Evidence for dissociation of chlorophyll b from the main light-harvesting complex in the oligomerization state isolated from marine alga, Bryopsis corticulans

We investigated the composition and organization of chlorophylls in monomers, trimers and oligomers (small aggregates) of the main light-harvesting complex (LHC II) isolated from marine alga, Bryopsis corticulans, using a combination of measurements with reversed-phase high performance liquid chromatography (RP-HPLC) and steady-state spectroscopy of absorption, circular dichroism (CD) and low temperature fluorescence. The composition and organization of the chlorophylls in monomeric and trimeric LHC II were essentially identical to those of LHC II from higher plants. For LHC II oligomers, a large decrease of chlorophyll (Chl) b absorption and of CD signals corresponding to Chl b was consistent with the quantitative analysis of Chl b by RP-HPLC, indicating that oligomerization of the LHC II proteins significantly influenced spectroscopic properties and led to the dissociation of Chl b molecules from LHC II. Our data strongly suggested that protein oligomerization constitutes a structural basis for the decrease of Chl b molecules in LHC II of B. corticulans. The LHC II of B. corticulans might play a photoprotective role with the reduction of the ability of light absorption via alteration of its own structural conformation.     

Generation of fluorescence quenchers from the triplet states of chlorophylls in the major light-harvesting complex II from green plants

Laser flash-induced changes of the fluorescence yield were studied in aggregates of light-harvesting complex II (LHCII) on a time scale ranging from microseconds to seconds. Carotenoid (Car) and chlorophyll (Chl) triplet states, decaying with lifetimes of several microseconds and hundreds of microseconds, respectively, are responsible for initial light-induced fluorescence quenching via singlet-triplet annihilation. In addition, at times ranging from milliseconds to seconds, a slow decay of the light-induced fluorescence quenching can be observed, indicating the presence of additional quenchers generated by the laser. The generation of the quenchers is found to be sensitive to the presence of oxygen. It is proposed that long-lived fluorescence quenchers can be generated from Chl triplets that are not transferred to Car molecules. The quenchers could be Chl cations or other radicals that are produced directly from Chl triplets or via Chl triplet-sensitized singlet oxygen. Decay of the quenchers takes place on a millisecond to second time scale. The decay is slowed by a few orders of magnitude at 77 K indicating that structural changes or migration-limited processes are involved in the recovery. Fluorescence quenching is not observed for trimers, which is explained by a reduction of the quenching domain size compared to that of aggregates. This type of fluorescence quenching can operate under very high light intensities when Chl triplets start to accumulate in the light-harvesting antenna.     

Effect of detergent on aggregation of the light-harvesting chlorophyll a/b complex of photosystem 2 and its impact for carotenoid function and fluorescence quenching

Spectroscopy was used to investigate the fluorescence quenching mechanism in light-harvesting complex 2 (LHC2). The 77 K fluorescence excitation spectroscopy was performed for detection of aggregation state of LHC2 treated with different concentrations of octylphenol poly(ethyleneglycol ether)₁₀ (TX-100). Resonance Raman (RR) spectra excited with 488, 496, and 514 nm provided molecular configuration of neoxanthin, lutein 1, and lutein 2, respectively. At increased concentration of TX-100, the RR signals of xanthophylls were enhanced in the four frequency regions, which was accompanied with increase of fluorescence of chlorophyll (Chl) a. Thus the absorption of the three xanthophyll molecules was inclined to excitation wavelength, which proved that functional configurations of xanthophyll molecules in LHC2 were vital for fast transfer of excitation energy to Chl a molecules. Changes in the v4 region (C-H out-of-plane bending modes, at ∼960 cm⁻¹ in RR spectra) demonstrated that the twist feature of neoxanthin, lutein 1, and lutein 2 molecules existed in LHC2 trimers, however, it was lost in the LHC2 macro-aggregates. In the second derivative absorption spectra of LHC2, neoxanthin absorption was not detected in LHC2 macro-aggregates, while evident absorption was found in LHC2 trimers and this absorption decreased obviously when TX-100 concentration was higher than 1 mM. Hence the neoxanthin molecule had a structural role in formation of LHC2 trimers. The RR and absorption spectra also implied that carotenoid molecules constructed the functional LHC2 trimers via their intrinsic configuration features, which enabled energy transfer to Chl a efficiently and led to lower fluorescence quenching efficiency. In contrast, these intrinsic twist configurations were lost in LHC2 macro-aggregates and led to lower energy transfer efficiency and higher fluorescence quenching efficiency.     

