Photosystem II antenna complexes CP26 and CP29 are essential for nonphotochemical quenching in Chlamydomonas reinhardtii

Photosystems must balance between light harvesting to fuel the photosynthetic process for CO₂ fixation and mitigating the risk of photodamage due to absorption of light energy in excess. Eukaryotic photosynthetic organisms evolved an array of pigment-binding proteins called light harvesting complexes constituting the external antenna system in the photosystems, where both light harvesting and activation of photoprotective mechanisms occur. In this work, the balancing role of CP29 and CP26 photosystem II antenna subunits was investigated in Chlamydomonas reinhardtii using CRISPR-Cas9 technology to obtain single and double mutants depleted of monomeric antennas. Absence of CP26 and CP29 impaired both photosynthetic efficiency and photoprotection: Excitation energy transfer from external antenna to reaction centre was reduced, and state transitions were completely impaired. Moreover, differently from higher plants, photosystem II monomeric antenna proteins resulted to be essential for photoprotective thermal dissipation of excitation energy by nonphotochemical quenching.     

A mechanism for regulation of chloroplast LHC II kinase by plastoquinol and thioredoxin

State transitions are acclimatory responses to changes in light quality in photosynthesis. They involve the redistribution of absorbed excitation energy between photosystems I and II. In plants and green algae, this redistribution is produced by reversible phosphorylation of the chloroplast light harvesting complex II (LHC II). The LHC II kinase is activated by reduced plastoquinone (PQ) in photosystem II-specific low light. In high light, when PQ is also reduced, LHC II kinase becomes inactivated by thioredoxin. Based on newly identified amino acid sequence features of LHC II kinase and other considerations, a mechanism is suggested for its redox regulation.     

Complex formation in plant thylakoid membranes. Competition studies on membrane protein interactions using synthetic peptide fragments

Thylakoid membranes of pea were used to study competition between extra-membrane fragments and their parental membrane-bound proteins. Phosphorylated and unphosphorylated fragments of light harvesting complex II (LHC II) from higher plants were used to compete with LHC II for interactions with itself and with other thylakoid protein complexes. Effects of these peptide fragments of LHC II and of control peptides were followed by 80 K chlorophyll fluorescence spectroscopy of isolated thylakoids. The phosphorylated LHC II fragment competes with membrane-bound phosphoproteins in the phosphatase reaction. The same fragment accelerates the process of dark-to-light adaptation and decreases the rate of the light-to-dark adaptation when these are followed by fluorescence spectroscopy. In contrast, the non-phosphorylated LHC II peptide does not affect the rate of adaptation but produces results consistent with inhibition of formation of a quenching complex. In this quenching complex we propose that LHC II remains inaccessible to the LHC II kinase, explaining an observed decrease in LHC II phosphorylation in the later stages of the time-course of phosphorylation. The most conspicuous protein which is steadily phosphorylated during the time-course of phosphorylation is the 9 kDa (psbH) protein. The participation of the phosphorylated form of psbH in the quenching complex, where it is inaccessible to the phosphatase, may explain its anomalously slow dephosphorylation. The significance of the proposed complex of LHC II with phospho-psbH is discussed.Abbreviations LHC II light harvesting complex II - PS II Photosystem II - PS I Photosystem I     

Structural analysis and comparison of light-harvesting complexes I and II

Photosynthesis is a fundamental biological process involving the conversion of solar energy into chemical energy. The initial photochemical and photophysical events of photosynthesis are mediated by photosystem II (PSII) and photosystem I (PSI). Both PSII and PSI are multi-subunit supramolecular machineries composed of a core complex and a peripheral antenna system. The antenna system serves to capture light energy and transfer it to the core efficiently. Both PSII and PSI in the green lineage (plants and green algae) and PSI in red algae have an antenna system comprising a series of chlorophyll- and carotenoid-binding membrane proteins belonging to the light-harvesting complex (LHC) superfamily, including LHCII and LHCI. However, the antenna size and subunit composition vary considerably in the two photosystems from diverse organisms. On the basis of the plant and algal LHCII and LHCI structures that have been solved by X-ray crystallography and single-particle cryo-electron microscopy we review the detailed structural features and characteristic pigment properties of these LHCs in PSII and PSI. This article is part of a Special Issue entitled Light harvesting, edited by Dr. Roberta Croce.     

