The heart of oxygenic photosynthesis is photosystem II (PSII), a multisubunit protein complex that uses solar energy to drive the splitting of water and production of molecular oxygen. The effectiveness of the photochemical reaction center of PSII depends on the efficient transfer of excitation energy from the surrounding antenna chlorophylls. A kinetic model for PSII, based on the x-ray crystal structure coordinates of 37 antenna and reaction center pigment molecules, allows us to map the major energy transfer routes from the antenna chlorophylls to the reaction center chromophores. The model shows that energy transfer to the reaction center is slow compared with the rate of primary electron transport and depends on a few bridging chlorophyll molecules. This unexpected energetic isolation of the reaction center in PSII is similar to that found in the bacterial photosystem, conflicts with the established view of the photophysics of PSII, and may be a functional requirement for primary photochemistry in photosynthesis. In addition, the model predicts a value for the intrinsic photochemical rate constant that is 4 times that found in bacterial reaction centers.A s the site of water splitting and oxygen production, photosystem II (PSII) is essential for oxygenic photosynthesis. This multisubunit protein complex consists of at least 17 polypeptides and catalyzes the oxidation of water and the reduction of plastoquinone (1). The PSII holocomplex of higher plants and green algae contains 200-300 chlorophyll (Chl) molecules and various carotenoids that are noncovalently bound to a variety of PSII polypeptides (2). The minimal functionally active PSII complex contains the reaction center (RC) polypeptides (D1, D2, cytochrome b 559 ), the Chla core antenna polypeptides (CP43 and CP47), and the polypeptides of the oxygen-evolving complex. The total number of Chls in this PSII core complex is less than 40 per RC (3). Light energy absorbed by any PSII Chl generates an excited state, which is ultimately transferred to the primary electron donor in photosystem II, the RC photoactive pigment P680. Within the excited-state lifetime, primary charge separation [formation of P680 ϩ and pheophytin Ϫ (Pheo Ϫ )] and charge stabilization (reduction of the primary quinone electron acceptor, Q A , by Pheo Ϫ ) occur with greater than 90% efficiency.The kinetics of excited-state decay in PSII are highly dependent on the redox state of the RC (4). Accordingly, these kinetics contain valuable information about rates and mechanisms of excited-state energy transfer, primary charge separation, and stabilization reactions in the RC complex. Unfortunately, it is very difficult to measure directly these rates by using timeresolved spectroscopic techniques because of the complications of excited-state transfer processes that precede the electron transfer steps. In addition, transient absorption measurements in the Q y band of Chl are complicated by spectral congestion and also by competing absorption, bleaching, and stimulated emission. Although t...

The protein composition, steady state and time-resolved fluorescence emission spectra were studied in solubilized and aggregated LHCII complexes, that were prepared according to two different isolation protocols: (1) by fractionation of cation-depleted thylakoid membranes using the non-ionic detergent Triton X-100 according to the procedure of Burke et al. [(1978) Arch. Biochem. Biophys. 187, 252-263] or (2) by solubilization with N-beta-dodecyl maltoside (beta-DM) of photosystem II (PSII) membrane fragments in the presence of cations [Irrgang et al. (1988) Eur. J. Biochem. 178, 207-217]. Based on the analysis of the decay-associated emission spectra measured at 10 and 80 K five long-wavelength chlorophyll species were identified in aggregated LHCII complexes. These five forms are characterized by emission maxima at 681.5, 683, 687, 695, or 702 nm. All of these forms were found in both types of LHCII preparations but the relative amounts and temperature dependency of these species were markedly different in the aggregated LHCII complexes isolated by the two procedures. It was found that these differences cannot be simply explained by effects due to using a less mild detergent as beta-DM or by an ionic influence of Ca2+. Biochemical analysis of the protein composition showed that beta-DM type LHCII consists of all the chlorophyll (Chl)binding proteins belonging to the antenna system of PSII except the CP29 type II gene product (CP29). In contrast, the Triton X-100-solubilized LHCII is highly depleted in CP26 (CP 29 type I gene product) and is contaminated by a variety of unidentified polypeptides. It is proposed that the aggregates of LHCII prepared using Triton X-100 acquire specific spectral and kinetic features due to interaction between the bulk of LHCII subunits and minor protein(s).