Energy transfer in the light-harvesting complex II of Dunaliella tertiolecta is unusually sensitive to Triton X-100

Triton X-100, a detergent commonly used to solubilize higher plant thylakoid membranes, was found to be deleterious to Dunaliella LHC II. It disrupted the transfer of excitation energy from chlorophyll b to chlorophyll a. Based on analysis of pigments and immunoassays of LHC II apoproteins from sucrose density gradient fractions, Triton X-100 caused aggregation of the complex, but apparently did not remove chlorophyll b from the apoprotein. Following solubilization with Triton X-100 only CPI could be resolved by electrophoresis. In contrast, solubilization of Dunaliella thylakoids with octyl--D-glucopyranoside preserved energy transfer from chlorophyll b to chlorophyll a. This detergent also effectively prevented aggregation on sucrose gradients and preserved CPI oligomers, as well as LHCP1 and LHCP3 on non-denaturing gels. Solubilization with Deriphat gave similar results. We propose that room temperature fluorescence excitation and emission spectroscopy be used in conjunction with other biophysical and biochemical probes to establish the effects of detergents on the integrity of light harvesting chlorophyll protein complexes. Methods used here may be applicable to other chlorophytes which prove refractory to protocols developed for higher plants.Abbreviations LHC II light harvesting chlorophyll protein complex associated with photosystem II - LHCP1 and LHCP3 monomeric and oligomeric forms of LHC II, respectively, observed on non-denaturing gels - LiDS lithium dodecylsulphate - PMSF phenylmethylsulfonyl fluoride     

Crystal structure of plant light‐harvesting complex shows the active,energy‐transmitting state

Plants dissipate excess excitation energy as heat by non‐photochemical quenching (NPQ). NPQ has been thought to resemble in vitro aggregation quenching of the major antenna complex, light harvesting complex of photosystem II (LHC‐II). Both processes are widely believed to involve a conformational change that creates a quenching centre of two neighbouring pigments within the complex. Using recombinant LHC‐II lacking the pigments implicated in quenching, we show that they have no particular role. Single crystals of LHC‐II emit strong, orientation‐dependent fluorescence with an emission maximum at 680 nm. The average lifetime of the main 680 nm crystal emission at 100 K is 1.31 ns, but only 0.39 ns for LHC‐II aggregates under identical conditions. The strong emission and comparatively long fluorescence lifetimes of single LHC‐II crystals indicate that the complex is unquenched, and that therefore the crystal structure shows the active, energy‐transmitting state of LHC‐II. We conclude that quenching of excitation energy in the light‐harvesting antenna is due to the molecular interaction with external pigments in vitro or other pigment–protein complexes such as PsbS in vivo, and does not require a conformational change within the complex.     

Polyamines induce aggregation of LHC II and quenching of fluorescence in vitro

Dissipation of excess excitation energy within the light-harvesting complex of Photosystem II (LHC II) is a main process in plants, which is measured as the non-photochemical quenching of chlorophyll fluorescence or qE. We showed in previous works that polyamines stimulate qE in higher plants in vivo and in eukaryotic algae in vitro. In the present contribution we have tested whether polyamines can stimulate quenching in trimeric LHC II and monomeric light-harvesting complex b proteins from higher plants. The tetramine spermine was the most potent quencher and induced aggregation of LHC II trimers, due to its highly cationic character. Two transients are evident at 100μM and 350μM for the fluorescence and absorbance signals of LHC II respectively. On the basis of observations within this work, some links between polyamines and the activation of qE in vivo is discussed.     

Release and aggregation of the light-harvesting complex in intact leaves subjected to strong CO2 deficit

Tobacco plants were subjected to long-term CO₂ deficit. The stress caused photoinhibition of Photosystem (PS) II photochemistry and the aggregation of the light-harvesting complex of PS II (LHC II). The aggregation was shown by the appearance of the characteristic band at 698–700 nm (F₆₉₉) in 77 K fluorescence emission spectra. LHC II aggregates are considered to quench fluorescence and, therefore, the fluorescence yield was determined to verify their quenching capability. PS II photochemistry, measured as F_V/F_M, was largely depressed during first 4 days of the stress. Unexpectedly, the total fluorescence yield increased in this period. Fitting of emission spectra by Gaussian components approximating emission bands of LHC II, PS II core, PS I and F₆₉₉ revealed that mainly the bands at 680 and 699 nm, representing emission of LHC II aggregates, were responsible for the increase of the fluorescence yield. This shows an interruption of the excitation energy transfer between LHC II and both photosystems and, thus, a physical disconnection of LHC II from photosystems. PS II and PS I emissions were not quenched in this period. Therefore, it was concluded that these LHC II aggregates were accumulated out of PS II antenna, and, thus they cannot be involved in dumping of excess excitation. The total fluorescence yield turned to decrease only after the large depression of PS II photochemistry, when LHC II aggregation was considerably speeded up and the fluorescence yields of PS I and II turned to decline.     