Characterization of a novel Photosystem I-LHCI supercomplex isolated from Chlamydomonas reinhardtii under anaerobic (State II) conditions

A novel supercomplex of Photosystem I (PSI) with light harvesting complex I (LHCI) was isolated from the green alga Chlamydomonas reinhardtii. This novel supercomplex is unique as it is the first stable supercomplex of PSI together with its external antenna. The supercomplex contains 256 chlorophylls per reaction center. The supercomplex was isolated under anaerobic conditions and may represent the State II form of the photosynthetic unit. In contrast to previously reported supercomplexes isolated in State I, which contain only 4 LHC I proteins, this supercomplex contains 10-11 LHC I proteins tightly bound to the PSI core. In contrast to plants, no LHC II is tightly bound to the PSI-LHCI supercomplex in State II. Investigation of the energy transfer from the antenna system to the reaction center core shows that the LHC supercomplexes are tightly coupled to the PSI core, not only structurally but also energetically. The excitation energy transfer kinetics are completely dominated by the fast phase, with a near-complete lack of long-lived fluorescence. This tight coupling is in contrast to all reports of energy transfer in PSI-LHCI supercomplexes (in State I), which have so far been described as weakly coupled supercomplexes with low efficiency for excitation energy transfer. These results indicate that there are large and dynamic changes of the PSI-LHCI supercomplex during the acclimation from aerobic (State I) to anaerobic (State II) conditions in Chlamydomonas.     

Cation-mediated regulation of excitation energy distribution in chloroplasts lacking organized Photosystem II complexes

Despite the total loss of Photosystem II activity, thylakoids isolated from the green nuclear maize mutant hcf1-3 contain normal amounts of the light-harvesting chlorophyll $\text{a}\text{b}$ pigment-protein complex (LHC). We interpret the spectroscopic and ultrastructural characteristics of these thylakoids to indicate that the LHC present in these membranes is not associated with Photosystem II reaction centers and thus exists in a ‘free’ state within the thylakoid membrane. In contrast, the LHC found in wild-type maize thylakoids shows the usual functional association with Photosystem II reaction centers. Several lines of evidence suggest that the free LHC found in thylakoids isolated from hcf1-3 is able to mediate cation-dependent changes in both thylakoid appression and energy distribution between the photosystems: (1) Thylakoids isolated from hcf1-3 and wild-type seedlings exhibit a similar Mg²⁺-dependent increase in the short/long wavelength fluorescence emission peak ratio at 77 K. This Mg²⁺ effect is lost following incubation of thylakoids isolated from either source with low concentrations of trypsin. Such treatment results in the partial proteolysis of the LHC in both membrane types. (2) Thylakoids isolated from both hcf1-3 and wild-type seedlings show a similar Mg²⁺ dependence for the enhancement of the maximal yield of room temperature fluorescence and light scattering; both Mg²⁺ effects are abolished by brief incubation of the thylakoids with low concentrations of trypsin (3) Mg²⁺ acts to reduce the relative quantum efficiency of Photosystem I-dependent electron transport at limiting 650 nm light in thylakoids isolated from hcf1-3. (4) The pattern of digitonin fractionation of thylakoid membranes, which is dependent upon structural membrane interactions and upon LHC in the thylakoids, is similar in thylakoids isolated from both hcf1-3 and wild-type seedlings. We conclude that the surface-exposed segment of the LHC, but not the LHC-Photosystem II core association, is necessary for the cation-dependent changes in both thylakoid appression and energy distribution between the two photosystems, and that the LHC itself is able to transfer excitation energy directly to Photosystem I in a Mg²⁺-dependent fashion in the absence of Photosystem II reaction centers. The latter phenomenon is equivalent to a cation-induced change in the absorptive cross-section of Photosystem I.     

