Protons bound to the Mn cluster in photosystem II oxygen evolving complex detected by proton matrix ENDOR

Protons in the vicinity of the oxygen-evolving manganese cluster in photosystem II were studied by proton matrix ENDOR. Six pairs of proton ENDOR signals were detected in both the S(0) and S(2) states of the Mn-cluster. Two pairs of signals that show hyperfine constants of 2.3/2.2 and 4.0 MHz, respectively, disappeared after D(2)O incubation in both states. The signals with 2.3/2.2 MHz hyperfine constants in S(0) and S(2) state multiline disappeared after 3 h of D(2)O incubation in the S(0) and S(1) states, respectively. The signal with 4.0 MHz hyperfine constants in S(0) state multiline disappeared after 3 h of D(2)O incubation in the S(0) state, while the similar signal in S(2) state multiline disappeared only after 24 h of D(2)O incubation in the S(1) state. The different proton exchange rates seem to be ascribable to the change in affinities of water molecules to the variation in oxidation state of the Mn cluster during the water oxidation cycle. Based on the point dipole approximation, the distances between the center of electronic spin of the Mn cluster and the exchangeable protons were estimated to be 3.3/3.2 and 2.7 A, respectively. These short distances suggest the protons belong to the water molecules ligated to the manganese cluster. We propose a model for the binding of water to the manganese cluster based on these results.     

EPR and ENDOR studies of the water oxidizing complex of Photosystem II

A comparative study of X-band EPR and ENDOR of the S₂ state of photosystem II membrane fragments and core complexes in the frozen state is presented. The S₂ state was generated either by continuous illumination at T=200 K or by a single turn-over light flash at T=273 K yielding entirely the same S₂ state EPR signals at 10 K. In membrane fragments and core complex preparations both the multiline and the g=4.1 signals were detected with comparable relative intensity. The absence of the 17 and 23 kDa proteins in the core complex preparation has no effect on the appearance of the EPR signals. ¹H-ENDOR experiments performed at two different field positions of the S₂ state multiline signal of core complexes permitted the resolution of four hyperfine (hf) splittings. The hf coupling constants obtained are 4.0, 2.3, 1.1 and 0.6 MHz, in good agreement with results that were previously reported (Tang et al. (1993) J Am Chem Soc 115: 2382–2389). The intensities of all four line pairs belonging to these hf couplings are diminished in D₂O. A novel model is presented and on the basis of the two largest hfc's distances between the manganese ions and the exchangeable protons are deduced. The interpretation of the ENDOR data indicates that these hf couplings might arise from water which is directly ligated to the manganese of the water oxidizing complex in redox state S₂.Abbreviations cw continuous wave - ENDOR electron nuclear double resonance - EPR electron paramagnetic resonance - hf hyperfine - hfc hyperfine coupling - MLS multiline signal - PS II Photosystem II - rf radio frequency - WOC water oxidizing complex     

Highly resolved proton matrix ENDOR of oriented photosystem II membranes in the S2 state

Proton matrix ENDOR was performed to investigate the protons close to the manganese cluster in oriented samples of photosystem II (PS II). Eight pairs of ENDOR signals were detected in oriented PS II membranes. At an angle of θ = 0° between the membrane normal vector n and the external field H₀, five pairs of ENDOR signals were exchangeable in D₂O medium and three pairs were not exchangeable in D₂O medium. The hyperfine splitting of 3.60 MHz at θ = 0° increased to 3.80 MHz at θ = 90°. The non-exchangeable signals with 1.73 MHz hyperfine splitting at θ = 0°, which were assigned to a proton in an amino acid residue, were not detected at θ = 90° in oriented PS II or in non-oriented PS II. Highly resolved spectra show that only limited numbers of protons were detected by CW-ENDOR spectra, although many protons were located near the CaMn₄O₅ cluster. The detected exchangeable protons were proposed to arise from the protons belonging to the water molecules, labeled W1-W4 in the 1.9 Å crystal structure, directly ligated to the CaMn₄O₅ cluster, and nearby amino-acid residue.     

