The PsbZ subunit of Photosystem II in Synechocystis sp. PCC 6803 modulates electron flow through the photosynthetic electron transfer chain.

The psbZ gene of Synechocystis sp. PCC 6803 encodes the approximately 6.6 kDa photosystem II (PSII) subunit. We here report biophysical, biochemical and in vivo characterization of Synechocystis sp. PCC 6803 mutants lacking psbZ. We show that these mutants are able to perform wild-type levels of light-harvesting, energy transfer, PSII oxygen evolution, state transitions and non-photochemical quenching (NPQ) under standard growth conditions. The mutants grow photoautotrophically; however, their growth rate is clearly retarded under low-light conditions and they are not capable of photomixotrophic growth. Further differences exist in the electron transfer properties between the mutants and wild type. In the absence of PsbZ, electron flow potentially increased through photosystem I (PSI) without a change in the maximum electron transfer capacity of PSII. Further, rereduction of P700(+) is much faster, suggesting faster cyclic electron flow around PSI. This implies a role for PsbZ in the regulation of electron transfer, with implication for photoprotection.

ESEEM studies of substrate water and small alcohol binding to the oxygen-evolving complex of photosystem II during functional turnover.

We report the first examination of exchangeable proton and MeOH interactions with the Mn catalytic cluster in photosystem II, under functional flash turnover conditions, using 2H ESEEM spectroscopy on the S2 and S0 multiline states. Deuterium-labeled water (D2O) and methyl d3-labeled methanol (DMeOH) are employed. It was discovered that a hyperfine resolved multiline S0 signal could be seen in the presence of D2O, the hyperfine structure of which depended on the presence or absence of methanol (MeOH). In the presence of DMeOH, significant dipolar coupling of the three methyl deuterons to the multiline centers in the S2 and S0 states was seen (S2, 0.65, 0.39(2) MHz; and S0, 0.60, 0.37(2) MHz). These are consistent with direct binding of the methoxy fragment to Mn. Assuming terminal Mn-OMe ligation, the couplings indicated a spin projection coefficient (rho) magnitude of approximately 2 for the ligating Mn in both the S2 and S0 states, with inferred Mn-O distances of approximately 1.9-2.0 A. In the presence of D2O, four classes of exchangeable deuterons were identified by ESEEM in S2 and S0. Three of these classes (1, 2, and 4) exhibited populations and coupling strengths that were essentially constant under various conditions of sample preparation, illumination turnover, and small alcohol addition. Class 3 could be modeled with constant coupling but a highly variable deuteron population (n3 approximately 0-10) depending in part on the preparation used. For all classes, the coupling parameters were very similar in S2 and S0. The favored interpretation is that the two strongest coupling classes (1 and 2) represent close binding of one water molecule to a single Mn which has an oxidation state of II in S0 and III in S2, and rho approximately 2 in both cases. This water is not displaced by MeOH, but either the water or MeOH is singly deprotonated upon MeOH binding. Class 4 represents approximately 2 water molecules which are not closely bound to Mn (Mn-deuteron distances of approximately 3.7-4.7 A). Class 3 probably represents protein matrix protons within approximately 4 A of the Mn in the cluster, which can be variably exchanged in different preparations.

Ammonia displaces methanol bound to the water oxidizing complex of photosystem II in the S2 state.

Ammonia and methanol both bind to the water oxidising complex of photosystem II during its turnover, possibly at sites where water binds during the normal water oxidation process. We have investigated the interaction between these two water analogues at the S2 state of the water oxidising cycle using electron magnetic resonance techniques. We find evidence that ammonia displaces methanol from its binding site.

Structure of biological solar energy converters - further revelations.

Photosynthetic organisms harvest solar energy by absorbing light and ultimately transferring energy through a cascade of chemical reactions to power all cellular processes. Core components initiating this reaction cascade are the photosynthetic reaction centres Photosystem I and Photosystem II. Two recent publications on the structure of the reaction centres by Adam Ben-Shem et al. and Kristina Ferreira et al. represent a big step towards understanding the evolutionary development of the core energy conversion process and identifying the site of the water oxidation process, the source of atmospheric oxygen.