The consequences of chlorophyll deficiency for photosynthetic light use efficiency in a single nuclear gene mutation of cowpea

The light harvesting and photosynthetic characteristics of a chlorophyll-deficient mutant of cowpea (Vigna unguilata), resulting from a single nuclear gene mutation, are examined. The 40% reduction in total chlorophyll content per leaf area in the mutant is associated with a 55% reduction in pigment-proteins of the light harvesting complex associated with Photosystem II (LHC II), and to a lesser extent (35%) in the light harvesting complex associated with Photosystem I (LHC I). No significant differences were found in the Photosystem I (PS I) and Photosystem II (PS II) contents per leaf area of the mutant compared to the wildtype parent. The decreases in the PS I and PS II antennae sizes in the mutant were not accompanied by any major changes in quantum efficiencies of PS I and PS II in leaves at non-saturating light levels for CO₂ assimilation. Although the chlorophyll deficiency resulted in an 11% decrease in light absorption by mutant leaves, their maximum quantum yield and light saturated rate of CO₂ assimilation were similar to those of wildtype leaves. Consequently, the large and different decreases in the antennae of PS II and PS I in the mutant are not associated with any loss of light use efficiency in photosynthesis.Abbreviations LHC I, LHC II light harvesting chlorophyll a/b protein complexes associated with PS I and PS II - A₈₂₀ light-induced absorbance change at 820 nm - ø_{PS I}, ø_{PS II} relative quantum efficiencies of PS I and PS II photochemistry     

Long-wavelength absorbing antenna pigments and heterogeneous absorption bands concentrate excitons and increase absorption cross section

The light-harvesting apparatus of photosynthetic organisms is highly optimized with respect to efficient collection of excitation energy from photons of different wavelengths and with respect to a high quantum yield of the primary photochemistry. In many cases the primary donor is not an energetic trap as it absorbs hypsochromically compared to the most red-shifted antenna pigment present (long-wavelength antenna). The possible reasons for this as well as for the spectral heterogeneity which is generally found in antenna systems is examined on a theoretical basis using the approach of thermal equilibration of the excitation energy. The calculations show that long-wavelength antenna pigments and heterogeneous absorption bands lead to a concentration of excitons and an increased effective absorption cross section. The theoretically predicted trapping times agree remarkably well with experimental data from several organisms. It is shown that the kinetics of the energy transfer from a long-wavelength antenna pigment to a hypsochromically absorbing primary donor does not represent a major kinetic limitation. The development of long-wavelength antenna and spectrally heterogeneous absorption bands means an evolutionary advantage based on the chromatic adaptation of photosynthetic organelles to spectrally filtered light caused by self-absorption.Abbreviations LHC light-harvesting complex - P primary donor - PSI Photosystem I of green plants - PS II Photosystem II of green plants - RC reaction center - X primary acceptor     

Photoacoustic studies on the dependence of state transitions on grana stacking

Photoacoustic detection of oxygen evolution and Emerson enhancement in state 1 and state 2 were compared in a tobacco wild type and mutant (Su/su) deficient in chlorophyll. The mutant shows smaller changes in the distribution of excitation energy between the two photosystems than the wild type. Analysis of Emerson enhancement saturation curves indicates that in the mutant which is deficient in grana partitions and shows less stacking, state 1-state 2 transitions reflect changes in the yield of energy transfer from PS II to PS I (spillover). On the other hand, the wild type containing large grana shows changes in absorption cross-sections of the two photosystems upon state transitions. NaF, a specific phosphatase inhibitor, blocks the transition to state 1, indicating that LHC II phosphorylation has a role in excitation energy regulation in both the mutant as well as the wild type. It is demonstrated that N-ethylmaleimide, a specific sulfhydryl reagent, blocks the transition to state 2, suggesting that a disulfide-sulfhydryl redox couple activates the LHC II kinase in vivo.Abbreviations LHC II light harvesting chlorophyll a/b pigment protein complex of PS II - LHC II-P phosphorylated complex - NEM N-ethylmaleimide     