Enhancement of YD spin relaxation by the CaMn4 cluster in photosystem II detected at room temperature: A new probe for the S-cycle

The long-lived, light-induced radical Y_D^• of the Tyr161 residue in the D2 protein of Photosystem II (PSII) is known to magnetically interact with the CaMn₄ cluster, situated ∼ 30 Å away. In this study we report a transient step-change increase in Y_D^• EPR intensity upon the application of a single laser flash to S₁ state-synchronised PSII-enriched membranes from spinach. This transient effect was observed at room temperature and high applied microwave power (100 mW) in samples containing PpBQ, as well as those containing DCMU. The subsequent decay lifetimes were found to differ depending on the additive used. We propose that this flash-induced signal increase was caused by enhanced spin relaxation of Y_D^• by the OEC in the S₂ state, as a consequence of the single laser flash turnover. The post-flash decay reflected S₂ → S₁ back-turnover, as confirmed by their correlations with independent measurements of S₂ multiline EPR signal and flash-induced variable fluorescence decay kinetics under corresponding experimental conditions. This flash-induced effect opens up the possibility to study the kinetic behaviour of S-state transitions at room temperature using Y_D^• as a probe.     

Conversion of the g = 4.1 EPR signal to the multiline conformation during the S2 to S3 transition of the oxygen evolving complex of Photosystem II

The oxygen evolving complex of Photosystem II undergoes four light-induced oxidation transitions, S₀-S₁,…,S₃-(S₄)S₀ during its catalytic cycle. The oxidizing equivalents are stored at a (Mn)₄Ca cluster, the site of water oxidation. EPR spectroscopy has yielded valuable information on the S states. S₂ shows a notable heterogeneity with two spectral forms; a g = 2 (S = 1/2) multiline, and a g = 4.1 (S = 5/2) signal. These oscillate in parallel during the period-four cycle. Cyanobacteria show only the multiline signal, but upon advancement to S₃ they exhibit the same characteristic g = 10 (S = 3) absorption with plant preparations, implying that this latter signal results from the multiline configuration. The fate of the g = 4.1 conformation during advancement to S₃ is accordingly unknown. We searched for light-induced transient changes in the EPR spectra at temperatures below and above the half-inhibition temperature for the S₂ to S₃ transition (ca 230 K). We observed that, above about 220 K the g = 4.1 signal converts to a multiline form prior to advancement to S₃. We cannot exclude that the conversion results from visible-light excitation of the Mn cluster itself. The fact however, that the conversion coincides with the onset of the S₂ to S₃ transition, suggests that it is triggered by the charge-separation process, possibly the oxidation of tyr Z and the accompanying proton relocations. It therefore appears that a configuration of (Mn)₄Ca with a low-spin ground state advances to S₃.     

Direct quantification of the four individual S states in Photosystem II using EPR spectroscopy

EPR spectroscopy is very useful in studies of the oxygen evolving cycle in Photosystem II and EPR signals from the CaMn₄ cluster are known in all S states except S₄. Many signals are insufficiently understood and the S₀, S₁, and S₃ states have not yet been quantifiable through their EPR signals. Recently, split EPR signals, induced by illumination at liquid helium temperatures, have been reported in the S₀, S₁, and S₃ states. These split signals provide new spectral probes to the S state chemistry. We have studied the flash power dependence of the S state turnover in Photosystem II membranes by monitoring the split S₀, split S₁, split S₃ and S₂ state multiline EPR signals. We demonstrate that quantification of the S₁, S₃ and S₀ states, using the split EPR signals, is indeed possible in samples with mixed S state composition. The amplitudes of all three split EPR signals are linearly correlated to the concentration of the respective S state. We also show that the S₁ → S₂ transition proceeds without misses following a saturating flash at 1 °C, whilst substantial misses occur in the S₂ → S₃ transition following the second flash.     

