axis of the quinone was found to make an approximate 63 degrees angle to the membrane plane. The orientation of the ring plane is similar to that determined for the quinone electron acceptor (QA) in the purple bacterial reaction center, while the orientation of the O-O axis is significantly different. The new orientation information, when taken with data in the literature, allows the position of the phylloquinone in the reaction center to be better defined.

Site-directed mutations near the L-subunit D-helix of the purple bacterial reaction center: a partial model for the primary donor of photosystem II

We have engineered a photosynthetically competent mutant of the purple non-sulfur bacterium Rhodobacter capsulatus which seeks to mimic the behavior of the primary electron donor (P) of the plant photosystem II (PS II) reaction center (RC). To construct this mutant (denoted D1-ILMH), four residues in the bacterial L subunit were mutagenized, such that an 11-residue segment was made identical to the analogous segment from the D1 subunit of PS II. The electronic properties of the bacteriochlorophyll (Bchl) dimer which constitutes the primary donor are substantially altered by these modifications, to the degree that the dimer becomes functionally much more "monomeric". The changes include (1) an increase in the values of the zero-field splitting (ZFS) parameters, as measured by electron paramagnetic resonance (EPR), for the spin-polarized triplet state, 3P, from /D/ = 185 x 10(-4) cm(-1) and /E/ = 31 x 10(-4) cm(-1) in wild-type (WT) chromatophore membranes to /D/ = 200 x 10(-4) cm(-1) and /E/ = 44 x 10(-4) cm(-1) in the mutant and (2) an increase in the EPR line width of the oxidized state, P+, from 0.97 mT in WT to 1.09 mT in D1-ILMH RCs. However, unlike the PS II primary donor (P680), the orientation of 3P in the D1-ILMH mutant is the same as in WT bacteria and does not display the unusual orientation found for PS II. And whereas the redox couple P/P+ has a very high midpoint potential in PS II, P/P+ in the D1-ILMH mutant has a lower midpoint (90 mV more negative) than in WT Rb. capsulatus. In addition, Raman measurements indicate that the hydrogen bond between HisL168 and the C2 acetyl carbonyl oxygen of the Bchl on the active electron transfer pathway (P(A)) is absent in the mutant, due to the fact that HisL168 in the WT sequence has been replaced by a leucine in D1-ILMH. However, the Raman data also reveal the presence of a new hydrogen bond in the D1-ILMH RCs, between the C9 keto carbonyl oxygen of P(A) and an unknown hydrogen-bond donor. Thus, although the protein environment around one of the Bchls of the special pair is significantly changed in D1-ILMH, the chimeric RC does not, as a result of these changes, have a primary donor that is oriented like the one in PS II.

Membrane-bound c-type cytochromes in Heliobacillus mobilis. Characterisation by EPR and optical spectroscopy in membranes and detergent-solubilised material

The spectral and electrochemical parameters, as well as the orientations of the heme plane with respect to the membrane plane, of the c-type hemes present in membrane fragments from Heliobacillus mobilis were characterised by optical and EPR spectroscopy. Cytochrome C53, was thereby shown to represent at least four and possibly five heme species with the following characteristics: Em = -60 mV +/- 10 mV, g, = 2.92, 60 degrees; Em = +90 mV +/- 10 mV, g, = 2.92, 90 degrees; Em = +120 mV +/- 20 mV, g, = 3.03; and Em = +170 mV +/- 20 mV, g, = 3.03. The latter component may correspond to two hemes with redox midpoint potentials of Em = +160 mV +/- 20 mV and Em = +180 mV +/- 20 mV (all Em values at pH 7.0). For the heme species having g, peaks at g approximately 3.03, determination of individual orientations was precluded due to the superposition of several differently oriented hemes. About one copy of each heme was found to be present per photosynthetic reaction centre, with the exception of the +120 mV component for which a stoichiometry of 2 hemes/reaction centre was obtained. The heme proteins were detergent-solubilised and partially purified. Three c-type cytochromes that migrated with apparent molecular masses of 18, 29 and 50 kDa were detected on SDS/PAGE. Optical redox titrations at pH 7.0 showed redox midpoint potentials of +160 mV +/- 10 mV for the 18-kDa cytochrome, and -60 mV +/- 10 mV, with possible contributions around +160 mV, for the 50-kDa cytochrome. A tentative attribution of heme species observed in membranes to the isolated heme proteins is presented. The results obtained on H. mobilis are compared with those reported for green sulphur bacteria.