Protein tyrosine phosphorylation in the transition to light state 2 of chloroplast thylakoids

Redox dependent protein phosphorylation in chloroplast thylakoids regulates distribution of excitation energy between the two photosystems of photosynthesis, PS I and PS II. Several thylakoid phosphoproteins are known to be phosphorylated on N-terminal threonine residues exposed to the chloroplast stroma. Phosphorylation of light harvesting complex II (LHC II) on Thr-6 is thought to account for redistribution of light energy from PS II to PS I during the transition to light state 2. Here, we present evidence that a protein tyrosine kinase activity is required for the transition to light state 2. With an immunological approach using antibodies directed specifically towards either phospho-tyrosine or phospho-threonine, we observed that LHC II became phosphorylated on both tyrosine and threonine residues. The specific protein tyrosine kinase inhibitor genistein, at concentrations causing no direct effect on threonine kinase activity, was found to prevent tyrosine phosphorylation of LHC II, the transition to light state 2, and associated threonine phosphorylation of LHC II. Possible reasons for an involvement of tyrosine phosphorylation in light state transitions are proposed and discussed. This revised version was published online in June 2006 with corrections to the Cover Date.     

Isolation and characterization of a large photosystem I–light‐harvesting complex II supercomplex with an additional Lhca1–a4 dimer in Arabidopsis

The biological conversion of light energy into chemical energy is performed by a flexible photosynthetic machinery located in the thylakoid membranes. Photosystems I and II (PSI and PSII) are the two complexes able to harvest light. PSI is the last complex of the electron transport chain and is composed of multiple subunits: the proteins building the catalytic core complex that are well conserved between oxygenic photosynthetic organisms, and, in green organisms, the membrane light‐harvesting complexes (Lhc) necessary to increase light absorption. In plants, four Lhca proteins (Lhca1–4) make up the antenna system of PSI, which can be further extended to optimize photosynthesis by reversible binding of LHCII, the main antenna complex of photosystem II. Here, we used biochemistry and electron microscopy in Arabidopsis to reveal a previously unknown supercomplex of PSI with LHCII that contains an additional Lhca1–a4 dimer bound on the PsaB–PsaI–PsaH side of the complex. This finding contradicts recent structural studies suggesting that the presence of an Lhca dimer at this position is an exclusive feature of algal PSI. We discuss the features of the additional Lhca dimer in the large plant PSI–LHCII supercomplex and the differences with the algal PSI. Our work provides further insights into the intricate structural plasticity of photosystems.     

Chlorophyll fluorescence quenching in the alga Euglena gracilis

When far red light preincubated cells of Euglena gracilis are transferred to dark or light, chlorophyll fluorescence (F₀ and F_m) decreases. Non-photochemical quenching in the dark is suggested to be induced partly by chlororespiration and partly by changes in the distribution of excitation energy between the photosystems. Depending on the light intensities it was possible to resolve the non-photochemical quenching into at least three different components. The slowest relaxation phase of non-photochemical quenching occurred only after exposure to high light and was assigned to photoinhibition. The other two components were an energy-dependent quenching (qE), and the one which we attribute to a spill over mechanism. We suggest that both photosystems use a common antenna system consisting of LHC I and LHC II proteins. In contrast to higher plants, qE in Euglena gracilis is independent of the xanthophyll cycle and an aggregation of LHC II. This revised version was published online in June 2006 with corrections to the Cover Date.     