Spectroscopic properties of the peridinins involved in chlorophyll triplet quenching in high-salt peridinin-chlorophyll a-protein from Amphidinium carterae as revealed by optically detected magnetic resonance, pulse EPR and pulse ENDOR spectroscopies

The photoexcited triplet state of the carotenoid peridinin in the high-salt peridinin-chlorophyll a-protein (HSPCP) of the dinoflagellate Amphidinium carterae was investigated by ODMR (optically detected magnetic resonance), pulse EPR and pulse ENDOR spectroscopies. The properties of peridinins associated to the triplet state formation in HSPCP were compared to those of peridinins involved in triplet state population in the main-form peridinin-chlorophyll protein (MFPCP), previously reported. In HSPCP no signals due to the presence of chlorophyll triplet state have been detected, during either steady-state illumination or laser-pulse excitation, meaning that peridinins play the photo-protective role with 100% efficiency as in MFPCP. The general spectroscopic features of the peridinin triplet state are very similar in the two complexes and allow drawing the conclusion that the triplet formation pathway and the triplet localization in one specific peridinin in each subcluster are the same in HSPCP and MFPCP. However some significant differences also emerged from the analysis of the spectra. Zero field splitting parameters of the peridinin triplet states are slightly smaller in HSPCP and small changes are also observed for the hyperfine splittings measured by pulse ENDOR and assigned to the β-protons belonging to one of the two methyl groups present in the conjugated chain, (a_iso = 10.3 MHz in HSPCP vs a_iso = 10.6 MHz in MFPCP). The differences are explained in terms of local distortion of the tails of the conjugated chains of the peridinin molecules, in agreement with the conformational data resulting from the X-ray structures of the two complexes.     

EPR properties of a g=2 broad signal trapped in an S1 state in Ca-depleted Photosystem II

We investigated a new EPR signal that gives a broad line shape around g=2 in Ca²⁺-depleted Photosystem (PS) II. The signal was trapped by illumination at 243 K in parallel with the formation of Y_Z. The ratio of the intensities between the g=2 broad signal and the Y_Z signal was 1:3, assuming a Gaussian line shape for the former. The g=2 broad signal and the Y_Z signal decayed together in parallel with the appearance of the S₂ state multiline at 243 K. The g=2 broad signal was assigned to be an intermediate S₁X state in the transition from the S₁ to the S₂ state, where X represents an amino acid radical nearby manganese cluster, such as D1-His337. The signal is in thermal equilibrium with Y_Z. Possible reactions in the S state transitions in Ca²⁺-depleted PS II were discussed.     

Determination of the proton environment of high stability Menasemiquinone intermediate in Escherichia coli nitrate reductase A by pulsed EPR

Escherichia coli nitrate reductase A (NarGHI) is a membrane-bound enzyme that couples quinol oxidation at a periplasmically oriented Q-site (Q_D) to proton release into the periplasm during anaerobic respiration. To elucidate the molecular mechanism underlying such a coupling, endogenous menasemiquinone-8 intermediates stabilized at the Q_D site (MSQ_D) of NarGHI have been studied by high-resolution pulsed EPR methods in combination with ¹H₂O/²H₂O exchange experiments. One of the two non-exchangeable proton hyperfine couplings resolved in hyperfine sublevel correlation (HYSCORE) spectra of the radical displays characteristics typical from quinone methyl protons. However, its unusually small isotropic value reflects a singularly low spin density on the quinone carbon α carrying the methyl group, which is ascribed to a strong asymmetry of the MSQ_D binding mode and consistent with single-sided hydrogen bonding to the quinone oxygen O1. Furthermore, a single exchangeable proton hyperfine coupling is resolved, both by comparing the HYSCORE spectra of the radical in ¹H₂O and ²H₂O samples and by selective detection of the exchanged deuterons using Q-band ²H Mims electron nuclear double resonance (ENDOR) spectroscopy. Spectral analysis reveals its peculiar characteristics, i.e. a large anisotropic hyperfine coupling together with an almost zero isotropic contribution. It is assigned to a proton involved in a short ∼1.6 Å in-plane hydrogen bond between the quinone O1 oxygen and the Nδ of the His-66 residue, an axial ligand of the distal heme b_D. Structural and mechanistic implications of these results for the electron-coupled proton translocation mechanism at the Q_D site are discussed, in light of the unusually high thermodynamic stability of MSQ_D.     