Location of the calcium binding site in Photosystem II: A Mn2+ substitution study

The whereabouts of the Ca²⁺ site in Photosystem II (PSII) was investigated by experiments in which Mn²⁺ was substituted for Ca²⁺. When stoichiometric amounts of Mn²⁺ ions were added to Ca²⁺-depleted PSII, the Mn²⁺ was not detected by EPR. The titration of Ca²⁺ back into Ca²⁺-depleted/Mn²⁺-containing PSII resulted in the simultaneous release of the Mn²⁺ and the loss of the two EPR signals which are characteristic of the Ca²⁺-depleted enzyme (i.e., the stable, modified S₂ multiline signal arising from the intrinsic Mn cluster and the split S₃ signal from an organic radical interacting with the Mn cluster). These results indicate that the Mn²⁺ occupies the functional Ca²⁺ site. The S₂ and S₃ EPR signal characteristic of this kind of Ca²⁺-depleted preparation were unaffected by the binding of the Mn²⁺ Since, from earlier results, it seems likely that the modification and stability of S₂ multiline signal in these PSII preparations is due to binding of chelator to or close to the Mn cluster, the present results indicate that the Ca²⁺ site (at least when occupied by Mn²⁺) does not overlap with the chelator binding site. Since Mn²⁺ binding does not effect the S₂ EPR signal from the Mn cluster, it can be concluded that the Mn²⁺ is not involved in detectable magnetic interactions with the cluster. This result indicates that the Mn²⁺-occupied Ca²⁺ binding site is outside the first co-ordination sphere of the Mn cluster. The relaxation properties of TyrD^. were enhanced by the presence of the Mn²⁺ when the Mn cluster was in the S₁ state.

The role of the extrinsic 33 kDa protein in Ca2+ binding in photosystem II

The role of the 33 kDa protein in Ca2+ binding was studied by comparing the EPR properties of photosystem II in the presence and absence of the 33 kDa protein and Ca2+. When the removal of the 33 kDa protein was carried out in the dark, a normal manganese multiline EPR signal could be observed when the S2 state was generated. In addition, the split S3 signal could not be generated by illumination at 273 K. Exposure of the 33 kDa protein-less photosystem II to room light did not lead to any change in the EPR properties of the S2 state, but the split S3 state signal at around g = 2 could then be generated, indicating that Ca2+ was released from this preparation during the exposure to light. Treatment of photosystem II lacking the 33 kDa protein with EGTA in the light led to a modification of the S2 state characterized by a dark-stable multiline EPR signal. Much lower EGTA concentrations were required in order to obtain this modification in the absence of the 33 kDa protein than was required when the 33 kDa protein was present. This indicates that the manganese cluster was more accessible to chelator binding when the 33 kDa protein was absent. When 33 kDa protein-less photosystem II was treated with EGTA in the dark, no modification of the multiline EPR signal of the S2 state of the manganese cluster occurred, nor was Ca2+ released as monitored by the inability to generate the split S3 signal. These chelator- and Ca(2+)-binding properties occurring in PSII lacking the 33 kDa protein are very similar to those observed previously in NaCl-washed PSII in which the 33 kDa protein is present (reviewed in Boussac & Rutherford, 1994a). It is concluded that the 33 kDa protein has little or no direct role in binding the Ca2+ ion which is required for oxygen evolution.