Light-Harvesting Features Revealed by the Structure of Plant Photosystem I

Oxygenic photosynthesis is driven by two multi-subunit membrane protein complexes, Photosystem I and Photosystem II. In plants and green algae, both complexes are composed of two moieties: a reaction center (RC), where light-induced charge translocation occurs, and a peripheral antenna that absorbs light and funnels its energy to the reaction center. The peripheral antenna of PS I (LHC I) is composed of four gene products (Lhca 1-4) that are unique among the chlorophyll a/b binding proteins in their pronounced long-wavelength absorbance and in their assembly into dimers. The recently determined structure of plant Photosystem I provides the first relatively high-resolution structural model of a super-complex containing a reaction center and its peripheral antenna. We describe some of the structural features responsible for the unique properties of LHC I and discuss the advantages of the particular LHC I dimerization mode over monomeric or trimeric forms. In addition, we delineate some of the interactions between the peripheral antenna and the reaction center and discuss how they serve the purpose of dynamically altering the composition of LHC I in response to environmental pressure. Combining structural insight with spectroscopic data, we propose how altering LHC I composition may protect PS I from excessive light.     

Drying pretreatment enhances the photosynthetic stability of alginate immobilisedPhormidium laminosum

Summary Immobilisation of the thermophilic cyanobacteriumP. laminosum in alginate beads with a drying pretreatment led to stabilization of the Photosystem II water splitting activity for at least 3 months. This was accompanied by an increase of energy transfer from phycobilins, a maintenance of the variable fluorescence and a red shift of 77k emissions of allophycocyanin and PSI complexes. These changes indicate improvements in the photosynthetic efficiencies of immobilised cells.Abbreviations PSI, II Photosystem I, II: Chl a: chlorophyll a - LHC light harvesting complex - DCP IP 2–6 dichlorophenol indophenol - DCMU 3(3,4-dichlorophenyl)-1,1 dimethylurea - IMPD 2, 3, 5, 6 tetramethyl phenylenediamine     

Electron transport and photophosphorylation by Photosystem I in vivo in plants and cyanobacteria

Recently, a number of techniques, some of them relatively new and many often used in combination, have given a clearer picture of the dynamic role of electron transport in Photosystem I of photosynthesis and of coupled cyclic photophosphorylation. For example, the photoacoustic technique has detected cyclic electron transport in vivo in all the major algal groups and in leaves of higher plants. Spectroscopic measurements of the Photosystem I reaction center and of the changes in light scattering associated with thylakoid membrane energization also indicate that cyclic photophosphorylation occurs in living plants and cyanobacteria, particularly under stressful conditions.In cyanobacteria, the path of cyclic electron transport has recently been proposed to include an NAD(P)H dehydrogenase, a complex that may also participate in respiratory electron transport. Photosynthesis and respiration may share common electron carriers in eukaryotes also. Chlororespiration, the uptake of O₂ in the dark by chloroplasts, is inhibited by excitation of Photosystem I, which diverts electrons away from the chlororespiratory chain into the photosynthetic electron transport chain. Chlororespiration in N-starved Chlamydomonas increases ten fold over that of the control, perhaps because carbohydrates and NAD(P)H are oxidized and ATP produced by this process.The regulation of energy distribution to the photosystems and of cyclic and non-cyclic phosphorylation via state 1 to state 2 transitions may involve the cytochrome b ₆-f complex. An increased demand for ATP lowers the transthylakoid pH gradient, activates the b ₆-f complex, stimulates phosphorylation of the light-harvesting chlorophyll-protein complex of Photosystem II and decreases energy input to Photosystem II upon induction of state 2. The resulting increase in the absorption by Photosystem I favors cyclic electron flow and ATP production over linear electron flow to NADP and poises the system by slowing down the flow of electrons originating in Photosystem II.Cyclic electron transport may function to prevent photoinhibition to the photosynthetic apparatus as well as to provide ATP. Thus, under high light intensities where CO₂ can limit photosynthesis, especially when stomates are closed as a result of water stress, the proton gradient established by coupled cyclic electron transport can prevent over-reduction of the electron transport system by increasing thermal de-excitation in Photosystem II (Weis and Berry 1987). Increased cyclic photophosphorylation may also serve to drive ion uptake in nutrient-deprived cells or ion export in salt-stressed cells.There is evidence in some plants for a specialization of Photosystem I. For example, in the red alga Porphyra about one third of the total Photosystem I units are engaged in linear electron transfer from Photosystem II and the remaining two thirds of the Photosystem I units are specialized for cyclic electron flow. Other organisms show evidence of similar specialization.Improved understanding of the biological role of cyclic photophosphorylation will depend on experiments made on living cells and measurements of cyclic photophosphorylation in vivo.Abbreviations CCCP carbonylcyanide m-chlorophenylhydrazone - cyt cytochrome - DBMIB 2,5-dibromo-3-methyl-6-isopropyl-p-benzoquinone - DCCD dicyclohexylcarbodiimide - DCHC dicyclohexyl-18-crown-6 - DCMU 3-(3,4-dichlorophenyl)-1,1-dimethylurea - FCCP carbonylcyanide 4-(trifluoromethoxy) phenylhydrazone - LHC light harvesting chlorophyll - LHCP II light harvesting chlorophyll protein of Photosystem II - PQ plastoquinone - PS I, II Photosystem I, II - SHAM salicyl hydroxamic acid - TBT Tri-n-butyltin CIW/DPB Publication No. 1146     