Pulse EPR, 55Mn-ENDOR and ELDOR-detected NMR of the S2-state of the oxygen evolving complex in Photosystem II

Pulse EPR, ⁵⁵Mn-ENDOR and ELDOR-detected NMR experiments were performed on the S₂-state of the oxygen-evolving complex from spinach Photosystem II. The novel technique of random acquisition in ENDOR was used to suppress heating artefacts. Our data unambiguously shows that four Mn ions have significant hyperfine coupling constants. Numerical simulation of the ⁵⁵Mn-ENDOR spectrum allowed the determination of the principal values of the hyperfine interaction tensors for all four Mn ions of the oxygen-evolving complex. The results of our ⁵⁵Mn-ENDOR experiments are in good agreement with previously published data [Peloquin JM et al. (2000) J Am Chem Soc 122: 10926–10942]. For the first time ELDOR-detected NMR was applied to the S₂-state and revealed a broad peak that can be simulated numerically with the same parameters that were used for the simulation of the ⁵⁵Mn-ENDOR spectrum. This provides strong independent support for the assigned hyperfine parameters.     

Assignment of Proton Endor Resonances of Nitroxyl Spin-Labels in Frozen Solution

Spin-label nitroxyl derivatives of tetramethylpyrroline and tetramethylpyrrolidine in frozen solutions of perdeuterated methanol have been characterized by electron nucleus double resonance (ENDOR spec-troscopy). With use of selectively deuterated derivatives of 2,2,5,5-tetramethylpyrroline-l-oxyl-3-carboxamide, proton ENDOR resonance features have been assigned to the vinylic proton in the five membered pyrrolinyl ring and to the methyl groups. The ENDOR resonance features were analyzed on the basis of their dependence on H₀. Two pairs of resonance features were assigned to the vinylic proton and were shown to correspond to ‖ and ⊥ hyperfine coupling (hfc) components. Six pairs of resonance features were ascribed to the methyl groups. The proton ENDOR spectra of the 3-carboxylic acid spin-label derivatives of tetramethylpyrroline and of tetramethylpyrrolidine compounds exhibited comparable features with nearly identical line splittings. From the observed ENDOR splittings, we have estimated the isotropic hfc component of the vinylic proton in 2,2,5,5-tetramethylpyrroline-l-oxyl-3-carboxamide to be -1.81 ± 0.04 MHz in frozen methanol. On the basis of the anisotropic dipolar hfc components, the electron-to-vinylic proton distance is estimated as 3.78 ± 0.01 Å. in excellent agreement with that of 3.79 Å calculated from X-ray defined coordinates.     

The two forms of the S2 state multiline signal in Photosystem II: effect of methanol and ethanol

The characteristic Mn hyperfine ‘multiline’ signal exhibited in the S₂ state of the oxygen-evolving complex (OEC) complex of Photosystem II (PSII) has been shown to be heterogeneous in character. In this study, we have explored the effects that influence the proportions of the two forms of the S₂ state multiline signal present in any sample. The narrow form of the signal is lost upon storage (weeks) at 77 K, whereas the broad form remains. In particular, we explore the roles of ethanol and methanol as well as effects of the second turnover of the enzyme on storage of the sample at 77 K. We find that in samples containing methanol, the narrow form may predominate upon the first flash, but the broad form predominates on the fifth flash and also in samples containing ethanol.     

Influence of protein phosphorylation on the electron-transport properties of Photosystem II