Spin-lattice relaxation of the pheophytin, Pheo-, radical of photosystem II

The spin-lattice relaxation times (T1) of the pheophytin anion radical, Pheo-, of the PSII reaction center, were measured between 5 and 80 K by electron spin-echo spectroscopy. The Pheo- was studied in Mn-depleted PSII reaction centers in which the primary quinone, QA, was doubly reduced. The selective conversion of the non-heme Fe2+ into its low-spin (S = O) state, in CN-treated PSII, allowed the measurement of the intrinsic T1 of the Pheo- radical. The temperature dependence of the intrinsic (T1)-1 was found to be approximately T1.3 +/- 0.1. In Mn-depleted PSII membranes the high-spin (S = 2) non-heme iron, enhances the spin-lattice relaxation of Pheo-. By analyzing the data with a dipolar model, the dipolar interaction (k1d) between the Pheo and the Fe2+ (S = 2) is estimated over the temperature range 5-80 K. Comparison with the dipolar coupling between the iron and the tyrosine, YD+, shows that the Pheo is much closer to the iron than the YD+ in the PSII reaction center. By scaling the reported Fe(2+)-YD+ distance by the ratio [k1dPheo-]/[k1dYD+], we estimate the Fe(2+)-Pheo- distance in PSII to be 20 +/- 4.2 A. This distance is close to the Fe(2+)-BPheo- distance in the bacterial reaction center, and this result provides further evidence that the acceptor sides of the reaction centers in PSII and bacteria are homologous.

Conversion of the spin state of the manganese complex in photosystem II induced by near-infrared light

The manganese complex (Mn4) which is responsible for water oxidation in photosystem II is EPR detectable in the S2 state, one of the five redox states of the enzyme cycle. The S2 state is observable at 10 K either as a multiline signal (spin 1/2) or as a signal at g = 4.1 (spin 3/2 or spin 5/2). It is shown here that at around 150 K the state responsible for the multiline signal is converted to that responsible for the g = 4.1 signal upon the absorption of infrared light. This conversion is fully reversible at 200 K. The action spectrum of this conversion has its maximum at 820 nm (12 200 cm-1) and is similar to the intervalence charge transfer band in di-mu-oxo-(MnIIIMnIV) model systems. It is suggested that the conversion of the multiline signal to the g = 4.1 signal results from absorption of infrared light by the Mn cluster itself, resulting in electron transfer from MnIII to MnIV. The g = 4.1 signal is thus proposed to arise from a state which differs from that which gives rise to the multiline signal only in terms of this change in its valence distribution. The near-infrared light effect was observed in the S2 state of Sr(2+)-reconstituted photosystem II and in Ca(2+)-depleted, EGTA (or citrate-)-treated photosystem II but not in ammonia-treated photosystem II. Earlier results in the literature which showed that the g = 4.1 state was preferentially formed by illumination at 130 K are reinterpreted as being the result of two photochemical events: the first being photosynthetic charge separation resulting in an S2 state which gives rise to the multiline signal and the second being the conversion of this state to the g = 4.1 state due to the simultaneous and inadvertent presence of 820 nm light in the broad-band illumination given. There is therefore no reason to consider the state responsible for the g = 4.1 signal as a precursor of that which gives rise to the multiline signal.

On the role of the N-terminus of the extrinsic 33 kDa protein of Photosystem II

The role of the N-terminus of the extrinsic 33 kDa protein of Photosystem II has been investigated by means of site-directed mutagenesis and cross-linking. Replacement of Asp-9 resulted in a dramatic increase in proteolytic sensitivity leading to the degradation of the protein forming a 31 kDa fragment with an undefined N-terminus. This fragment was unable to restore oxygen evolution. However, the variants of the 33 kDa protein which remained intact could reconstitute oxygen evolution as effectively as the wild-type protein. Cross-linking experiments with a water-soluble carbodiimide revealed that mutagenesis of residue D9 led to the disruption of an intramolecular salt bridge. Therefore we suggest that the N-terminus of the 33 kDa protein is necessary for maintaining the binding ability of the protein to Photosystem II but might not be involved in binding itself.