Rapid isolation of photosystem I chlorophyll-binding proteins by anion exchange perfusion chromatography

With the new method of anion exchange perfusion chromatography we have devised an extremely rapid technique to subfractionate spinach Photosystem I into its chlorophyll a containing core complex and various components of the Photosystem I light-harvesting antenna (LHC I). The isolation time for the LHC I subcomplexes following solubilisation of native Photosystem I was reduced from 50 h using traditional density centrifugation procedures down to only 10–25 min by perfusion chromatography. Within this very short period of isolation, LHC I has been obtained as subfractions highly enriched in Lhca2+3 (LHC I-680) and Lhca1+4 (LHC I-730). Moreover, other highly enriched subfractions of LHC I such as Lhca2, Lhca3 and Lhca1+2+4 were obtained where the later two populations have not previously been obtained in a soluble form and without the use of SDS. These various subfractions of the LHC I antenna have been characterised by absorption spectroscopy, 77 K fluorescence-spectroscopy and SDS-PAGE demonstrating their identities, functional intactness and purity. Furthermore, the analyses located a chlorophyll b pool to preferentially transfer its excitation energy to the low energy F735 chromophore, and located specifically the origin of the 730 nm fluorescence to the Lhca4 component. It was also revealed that Lhca2 and Lhca3 have identical light-harvesting properties. The isolated Photosystem I core complex showed high electron transport capacity (1535 moles O₂ mg Chl^–1 h^–1) and low fluorescence yield (0.4%) demonstrating its high functional integrity. The very rapid isolation procedure based upon perfusion chromatography should in a significant way facilitate the subfractionation of Photosystem I proteins and thereby allow more accurate functional and structural studies of individual components.Abbreviations a.u. arbitrary units - DCIP 2.6-dichlorophenol indophenol - LHC light harvesting complex     

Energy distribution in the photochemical apparatus of Porphyridium cruentum in state I and state II

Fluorescence of Porphyridium cruentum in state I (cells equilibrated in light absorbed predominantly by Photosystem I) and in state II (cells equilibrated in light absorbed appreciably by Photosystem II) was examined to determine how the distribution of excitation energy was altered in the transitions between state I and state II. Low temperature emission spectra of cells frozen in state I and state II confirmed that a larger fraction of the excitation energy is delivered to Photosystem II in state I. Low temperature measurements showed that the yield of energy transfer from Photosystem II to Photosystem I was greater in state II and calculations indicated that the photochemical rate constant for such energy transfer was approximately twice as large in state II. Measurements at low temperature also showed that the cross sections and the spectral properties of the photosystems did not change in the transitions between state I and state II. In agreement with predictions made from the parameters measured at low temperature, the action spectra for oxygen evolution measured at room temperature were found to be the same in state I and state II.     