The light-harvesting chlorophyll a/b protein acts as a torque aligning chloroplasts in a magnetic field

Displacement of particles from the purified light-harvesting chlorophyll a/b protein aggregate (LHC) was studied in magnetic fields of various strengths (0 to 1.6 T) by polarized fluorescence measurements. Macromolecular aggregates of LHC have a considerable magnetic susceptibility which enables the particles to rotate and align with their nematic axes parallel with H. As LHC is embedded in a transmembrane direction thylakoids should align perpendicular to H, the mode of alignment experimentally observed in thylakoids. The value of the magnetic susceptibility could be estimated by relating it to the integral susceptibility of the chlorophyll molecules in LHC. The fitting of this value with the field strength dependency of the fluorescence polarization ratio (FP) revealed a relationship between the LHC content of various photosynthetic membranes and their capacity for alignment, which suggested that LHC might be the torque ordering chloroplasts in a magnetic field.Abbreviations LHC light-harvesting chlorophyll a/b protein - FP fluorescence polarization ratio, Iz/Iy     

The state of detergent solubilised light-harvesting chlorophyll-a/b protein complex as monitored by picosecond time-resolved fluorescence and circular dichroism

Steady-state and picosecond time-resolved fluorescence techniques in conjunction with circular dichroism have been used to study the light-harvesting chlorophyll-a/b protein complex (LHC) isolated from pea chloroplasts. In particular, the effect of changing the detergent / chlorophyll ratio on the state of the LHC has been investigated. Our results have been interpreted in light of the known protein geometry of the LHC in 2-dimensional crystals (Kühlbrandt, W. (1984) Nature 307, 478–479). The fluorescence lifetime data reveals 1 / e-lifetimes of 3.53 (±0.04) ns and 1.10 (±0.01) ns for a stable, efficiently energy-transferring state of the LHC. Subnanosecond lifetimes are observed under conditions leading to aggregation, while a long component of 5.50 (±0.16) ns corresponding to free Chl a is found when the detergent / chlorophyll ratio is high. The circular dichroism shows a major Chl-b exciton, a Chl-a / b exciton and a further ‘quenching’ Chl-b exciton. These have been attributed to: a C₃ symmetric Chl-b interaction for which the intact C₃ protein trimer geometry is a prerequisite; a dimeric Chl-a / b interaction, the presence of which is critically dependent on the detergent type; and a further Chl-b interaction which arises from the presence of aggregated trimers, respectively. We have found that the degree of heterogeneity with respect to the oligomeric state of the pigment-protein trimers is dependent upon the detergent / chlorophyll ratio used. Low detergent / chlorophyll ratios result in extensive aggregation of the trimers with a geometry similar to that found in 2-dimensional crystals of the LHC. Moderate detergent conditions yield predominantly non-aggregated trimers. Excess detergent conditions result in considerable chromophore heterogeneity and loss of the main Chl-b exciton consistent with protein denaturation through an initial break up of the trimer geometry. From these results we believe that in vitro the minimum stable functional unit corresponds to a C₃ symmetric protein trimer.     

Fluorescence lifetime heterogeneity in aggregates of LHCII revealed by time-resolved microscopy.