Properties of the chloride-depleted oxygen-evolving complex of photosystem II studied by electron paramagnetic resonance

The effects of different Cl- depletion treatments in photosystem II (PS-II)-enriched membranes have been investigated by electron paramagnetic resonance (EPR) spectroscopy and by measurements of oxygen-evolving activity. The results indicated that the oxygen-evolving complex of PS-II exhibits two distinct Cl(-)-dependent properties. (1) After Cl(-)-free washes at pH 6.3, a reversibly altered distribution of structural states of PS-II was observed, manifested as the appearance of a g = 4 EPR signal from the S2 state in a significant fraction of centers (20-40%) at the expense of the S2 multiline signal. In addition, small but significant changes in the shape of the S2 multiline EPR signal were observed. Reconstitution of Cl- to Cl(-)-free washed PS-II rapidly reversed the observed effects of the Cl(-)-free washing. The anions, SO4(2-) and F-, which are often used during Cl- depletion treatments, had no effect on the S2 EPR properties of PS-II under these conditions in the absence or presence of Cl-. Flash experiments and measurements of oxygen evolution versus light intensity indicated that the two structural states observed after the removal of Cl- at pH 6.3 originated from oxygen-evolving centers exhibiting a lowered quantum yield of water oxidation. (2) Depletion of Cl- in PS-II by pH 10 treatment reversibly inhibited the oxygen-evolving activity to approximately 15%. The pH 10 treatment depleted the Cl- from a site which is considered to be equivalent to that studied in most earlier work on Cl(-)-depleted PS-II. The S2 state in pH 10/Cl(-)-depleted PS-II was reversibly modified to a state from which no S2 multiline EPR signal was generated and which exhibited an intense S2 g = 4 EPR signal corresponding to at least 40% of the centers but possibly to a much larger fraction of centers. The state responsible for the intense S2 g = 4 signal generated under these conditions is unlike that observed after removal of Cl- from PS-II at pH 6.3, in that this state was more stable in the dark, showing a half-decay time of approximately 1.5 h at 0 degrees C, and was unable to undergo further charge accumulation. Nevertheless, a fraction of centers, probably different from those exhibiting the S2 g = 4 signal, was able to advance to the formal S3 state, giving rise to a narrow EPR signal around g = 2. Addition of the anions SO4(2-) or F- to pH 10/Cl(-)-depleted PS-II affected the properties of PS-II, resulting in EPR properties of the S2 state similar to those reported earlier following Cl- depletion treatment of PS-II in the presence of these anions. Surprisingly, after addition of F-, the g = 4 EPR signal showed a damped flash-dependent oscillation. In addition, a narrow signal around g = 2, corresponding to the formal S3 state, also showed a damped flash-dependent oscillation pattern. The presence of oscillating EPR signals (albeit damped) in F(-)-treated pH 10/Cl(-)-depleted PS-II indicates functional enzyme turnover. This was confirmed by measurements of the oxygen-evolving activity versus light intensity which indicated that in approximately 45% of oxygen-evolving centers the enzyme turnover was slowed by a factor of 2. The distinct Cl- depletion effects in PS-II observed under the two different Cl- depletion treatments are considered to reflect the presence of two distinct Cl(-)-binding sites in PS-II.

ESEEM study of the plastoquinone anion radical (QA.--) in 14N- and 15N-labeled photosystem II treated with CN

The nonheme iron of the photosystem II reaction center was converted to its low-spin state (S = 0) by treatment with CN-. This allowed the study of the plastoquinone, QA- anion radical by electron spin-echo envelope modulation (ESEEM) spectroscopy. A comparative analysis of the ESEEM data of QA- in 14N- and 15N-labeled PSII demonstrates the existence of a protein nitrogen nucleus coupled to the QA-. The 14N coupling is characterized by a quadrupolar coupling constant e2qQ/4h = 0.82 MHz, an asymmetry parameter eta = 0.45, and hyperfine coupling constant A approximately 2.1 MHz. The 15N hyperfine coupling is characterized by T = 0.41 MHz and alpha iso approximately 3.3 MHz. The possible origins of the nitrogen hyperfine coupling are discussed in terms of the amino acids thought to be close to the QA- in PSII. Based on a comparison of the 14N ESEEM with 14N-NQR and 14N-ESEEM data from the literature, the most likely candidate is the amide nitrogen of the peptide backbone of Ala261 of the polypeptide D2, although the indole nitrogen of Trp254 and the imino nitrogen of His215 of D2 also remain candidates.