Many of the core proteins in Photosystem II (PS II) undergo reversible phosphorylation. It is known that protein phosphorylation controls the repair cycle of Photosystem II. However, it is not known how protein phosphorylation affects the partial electron transport reactions in PS II. Here we have applied variable fluorescence measurements and EPR spectroscopy to probe the status of the quinone acceptors, the Mn cluster and other electron transfer components in PS II with controlled levels of protein phosphorylation. Protein phosphorylation was induced in vivo by varying illumination regimes. The phosphorylation level of the D1 protein varied from 10 to 58% in PS II membranes isolated from pre-illuminated spinach leaves. The oxygen evolution and Q_A ⁻ to Q_B(Q_B ⁻) electron transfer measured by flash-induced fluorescence decay remained similar in all samples studied. Similar measurements in the presence of DCMU, which reports on the status of the donor side in PS II, also indicated that the integrity of the oxygen-evolving complex was preserved in PS II with different levels of D1 protein phosphorylation. With EPR spectroscopy we examined individual redox cofactors in PS II. Both the maximal amplitude of the charge separation reaction (measured as photo-accumulated pheophytin⁻) and the EPR signal from the Q_A ⁻ Fe²⁺ complex were unaffected by the phosphorylation of the D1 protein, indicating that the acceptor side of PS II was not modified. Also the shape of the S₂ state multiline signal was similar, suggesting that the structure of the Mn-cluster in Photosystem II did not change. However, the amplitude of the S₂ multiline signal was reduced by 35% in PS II, where 58% of the D1 protein was phosphorylated, as compared to the S₂ multiline in PS II, where only 10% of the D1 protein was phosphorylated. In addition, the fraction of low potential Cyt b ₅₅₉ was twice as high in phosphorylated PS II. Implications from these findings, were precise quantification of D1 protein phosphorylation is, for the first time, combined with high-resolution biophysical measurements, are discussed. This revised version was published online in June 2006 with corrections to the Cover Date.     

Orientation-selected ENDOR of the active center in Chromatium vinosum [NiFe] hydrogenase in the oxidized "ready" state

 Electron nuclear double resonance (ENDOR) was applied to study the active site of the oxidized "ready" state, Ni_r, in the [NiFe] hydrogenase of Chromatium vinosum. The magnetic field dependence of the EPR was used to select specific subsets of molecules contributing to the ENDOR response by stepping through the EPR envelope. Three hyperfine couplings could be clearly followed over the complete field range. Two protons, H1 and H2, display a very similar large isotropic coupling of 12.5 and 12.6 MHz, respectively. Their dipolar coupling is small (2.1 and 1.4 MHz, respectively). A third proton, H3, exhibits a small isotropic coupling of 0.5 MHz and a larger anisotropic contribution of 3.5 MHz. Based on a comparison with structural data obtained from X-ray crystallography of single crystals of hydrogenases from Desulfovibrio gigas and D. vulgaris and the known g-tensor orientation of Ni_r, an assignment of the ¹H hyperfine couplings could be achieved. H1 and H2 were assigned to the β-CH₂ protons of the bridging cysteine Cys533 and H3 could belong to a β-CH₂ proton of Cys68 or to a protonated cysteine (-SH) of Cys68 or Cys530. Received: 26 November 1998 / Accepted: 1 April 1999     

Pulse ENDOR and density functional theory on the peridinin triplet state involved in the photo-protective mechanism in the peridinin-chlorophyll a-protein from Amphidinium carterae

The photoexcited triplet state of the carotenoid peridinin in the Peridinin-chlorophyll a-protein of the dinoflagellate Amphidinium carterae has been investigated by pulse EPR and pulse ENDOR spectroscopies at variable temperatures. This is the first time that the ENDOR spectra of a carotenoid triplet in a naturally occurring light-harvesting complex, populated by energy transfer from the chlorophyll a triplet state, have been reported. From the electron spin echo experiments we have obtained the information on the electron spin polarization dynamics and from Mims ENDOR experiments we have derived the triplet state hyperfine couplings of the α- and β-protons of the peridinin conjugated chain. Assignments of β-protons belonging to two different methyl groups, with a_iso = 7.0 MHz and a_iso = 10.6 MHz respectively, have been made by comparison with the values predicted from density functional theory. Calculations provide a complete picture of the triplet spin density on the peridinin molecule, showing that the triplet spins are delocalized over the whole π-conjugated system with an alternate pattern, which is lost in the central region of the polyene chain. The ENDOR investigation strongly supports the hypothesis of localization of the triplet state on one peridinin in each subcluster of the PCP complex, as proposed in [Di Valentin et al. Biochim. Biophys. Acta 1777 (2008) 186-195]. High spin density has been found specifically at the carbon atom at position 12 (see Fig. 1B), which for the peridinin involved in the photo-protective mechanism is in close contact with the water ligand to the chlorophyll a pigment. We suggest that this ligated water molecule, placed at the interface between the chlorophyll-peridinin pair, is functioning as a bridge in the triplet-triplet energy transfer between the two pigments.     