Two-photon excitation, time-resolved fluorescence microscopy was used to investigate the fluorescence quenching mechanisms in aggregates of light-harvesting chlorophyll a/b pigment protein complexes of photosystem II from green plants (LHCII). Time-gated microscopy images show the presence of large heterogeneity in fluorescence lifetimes not only for different LHCII aggregates, but also within a single aggregate. Thus, the fluorescence decay traces obtained from macroscopic measurements reflect an average over a large distribution of local fluorescence kinetics. This opens the possibility to resolve spatially different structural/functional units in chloroplasts and other heterogeneous photosynthetic systems in vivo, and gives the opportunity to investigate individually the excited states dynamics of each unit. We show that the lifetime distribution is sensitive to the concentration of quenchers contained in the system. Triplets, which are generated at high pulse repetition rates of excitation (>1 MHz), preferentially quench domains with initially shorter fluorescence lifetimes. This proves our previous prediction from singlet-singlet annihilation investigations (Barzda, V., V. Gulbinas, R. Kananavicius, V. Cervinskas, H. van Amerongen, R. van Grondelle, and L. Valkunas. 2001. Biophys. J. 80:2409-2421) that shorter fluorescence lifetimes originate from larger domains in LHCII aggregates. We found that singlet-singlet annihilation has a strong effect in time-resolved fluorescence microscopy of connective systems and has to be taken into consideration. Despite that, clear differences in fluorescence decays can be detected that can also qualitatively be understood.     

Chlorophyll fluorescence changes at high temperatures induced by linear heating of greening barley leaves

A relative decrease of the high temperature part (above 60°C) of the chlorophyll fluorescence temperature curve during 3 h to 10 h greening period of barley (Hordeum vulgare L.) leaves was found to be concomitant to a decrease of Chl alb ratio and to a gradual increase of LHCP/core ratio found by electrophoresis and the ratio of granal to total length of thylakoid membranes. It is suggested that the high temperature part of the fluorescence temperature curve depends inversely on the relative amount of LHC II in thylakoid membranes.Abbreviations Chl a(b) chlorophyll a(b) - CPa chlorophyll a protein complex of PS II - CP1 P700 chlorophyll a protein complex of PS I - FP free pigments - FTC fluorescence temperature curve - F(T30) fluorescence intensity at 30°C - LHC II light harvesting complex II - LHCP light harvesting chlorophyll protein - LHCP3 (LHCPm) monomeric form of LHC II - LHCPo oligomeric form of LHC II complex - M1 first maximum of FTC - M2 second maximum (region) of FTC - PAA polyacrylamide - PAR photosynthetically active radiation - PS I(II) Photosystem I(II) - SDS-PAGE sodium dodecyl sulfate polyacrylamide gel electrophoresis     

Expression of ELIPs and PS II-S protein in spinach during acclimative reduction of the Photosystem II antenna in response to increased light intensities

The PS II-S protein and the so-called early light-inducible proteins (ELIPs) are homologous to the chlorophyll a/b-binding (Cab) gene products functioning in light-harvesting. The functional significance of these two CAB homologues is not known although they have been considered to bind pigments and in the case of the PS II–S protein this has been experimentally supported. The role of these two proteins does not appear to be light-harvesting but instead they are suggested to play a role as quenchers of free chlorophyll molecules during biogenesis and/or degradation of pigment-binding proteins. Such a role would be essential to eliminate the toxic and damaging effects that can be induced by free chlorophyll in the light. To this end the expression and characteristics of the ELIPs and the PS II–S protein were investigated in spinach leaves acclimating from low to high light intensities. Under these conditions there is a reduction in the antenna size of Photosystem II due to proteolytic digestion of its major chlorophyll a/b-binding protein (LHC II). During this acclimative proteolysis, up to one third of LHC II can be degraded and consequently substantial amounts of chlorophyll molecules will lose their binding sites. Our results reveal that there is a close correlation between ELIP accumulation and the onset of the LHC II degradation as low light-grown spinach leaves are subjected to increased light intensities. In contrast, there was no change in the relative level of the PS II–S protein during the acclimation process. It is concluded that the role for the ELIPs may be related to binding of liberated chlorophyll molecules and quenching of the toxic effects during LHC II degradation. In addition it was shown that in spinach four different ELIP species can be expressed and that they show different accumulation patterns in response to increased light intensities.     

Modification of excitation energy distribution to photosystem I by protein phosphorylation and cation depletion during thylakoid biogenesis in wheat