The light state transition regulates the distribution of absorbed excitation energy between the two photosystems (PSs) of photosynthesis under varying environmental conditions and/or metabolic demands. In cyanobacteria, there is evidence for the redistribution of energy absorbed by both chlorophyll (Chl) and by phycobilin pigments, and proposed mechanisms differ in the relative involvement of the two pigment types. We assayed changes in the distribution of excitation energy with 77K fluorescence emission spectroscopy determined for excitation of Chl and phycobilin pigments, in both wild-type and state transition-impaired mutant strains of Synechococcus sp. PCC 7002 and Synechocystis sp. PCC 6803. Action spectra for the redistribution of both Chl and phycobilin pigments were very similar in both wild-type cyanobacteria. Both state transitionimpaired mutants showed no redistribution of phycobilin-absorbed excitation energy, but retained changes in Chl-absorbed excitation. Action spectra for the Chl-absorbed changes in excitation in the two mutants were similar to each other and to those observed in the two wild types. Our data show that the redistribution of excitation energy absorbed by Chl is independent of the redistribution of excitation energy absorbed by phycobilin pigments and that both changes are triggered by the same environmental light conditions. We present a model for the state transition in cyanobacteria based on the x-ray structures of PSII, PSI, and allophycocyanin consistent with these results.The effective absorption of sunlight by antenna pigments is the critical first step in photosynthesis. All oxygenic photosynthetic organisms share a common core antenna pigment complement of about 40 chlorophyll (Chl) a in PSII and about 100 Chl a in PSI (Rö gner et al., 1990). Photosynthetic organisms do not, however, limit their photon capturing ability to this level, but rather use some form of additional peripheral antenna pigments to increase the effective "absorption cross section" of one or both PSs. Higher plants and algae have evolved diverse mechanisms to increase their ability to absorb sunlight. In cyanobacteria, the soluble phycobiliproteins are organized into phycobilisomes (PBSs), which are primarily associated excitonically with PSII in a manner analogous to the family of intrinsic thylakoid membrane Chl a/b-containing light-harvesting complex polypeptides (LHCII), which serve the same function in higher plants (Glazer, 1984; Zilinskas and Greenwald, 1986).Both cyanobacteria and higher plants can regulate the efficiency of excitation energy transfer to the two PSs. The light state transition appears designed to adjust the relative activities of PSII and PSI in response to a dynamic environment or to changing metabolic demands (Yu et al., 1993). The mechanism in higher plants involves a reversible association of LHCII with PSII and PSI triggered by the redox state of intersystem electron transport carriers and driven by the reversible phosphorylation of LHCII (for review, see Allen, 1992; Woll...

Lichens, a symbiotic relationship between a fungus (mycobiont) and a photosynthetic green algae or cyanobacteria (photobiont), belong to an elite group of survivalist organisms termed resurrection species. When lichens are desiccated, they are photosynthetically inactive, but upon rehydration they can perform photosynthesis within seconds. Desiccation is correlated with both a loss of variable chlorophyll a fluorescence and a decrease in overall fluorescence yield. The fluorescence quenching likely reflects photoprotection mechanisms that may be based on desiccation-induced changes in lichen structure that limit light exposure to the photobiont (sunshade effect) and/or active quenching of excitation energy absorbed by the photosynthetic apparatus. To separate and quantify these possible mechanisms, we have investigated the origins of fluorescence quenching in desiccated lichens with steady-state, low temperature, and time-resolved chlorophyll fluorescence spectroscopy. We found the most dramatic target of quenching to be photosystem II (PSII), which produces negligible levels of fluorescence in desiccated lichens. We show that fluorescence decay in desiccated lichens was dominated by a short lifetime, long-wavelength component energetically coupled to PSII. Remaining fluorescence was primarily from PSI and although diminished in amplitude, PSI decay kinetics were unaffected by desiccation. The long-wavelength-quenching species was responsible for most (about 80%) of the fluorescence quenching observed in desiccated lichens; the rest of the quenching was attributed to the sunshade effect induced by structural changes in the lichen thallus.