The origin of split EPR signals in the Ca2+-depleted Photosystem II

A light-driven reaction model for the Ca²⁺-depleted Photosystem (PS) II is proposed to explain the split signal observed in electron paramagnetic resonance (EPR) spectra based on a comparison of EPR assignments with recent x-ray structural data. The split signal has a splitting linewidth of 160 G at around g = 2 and is seen upon illumination of the Ca²⁺-depleted PS II in the S₂ state associated with complete or partial disappearance of the S₂ state multiline signal. Another g=2 broad ESR signal with a 110 G linewidth was produced by 245 K illumination for a short period in the Ca²⁺-depleted PS II in S₁ state. At the same time a normal Y_Z^· radical signal was also efficiently trapped. The g=2 broad signal is attributed to an intermediate S₁X^· state in equilibrium with the trapped Y_Z^· radical. Comparison with x-ray structural data suggests that one of the split signals (doublet signal) is attributable to interaction between His 190 and the Y_Z^· radical, and other signals is attributable to interaction between His 337 and the manganese cluster, providing further clues as to the mechanism of water oxidation in photosynthetic oxygen evolution.     

Electron transfer in the water-oxidizing complex of Photosystem II

An overview is presented of secondary electron transfer at the electron donor side of Photosystem II, at which ultimately two water molecules are oxidized to molecular oxygen, and the central role of manganese in catalyzing this process is discussed. A powerful technique for the analysis of manganese redox changes in the water-oxidizing mechanism is the measurement of ultraviolet absorbance changes, induced by single-turnover light flashes on dark-adapted PS II preparations. Various interpretations of these ultraviolet absorbance changes have been proposed. Here it is shown that these changes are due to a single spectral component, which presumably is caused by the oxidation of Mn(III) to Mn(IV), and which oscillates with a sequence +1, +1, +1, –3 during the so-called S₀ S₁ S₂ S₃ S₀ redox transitions of the oxygen-evolving complex. This interpretation seems to be consistent with the results obtained with other techniques, such as those on the multiline EPR signal, the intervalence Mn(III)-Mn(IV) transition in the infrared, and EXAFS studies. The dark distribution of the S states and its modification by high pH and by the addition of low concentrations of certain water analogues are discussed. Finally, the patterns of proton release and of electrochromic absorbance changes, possibly reflecting the change of charge in the oxygen-evolving system, are discussed. It is concluded that nonstoichiometric patterns must be considered, and that the net electrical charge of the system probably is the highest in state S₂ and the lowest in state S₁.     

Comparative EPR and thermoluminescence study of anoxic photoinhibition in Photosystem II particles

Photosystem II particles were exposed to 800 W m^–2 white light at 20 °C under anoxic conditions. The F_o level of fluorescence was considerably enhanced indicating formation of stable-reduced forms of the primary quinone electron acceptor, Q_A. The F_m level of fluorescence declined only a little. The g=1.9 and g=1.82 EPR forms characteristic of the bicarbonate-bound and bicarbonate-depleted semiquinone-iron complex, Q_A ^–Fe²⁺, respectively, exhibited differential sensitivity against photoinhibition. The large g=1.9 signal was rapidly diminished but the small g=1.82 signal decreased more slowly. The S₂-state multiline signal, the oxygen evolution and photooxidation of the high potential form of cytochrome b-559 were inhibited approximately with the same kinetics as the g=1.9 signal. The low potential form of oxidized cytochrome b-559 and Signal II_slow arising from Tyr_D ⁺ decreased considerably slower than the g=1.9 semiquinone-iron signal. The high potential form of oxidized cytochrome b-559 was diminished faster than the low potential form. Photoinhibition of the g=1.9 and g=1.82 forms of Q_A was accompanied with the appearance and gradual saturation of the spin-polarized triplet signal of P 680. The amplitude of the radical signal from photoreducible pheophytin remained constant during the 3 hour illumination period. In the thermoluminescence glow curves of particles the Q band (S₂Q_A ^– charge recombination) was almost completely abolished. To the contrary, the C band (Tyr_D ⁺Q_A ^– charge recombination) increased a little upon illumination. The EPR and thermoluminescence observations suggest that the Photosystem II reaction centers can be classified into two groups with different susceptibility against photoinhibition.Abbreviations C band thermoluminescence band associated with Tyr-D⁺Q _a ^– charge recombination - Chl chlorophyll - DCMU 3-(3,4-dichlorophenyl)-1,1-dimethylurea - EPR electron paramagnetic resonance - F_o initial fluorescence - F_m maximum fluorescence - Q band thermoluminescence band originating from S₂Q _a -charge recombination - Q _a the primary quinone electron acceptor of PS II - P 680 the primary electron donor chlorophyll of PS II - S₂ oxidation state of the water-splitting system - Phe pheophytin - TL thermoluminescence - Tyr _d redox active tyrosine-160 of the D₂ protein     