The composition and spectral properties of three different forms of light-harvesting complex II

Light-harvesting pigment-protein complexes arrayed in the thylakoid membrane serve as antenna to capture light energy and deliver it to photosynthetic reaction centers. The antenna complex of photosystem II (LHC II) is the most abundant pigment-protein complex in green plants. LHC II contains a set of polypeptides encoded by nuclear genes belonging to Lhcb family, of which, LHCB1, LHCB2 and LHCB3, encoded by Lhcb13, assemble to form heterotrimer on thylakoid membrane. The LHC II tr…     

Thylakoid protein phosphorylation in dynamic regulation of photosystem II in higher plants

In higher plants, the photosystem (PS) II core and its several light harvesting antenna (LHCII) proteins undergo reversible phosphorylation cycles according to the light intensity. High light intensity induces strong phosphorylation of the PSII core proteins and suppresses the phosphorylation level of the LHCII proteins. Decrease in light intensity, in turn, suppresses the phosphorylation of PSII core, but strongly induces the phosphorylation of LHCII. Reversible and differential phosphorylation of the PSII-LHCII proteins is dependent on the interplay between the STN7 and STN8 kinases, and the respective phosphatases. The STN7 kinase phosphorylates the LHCII proteins and to a lesser extent also the PSII core proteins D1, D2 and CP43. The STN8 kinase, on the contrary, is rather specific for the PSII core proteins. Mechanistically, the PSII-LHCII protein phosphorylation is required for optimal mobility of the PSII-LHCII protein complexes along the thylakoid membrane. Physiologically, the phosphorylation of LHCII is a prerequisite for sufficient excitation of PSI, enabling the excitation and redox balance between PSII and PSI under low irradiance, when excitation energy transfer from the LHCII antenna to the two photosystems is efficient and thermal dissipation of excitation energy (NPQ) is minimised. The importance of PSII core protein phosphorylation is manifested under highlight when the photodamage of PSII is rapid and phosphorylation is required to facilitate the migration of damaged PSII from grana stacks to stroma lamellae for repair. The importance of thylakoid protein phosphorylation is highlighted under fluctuating intensity of light where the STN7 kinase dependent balancing of electron transfer is a prerequisite for optimal growth and development of the plant. This article is part of a Special Issue entitled: Photosystem II.     

The composition and spectral properties of three different forms of light-harvesting complex II

Different aggregates of LHC II play a very important role in regulating the light absorption and excitation energy transfer of plant. Trimeric LHC II was purified from spinach thylakoid membrane. In order to obtain the dimeric and monomeric LHC II, the trimer was treated with the mixture of 2% OGP and 10 μg/mL PLA₂, then loaded onto the sucrose density gradient in the presence of 0.06% triton X-100. The LHC II trimer, dimer and monomer isolated by sucrose density gradient all contained three polypeptides with molecular weight of 29, 28 and 26 kd respectively. The pigment composition showed much difference in the content of Chl b and xanthophyll among three forms of LHC II. To study the light capture and excitation energy transfer in different forms of LHC II, the absorption and fluorescence spectra were analyzed. The results clearly showed that the efficiency of energy absorption and transfer was different in the three kinds of LHC II, the highest for trimeric LHC II, intermediate for dimeric LHC II, and the lowest for monomeric LHC II. It was suggested that there might be a physiological homeostasis of different aggregates of LHC II in plants, which is significant for the plant self-regulating upon exposure to variable light environment.