Charge recombination reactions in photosystem II. I. Yields, recombination pathways, and kinetics of the primary pair

Recombination reactions of the primary radical pair in photosystem II (PS II) have been studied in the nanosecond to millisecond time scales by flash absorption spectroscopy. Samples in which the first quinone acceptor (QA) was in the semiquinone form (QA-) or in the doubly reduced state (presumably QAH2) were used. The redox state of QA and the long-lived triplet state of the primary electron donor chlorophyll (3P680) were monitored by EPR. The following results were obtained at cryogenic temperatures (around 20 K). (1) the primary radical pair, P680+Pheo-, is formed with a high yield irrespective of the redox state of QA. (2) The decay of the primary pair is faster with QA- than with QAH2 and could be described biexponentially with t1/2 approximately 20 ns (approximately 65%)/150 ns (approximately 35%) and t1/2 approximately 60 ns (approximately 35%)/250 ns (approximately 65%), respectively. The different kinetics may be due to electrostatic and/or magnetic effects of QA- on charge recombination or due to conformational changes caused by the double reduction treatment. (3) The yield of the triplet state 3P680 was high both with QA- and QAH2. (4) The triplet decay was much faster with QA- [t1/2 approximately 2 microseconds (approximately 50%)/20 microseconds (approximately 50%)] than with QAH2 [t1/2 approximately 1 ms (approximately 65%)/3 ms (approximately 35%)]. The short lifetime of the triplet with QA- explains why it was not detected earlier. The mechanism of triplet quenching in the presence of QA- is not understood; however it may represent a protective process in PS II. (5) Almost identical data were obtained for PS II-enriched membranes from spinach and PS II core preparations from Synechococcus. Room temperature optical studies were performed on the Synechococcus preparation. In samples containing sodium dithionite to form QA- in the dark, EPR controls showed that multiple excitation flashes given at room temperature led to a decrease of the QA-Fe2+ signal, indicating double reduction of QA. During the first few flashes, QA- was still present in the large majority of the centers. In this case, the yield of the primary pair at room temperature was around 50%, and its decay could be described monoexponentially with t1/2 approximately 8 ns (a slightly better fit was obtained with two exponentials: t1/2 approximately 4 ns (approximately 80%)/25 ns (approximately 20%).(ABSTRACT TRUNCATED AT 400 WORDS)

Charge recombination reactions in photosystem II. 2. Transient absorbance difference spectra and their temperature dependence

Absorbance difference spectra of the transient states in photosystem II (PS II) have been examined in the Qv absorption region between 660 and 700 nm. The P680+Pheo-/P680Pheo, 3P680/P680, and P680+QA-/P680QA spectra were measured in O2-evolving PS II core complexes from Synechococcus and PS II-enriched membrane fragments from spinach. The low-temperature absorbance difference spectra vary only slightly between both PS II preparations. The 3P680/P680 spectrum is characterized by a bleaching at 685 nm at 25 K and indicates weak exciton coupling with neighboring pigment(s). We conclude that P680 absorbs at 685 nm in more intact PS II preparations at cryogenic temperature. The difference spectra of the radical pairs are strongly temperature dependent. At low temperature the P680+QA-/P680QA- spectrum exhibits the strongest bleaching at 675 nm whereas the P680+Phe-/P680Pheo spectra show two distinct bleaching bands at 674 and 684 nm. It is suggested that an electrochronic red shift resulting in a bleaching at 675 nm and an absorbance increase at about 682 nm dominates the spectral features of the charge-separated states. On the basis of the present results and those in the literature, we conclude that the interactions between the pigments and especially the organization of the primary donor must be quite different in PS II compared to bacterial reaction centers, although the basic structural arrangement of the pigments might be similar. Spectral data obtained with samples in the presence of singly and doubly reduced QA indicate that the primary photochemistry in PS II is not strongly influenced by the redox state of QA at low temperature and confirm the results of the accompanying paper [Van Mieghem, F. J. E., Brettel, K., Hillmann, B., Kamlowski, A., Rutherford, A. W., & Schlodder, E. (1995) Biochemistry 34, 4798-4813]. The spectra of the primary radical pair and the reaction center triplet obtained with more intact PS II preparations differ widely from those of D1/D2/cyt b-559 complexes. In the latter sample, where 3P680 formation results in a bleaching at 680 nm, the P680+Pheo-/P680Pheo spectrum shows only one broad bleaching band at about 680 nm, and the main bleaching due to photoaccumulation of Pheo- at 77 K appears at 682 nm instead of 685 nm in PS II core complexes. This indicates that the removal of the core antenna which is accompanied by the loss of QA causes also structural changes of the reaction center.