Photosynthetic water oxidation: the role of tyrosine radicals.

This mini-review outlines the involvement of the tyrosine electron carriers, Y(D) and Y(Z), in the mechanism of electron transfer from water to P680. We discuss our data and put forward our ideas on the role of Y(D) and Y(Z).

Molecular analysis of the Chlamydomonas nuclear gene encoding PsbW and demonstration that PsbW is a subunit of photosystem II, but not photosystem I.

PsbW is a nuclear-encoded protein located in the thylakoid membrane of the chloroplast. Studies in higher plants have provided substantial evidence that PsbW is a core component of photosystem II. However, recent data have been presented to suggest that PsbW is also a subunit of photosystem I. Such a sharing of subunits between the two photosystems would represent a novel phenomenon. To investigate this, we have cloned and characterized the psbW gene from the green alga Chlamydomonas reinhardtii. The gene is split by five introns and encodes a polypeptide of 115 residues comprising the 6.1 kDa mature PsbW protein preceded by a 59 amino acid bipartite transit sequence. Using antibodies raised to PsbW we have examined: (1) C. reinhardtii mutants lacking either photosystem and (2) purified photosystem preparations. We find that PsbW is a subunit of photosystem II, but not photosystem I.

Effect of hydroxylamine on photosystem II: reinvestigation of electron paramagnetic resonance characteristics reveals possible S state intermediates.

Previous work in many laboratories has established that hydroxylamine reduces the S(1) state of the water oxidizing complex (WOC) in one-electron steps. Significant levels of what can now be defined as the S(-1)* state are achieved by specific (concentration and incubation length) hydroxylamine treatments. This state has already been studied by electron paramagnetic resonance spectrometry (EPR), and unusual EPR signals were noted (for example, see Sivaraja, M., and Dismukes, G. C. (1988) Biochemistry 27, 3467-3475). We have now reinvestigated these initial experiments and confirmed many of the original observations. We then utilized more recent EPR markers for the S(0) and S(1) states to further explore the S(-1)* state. The broad radical "split" type EPR signal, produced by 200 K illumination of samples prepared to give a high yield of the S(-1)* state, is shown to most likely reflect a trapped intermediate state between S(-1)* and S(0)*, since samples where this signal is present can be warmed in the dark to produce S(0)*. The threshold for advancement from S(-1)* to S(0)* is near 200 K, as the yield of broad radical decreases and S(0)* multiline EPR signal increases with length of 200 K illumination. Advancement of S(0)* to S(1) is limited at 200 K, but S(1) can be restored by 273 K illumination. Illumination of these hydroxylamine-treated samples at temperatures below 77 K gives a second broad radical EPR signal. The line shape, decay, and other properties of this new radical signal suggest that it may arise from an interaction in the S(-2)* or lower S states, which are probably present in low yield in these samples. Illumination below 20 K of S(0)* state samples containing methanol, and therefore exhibiting the S(0) multiline signal, gives rise to a third broad radical with distinctive line shape. The characteristics of the three broad radicals are similar to those found from interactions between Y(Z)(*) and other S states. The evidence is presented that they do represent intermediate states in S state turnover. Further work is now needed to identify these radicals.

Intermediates of the S(3) state of the oxygen-evolving complex of photosystem II.