The effects of protein phosphorylation and cation depletion on the electron transport rate and fluorescence emission characteristics of photosystem I at two stages of chloroplast development in light-grown wheat leaves are examined. The light-harvesting chlorophyll a/b protein complex associated with photosystem I (LHC I) was absent from the thylakoids at the early stage of development, but that associated with photosystem II (LHC II) was present. Protein phosphorylation produced an increase in the light-limited rate of photosystem I electron transport at the early stage of development when chlorophyll b was preferentially excited, indicating that LHC I is not required for transfer of excitation energy from phosphorylated LHC II to the core complex of photosystem I. However, no enhancement of photosystem I fluorescence at 77 K was observed at this stage of development, demonstrating that a strict relationship between excitation energy density in photosystem I pigment matrices and the long-wavelength fluorescence emission from photosystem I at 77 K does not exist. Depletion of Mg²⁺ from the thylakoids produced a stimulation of photosystem I electron transport at both stages of development, but a large enhancement of the photosystem I fluorescence emission was observed only in the thylakoids containing LHC I. It is suggested that the enhancement of PS I electron transport by Mg²⁺-depletion and phosphorylation of LHC II is associated with an enhancement of fluorescence at 77 K from LHC I and not from the core complex of PS I.     

Light-induced fluorescence quenching in the light-harvesting chlorophyll a/b protein complex

Summary Irradiation of the principal photosystem II light-harvesting chlorophyll-protein antenna complex, LHC II, with high light intensities brings about a pronounced quenching of the chlorophyll fluorescence. Illumination of isolated thylakoids with high light intensities generates the formation of quenching centres within LHC II in vivo, as demonstrated by fluorescence excitation spectroscopy. In the isolated complex it is demonstrated that the light-induced fluorescence quenching: a) shows a partial, biphasic reversibility in the dark; b) is approximately proportional to the light intensity; c) is almost independent of temperature in the range 0–30°C; d) is substantially insensitive to protein modifying reagents and treatments; e) occurs in the absence of oxygen. A possible physiological importance of the phenomenon is discussed in terms of a mechanism capable of dissipating excess excitation energy within the photosystem II antenna.Abbreviations chla chlorophyll a - chlb chlorophyll b - F₀ fluorescence yield with reaction centers open - F_m fluorescence yield with reaction centres closed - F_i fluorescence at the plateau level of the fast induction phase - LHC II light-harvesting chlorophyll a/b protein complex II - PS II photosystem II - PSI photosystem I - Tricine N-[2-hydroxy-1,1-bis(hydroxymethyl)ethyl]glycine     

Functional domain size in aggregates of light-harvesting complex II and thylakoid membranes

The functional domain size for efficient excited singlet state quenching was studied in artificial aggregates of the main light-harvesting complex II (LHCIIb) from spinach and in native thylakoid membranes by picosecond time-resolved fluorescence spectroscopy and quantum yield measurements. The domain size was estimated from the efficiency of added exogenous singlet excitation quenchers-phenyl-p-benzoquinone (PPQ) and dinitrobenzene (DNB). The mean fluorescence lifetimes τ(av) were quantified for a range of quencher concentrations. Applying the Stern-Volmer formalism, apparent quenching rate constants k(q) were determined from the dependencies on quencher concentration of the ratio τ(0)(av)/τ(av), where τ(0)(av) is the average fluorescence lifetime of the sample without addition of an exogenous quencher. The functional domain size was gathered from the ratio k(q)'/k(q), i.e., the apparent quenching rate constants determined in aggregates (or membranes), k(q)', and in detergent-solubilised LHCII trimers, k(q), respectively. In LHCII macroaggregates, the resulting values for the domain size were 15-30 LHCII trimers. In native thylakoid membranes the domain size was equivalent to 12-24 LHCII trimers, corresponding to 500-1000 chlorophylls. Virtually the same results were obtained when membranes were suspended in buffers promoting either membrane stacking or destacking. These domain sizes are orders of magnitude smaller than the number of physically connected pigment-protein complexes. Therefore our results imply that the physical size of an antenna system beyond the numbers of a functional domain size has little or no effect on improving the light-harvesting efficiency.     

Characterization and isolation of intermediates in beta-lactoglobulin heat aggregation at high pH

The early stages of heat induced aggregation at 67.5 degrees C of beta-lactoglobulin were studied by combined static light scattering and size exclusion chromatography. At all conditions studied (pH 8.7 without salt and pH 6.7 with or without 60 mM NaCl) we observe metastable heat-modified dimers, trimers, and tetramers. These oligomers reach a maximum in concentration at about the time when large aggregates (1000-4000 kg/mol) appear, after which they decline in concentration. By isolating the oligomers it was demonstrated that they rapidly form aggregates upon heating in the absence of monomeric protein, showing that these species are central to the aggregation process. To our knowledge this is the first time that intermediates in protein aggregation have been isolated. At all stages of aggregation the dominant oligomer was the heat-modified dimer. Whereas the heat-modified oligomers are formed at a higher rate at pH 8.7 than at pH 6.7, the opposite is the case for the formation of aggregates from the metastable oligomers indicating cross-linking via disulfide bridges for the oligomers and noncovalent interaction in the formation of the aggregates. The data suggest that an aggregate nucleus is formed from four oligomers. For protein concentrations of 10 or 20 g/l a heat-modified monomer can be observed until about the time when the maximum in concentration appears of the heat-modified dimer. The disappearance of this heat-modified monomer correlates to the formation of dimers (trimers and tetramers).     