Chloride-depletion effects in the calcium-deficient oxygen-evolving complex of photosystem II

The effects of Cl-depletion in photosystem II (PS-II)-enriched membranes have been investigated by electron paramagnetic resonance (EPR) spectroscopy after removal of the 17- and 23-kDa polypeptides and depletion of Ca2+ by NaCl treatment. When the salt treatment was done in the presence of a high concentration (5 mM) of the chelator [ethylenebis(oxyethylenenitrilo)]tetraacetic acid (EGTA), a modified dark-stable multiline signal was observed from the S2 state and a 13 mT wide S3 signal could be generated by illumination at 0 degrees C as reported previously for experiments conducted under these conditions [Boussac, A., Zimmermann, J.-L., & Rutherford, A. W. (1990) FEBS Lett. 277, 69-74]. The modified S2 multiline signal was lost after a further Cl- depletion in the presence of a low EGTA concentration (50 microM). Upon Cl- reconstitution, a normal S2 multiline signal could be generated by continuous illumination at 200 K. In contrast, a lowering of the EGTA concentration (50 microM) alone, in the presence of Cl- (30 mM), had no effect on the modified S2 multiline signal. These results indicate that the modification of S2 is due to binding of the chelator to PS-II and that Cl- stabilizes the chelator binding. When Cl- depletion in Ca(2+)-depleted PS-II was done in the presence of a high concentration of EGTA (5 mM), the modified S2 multiline signal disappeared but was regenerated by Cl- reconstitution in darkness. These results indicate that when Cl- depletion is done to the EGTA-modified PS-II, the S2 multiline signal disappears but the S2 state remains stable in the dark.(ABSTRACT TRUNCATED AT 250 WORDS)

Structural and functional consequences of a Glu L212-->Lys mutation in the QB binding site of the photosynthetic reaction center of Rhodopseudomonas viridis

The properties of the quinone acceptor complex in the photosynthetic reaction center of the atrazine-resistant Rhodopseudomonas viridis mutant A2 (Glu L212-->Lys) were studied by EPR spectroscopy and by photoelectric measurements. The EPR signal attributed to the semiquinone-iron (QB-Fe2+) was significantly different from wild type and resembled that found in PS II. Essentially normal oscillations of QB-Fe2+ were observed upon flash illumination. The kinetics of the first and the second electron transfer from QA to QB were characterized by a photoelectric double-flash method. Compared to wild type, the rate of the first electron transfer in the large majority of reaction centers was decreased drastically from k1 = (18 microseconds)-1 in the wild type to (70 ms)-1 in the mutant, whereas the second electron transfer was only slightly slowed down with a rate of k2 = (260 microseconds)-1 compared to (65 microseconds)-1 in wild type (pH 7). When the pH was raised above 10, in a major fraction of the reaction centers a fast kinetics of the first electron transfer, like that in wild type, reappeared. The experimental results are interpreted as an effect of the positive charge on the lysine causing a significant structural change of the QB binding pocket and a strongly diminished affinity for ubiquinone. The slow QA(-)-->QB electron transfer kinetics are thus attributed to ubiquinone binding, which is rate limiting. The possible role of the residue Glu L212, which is conserved in all purple bacteria, in electron and proton transfer to QB is discussed.