The S(3) state of the water-oxidizing complex (WOC) of photosystem II (PSII) is the last state that can be trapped before oxygen evolution occurs at the transient S(4) state. A number of EPR-detectable intermediates are associated with this critical state. The preceding paper examined mainly the decay of S(3) at cryogenic temperatures leading to the formation of a proton-deficient configuration of S(2) termed S(2)'. This second paper examines all intermediates formed by the near-IR light (NIR) excitation of the S(3) state and compares these with the light-excitation products of the S(2)' state. The rather complex set of observations is organized in a comprehensive flowchart, the central part of which is the S(3)...Q(A)(-) state. This state can be converted to various intermediates via two main pathways: (A) Excitation of S(3) by NIR light at temperatures below 77 K results presumably in the formation of an excited S(3) state, S(3), which decays via either of two pathways. Slowly at liquid helium temperatures but much faster at 77 K, S(3) decays to an EPR-silent state, denoted S(3)' ', which by raising the temperature to ca. 190 K converts to a spin configuration of the Mn cluster, characterized by g = 21, 3.7 in perpendicular and g = 23 in parallel mode EPR, denoted S(3)'. Upon further warming to 220 K, S(3)' relaxes to the untreated S(3) state. Below about 77 K and more favorably at liquid helium temperatures, an alternative pathway of S(3) decay via the metallo-radical intermediate S(2)'Z*...Q(A)(-) can be traced. This leads to the metastable state S(2)'Z...Q(A) via charge recombination. S(2)'Z* is characterized by a split-radical signal at g = 2, while all S(2)' transients are characterized by the same g = 5/2.9 (S = (7)/(2)) configuration of the Mn cluster with small modifications, reflecting an influence of the tyr Z oxidation state on the crystal-field symmetry at the Mn cluster. (B) S(2)'...Q(A) can be reached alternatively by the slow charge recombination of S(3) and Q(A)(-) at 77 K. White-light illumination of S(2)'.Q(A) below about 20 K results in charge separation, reforming the intermediate S(2)'Z*...Q(A)(-). Thermally activated branches to the main pathways are also described, e.g., at elevated temperatures tyr Z* reoxidizes S(2)' to the S(3) state. The above observations are discussed in terms of a molecular model of the S(3) state of the OEC. Main aspects of the model are the following. Intermediates, isoelectronic to S(3), are attributed to the NIR-induced translocation of the positive hole to different Mn ligands, or to tyr Z. On the basis of a comparison of the electron-donating efficiency of tyr Z and tyr D at cryogenic temperatures, it is inferred that the Mn cluster acts as the main proton acceptor from tyr Z. Water associated with the Mn cluster is assumed to be in hydrogen-bonding equilibrium with tyr Z, and an array comprising this water and adjacent water (or OH or O) ligands to Mn followed by a sequence of proton acceptors is proposed to act as an efficient proton translocation pathway. Oxidation of the tyrosine by P(680)(+) repels protons to and out from the Mn cluster. This proposed role of tyr Z in the water-splitting process is described as a proton repeller/electron abstractor.

Electron transfer from the water oxidizing complex at cryogenic temperatures: the S1 to S2 step.

We report the detection of a "split" electron paramagnetic resonance (EPR) signal during illumination of dark-adapted (S(1) state) oxygen-evolving photosystem II (PSII) membranes at <20 K. The characteristics of this signal indicate that it arises from an interaction between an organic radical and the Mn cluster of PSII. The broad radical signal decays in the dark following illumination either by back-reaction with Qa*- or by forward electron transfer from the Mn cluster. The forward electron transfer (either from illumination at 11 K followed by incubation in the dark at 77 K or by illumination at 77 K) results in the formation of a multiline signal similar to, but distinct from, other well-characterized multiline forms found in the S0 and S2 states. The relative yield of the "S1 split signal", which we provisionally assign to S1X*, where X could be YZ* or Car*+, and that of the 77 K multiline signal indicate a relationship between the two states. An approximate quantitation of the yield of these signals indicates that up to 40-50% of PSII centers can form the S1 split signal. Ethanol addition removes the ability to observe the S1 split signal, but the multiline signal is still formed at 77 K. The multiline forms with <700 nm light and is not affected by near-infrared (IR) light, showing that we are detecting electron transfer in centers not responsive to IR illumination. The results provide important new information about the mechanism of electron abstraction from the water oxidizing complex (WOC).