Spin-probes designed for measuring the intrathylakoid pH in chloroplasts

Nitroxide radicals are widely used as molecular probes in different fields of chemistry and biology. In this work, we describe pH-sensitive imidazoline- and imidazolidine-based nitroxides with pK values in the range 4.7-7.6 (2,2,3,4,5,5-hexamethylperhydroimidazol-1-oxyl, 4-amino-2,2,5,5-tetramethyl-2,5-dihydro-1H-imidazol-1-oxyl, 4-dimethylamino-2,2-diethyl-5,5-dimethyl-2,5-dihydro-1H-imidazol-1-oxyl, and 2,2-diethyl-5,5-dimethyl-4-pyrrolidyline-1-yl-2,5-dihydro-1H-imidazol-1-oxyl), which allow the pH-monitoring inside chloroplasts. We have demonstrated that EPR spectra of these spin-probes localized in the thylakoid lumen markedly change with the light-induced acidification of the thylakoid lumen in chloroplasts. Comparing EPR spectrum parameters of intrathylakoid spin-probes with relevant calibrating curves, we could estimate steady-state values of lumen pH_in established during illumination of chloroplasts with continuous light. For isolated bean (Vicia faba) chloroplasts suspended in a medium with pH_out = 7.8, we found that pH_in ≈ 5.4-5.7 in the state of photosynthetic control, and pH_in ≈ 5.7-6.0 under photophosphorylation conditions. Thus, ATP synthesis occurs at a moderate acidification of the thylakoid lumen, corresponding to transthylakoid pH difference ΔpH ≈ 1.8-2.1. These values of ΔpH are consistent with a point of view that under steady-state conditions the proton gradient ΔpH is the main contributor to the proton motive force driving the operation of ATP synthesis, provided that stoichiometric ratio H⁺/ATP is n ≥ 4-4.7.     

The reduced S<Subscript>−1</Subscript> and S<Subscript>−2</Subscript> oxidation states of the O<Superscript>2</Superscript>-evolving complex of photosystem II: An EPR microwave power saturation study

Progressive microwave power saturation (P_1/2) measurements have been performed on the tyrosine D radical (Y_D ^•) of photosystem II (PSII) in order to examine its relaxation enhancement by the oxygen-evolving complex (OEC) poised to the reduced S₋₁ and S₋₂ oxidation states by NO treatment. Analysis of the power saturation curves showed that the S₋₁ oxidation state of the OEC does not enhance the relaxation of Y_D ^•: it therefore possesses a diamagnetic ground state. In contrast, the Mn(II)-Mn(III) multiline electron paramagnetic resonance (EPR) signal characteristic of the S₋₂ oxidation state of the OEC was shown to provide a relaxation enhancement pathway for Y_D ^•, however less efficient relative to the one provided by the S₂-state multiline EPR signal. We also examined the Y_D ^• relaxation enhancement characteristics of the EPR-silent oxidation state produced after brief (1–5 min) dark incubation at 0°C of a PSII sample poised to the EPRactive S₋₂ state. This EPR-silent oxidation state denoted as “0°C incubation” state was shown to possess remarkably similar P_1/2 values with the EPR-active S₋₂ state in the overall examined temperature range (6–20 K). In addition, these values remained unchanged after successive cycles of the OEC between the EPR-active S₋₂ state and the “0°C incubation” state. The data presented in this work point to the conclusion that the “0°C incubation” state is indeed an S₋₂ oxidation state with half-integer spin.