Exposure to blue light has previously been shown to induce the reversible quenching of fluorescence in cyanobacteria, indicative of a photoprotective mechanism responsible for the down regulation of photosynthesis. We have investigated the molecular mechanism behind fluorescence quenching by characterizing changes in excitation energy transfer through the phycobilin pigments of the phycobilisome to chlorophyll with steady-state and time-resolved fluorescence excitation and emission spectroscopy. Quenching was investigated in both a photosystem II-less mutant, and DCMU-poisoned wild-type Synechocystis sp. PCC 6803. The action spectra for blue-light-induced quenching was identical in both cell types and was dominated by a band in the blue region, peaking at 480 nm. Fluorescence quenching and its dark recovery was inhibited by the protein cross-linking agent glutaraldehyde, which could maintain cells in either the quenched or the unquenched state. We found that high phosphate concentrations that inhibit phycobilisome mobility and the regulation of energy transfer by the light-state transition did not affect blue-light-induced fluorescence quenching. Both room temperature and 77 K fluorescence emission spectra revealed that fluorescence quenching was associated with phycobilin emission. Quenching was characterized by a decrease in the emission of allophycocyanin and long wavelength phycobilisome terminal emitters relative to that of phycocyanin. A global analysis of the room-temperature fluorescence decay kinetics revealed that phycocyanin and photosystem I decay components were unaffected by quenching, whereas the decay components originating from allophycocyanin and phycobilisome terminal emitters were altered. Our data support a regulatory mechanism involving a protein conformational change and/or change in protein-protein interaction which quenches excitation energy at the core of the phycobilisome.

Molecular dynamics simulations have been performed to study photosystem II structure and function. Structural information obtained from simulations was combined with ab initio computations of chromophore excited states. In contrast to calculations based on the x-ray structure, the molecular-dynamics-based calculations accurately predicted the experimental absorbance spectrum. In addition, our calculations correctly assigned the energy levels of reaction-center (RC) chromophores, as well as the lowest-energy antenna chlorophyll. The primary and secondary quinone electron acceptors, Q(A) and Q(B), exhibited independent changes in position over the duration of the simulation. Q(B) fluctuated between two binding sites similar to the proximal and distal sites previously observed in light- and dark-adapted RC from purple bacteria. Kinetic models were used to characterize the relative influence of chromophore geometry, site energies, and electron transport rates on RC efficiency. The fluctuating energy levels of antenna chromophores had a larger impact on quantum yield than did their relative positions. Variations in electron transport rates had the most significant effect and were sufficient to explain the experimentally observed multi-component decay of excitation in photosystem II. The implications of our results are discussed in the context of competing evolutionary selection pressures for RC structure and function.

The membrane-spanning connexin proteins form microscopic intercellular channels that directly connect the cytoplasms of adjacent cells and as such have been implicated in maintenance of tissue homeostasis. They are considered to act as tumor suppressors since their function or expression is frequently aberrant in tumor cells. Several mechanisms appear to be involved in this, but irreversible mutational alterations have not yet been proved to be among them. In this study we have demonstrated for the first time that connexin 43 but not connexin 32 is specifically and quite frequently mutated in human colon sporadic adenocarcinomas. All tumor-associated mutations led to a shift of reading frame and were located in the multifunctional carboxylterminal domain of the protein. Expression of mutated connexin 43 protein was restricted to invasive structures of tumors. These findings suggest that mutational alterations of connexin 43 are involved in advanced stages of progression of human colon cancer towards malignancy.

The induction of the isiA (CP43#) protein in iron-stressed cyanobacteria is accompanied by the formation of a ring of 18 CP43# proteins around the photosystem I (PSI) trimer and is thought to increase the absorption cross section of PSI within the CP43#-PSI supercomplex. In contrast to these in vitro studies, our in vivo measurements failed to demonstrate any increase of the PSI absorption cross section in two strains (Synechococcus sp. PCC 7942 and Synechocystis sp. PCC 6803) of iron-stressed cells. We report that iron-stressed cells exhibited a reduced capacity for state transitions and limited dark reduction of the plastoquinone pool, which accounts for the increase in PSII-related 685 nm chlorophyll fluorescence under iron deficiency. This was accompanied by lower abundance of the NADP-dehydrogenase complex and the PSI-associated subunit PsaL, as well as a reduced amount of phosphatidylglycerol. Nondenaturating polyacrylamide gel electrophoresis separation of the chlorophyllprotein complexes indicated that the monomeric form of PSI is favored over the trimeric form of PSI under iron stress. Thus, we demonstrate that the induction of CP43# does not increase the PSI functional absorption cross section of whole cells in vivo, but rather, induces monomerization of PSI trimers and reduces the capacity for state transitions. We discuss the role of CP43# as an effective energy quencher to photoprotect PSII and PSI under unfavorable environmental conditions in cyanobacteria in vivo.