Aggregation and fluorescence quenching of chlorophyll a of the light-harvesting complex II from spinach in vitro

The salt-induced aggregation of the light-harvesting complex (LHC) II isolated from spinach and its correlation with fluorescence quenching of chlorophyll a is reported. Two transitions with distinctly different properties were observed. One transition related to salt-induced fluorescence quenching takes place at low salt concentration and is dependent both on temperature and detergent concentration. This transition seems to be related to a change in the lateral microorganization of LHCII. The second transition occurs at higher salt concentration and involves aggregation. It is independent of temperature and of detergent at sub-cmc concentrations. During the latter transition the small LHCII sheets (approximately 100 nm in diameter) are stacked to form larger aggregates of approximately 3 microm diameter. Based on the comparison between the physical properties of the transition and theoretical models, direct and specific binding of cations can practically be ruled out as driving force for the aggregation. It seems that in vitro aggregation of LHCII is caused by a complex mixture of different effects such as dielectric and electrostatic properties of the solution and surface charges.     

Lateral mobility of the light-harvesting complex in chloroplast membranes controls excitation energy distribution in higher plants

Chloroplast thylakoid protein phosphorylation produces changes in light-harvesting properties and in membrane structure as revealed by freeze-fracture electron microscopy. Protein phosphorylation resulted in an increase in the 77 °K fluorescence signal at 735 nm relative to that at 685 nm. In addition, a decrease in connectivity between Photosystem II centers (PS II) and a dynamic quenching of the room temperature variable fluorescence was observed upon phosphorylation. Accompanying these fluorescence changes was a 23% decrease in the amount of stacked membranes. Microscopic analyses indicated that 8.0-nm particles fracturing on the P-face moved from the stacked into the unstacked regions upon phosphorylation. The movement of the 8.0-nm particles was accompanied by the appearance of chlorophyll b and 25 to 29 kD polypeptides in isolated stroma lamellae fractions. We conclude that phosphorylation of a population of the light-harvesting chlorophyll $\text{a}\text{b}$ protein complexes (LHC) in grana partitions causes the migration of these pigment proteins from the PS II-rich appressed membranes into the Photosystem I (PS I) enriched unstacked regions. This increases the absorptive cross section of PS I. In addition, we suggest that the mobile population of LHC functions to interconnect PS II centers in grana partitions; removal of this population of LHC upon phosphorylation limits PS II → PS II energy transfer and thereby favors spillover of energy from PS II to PS I.     

Changes in lipid composition of Photosystem 1 particles from thylakoids phosphorylated under reductive or anaerobic conditions

Changes in lipid composition of Photosystem 1 (PS 1) particles isolated from thylakoids phosphorylated under reductive or anaerobic conditions have been studied. Under reductive conditions, there was an increase in monogalactosyldiacylglycerol containing highly saturated fatty acids and phosphatidylglycerol containing transhexadecenoic fatty acid. Under anaerobic conditions, the amount of all lipid classes was increased. As we have shown earlier (S. V. Manuilskaya, O. I. Volovik, A. I. Mikhno, A. I. Polischuk and S. M. Kochubey (1990) Photosynthetica 24: 419–423) these changes were due to a co-migration of some lipid species and light-harvesting chlorophyll a/b complex LHC II from PS 2 to PS 1. These data allow us to conclude that LHC II consists of the lipoproteins containing specific lipids. Different composition of lipids co-migrating with LHC II under various conditions of phosphorylation might be caused by the variety of LHC II subpopulations transferred under each reductive condition.Abbreviations PS 1 Photosystem 1 - PS 2 Photosystem 2 - LHC II light-harvesting chlorophyll a/b protein complex II - Chl chlorophyll - MGDG monogalactosyldiacylglycerol - DGDG digalactosyldiacylglycerol - PG phosphatidylglycerol - SQDG sulfoquinovosyldiacylglycerol     

High Yield Non-detergent Isolation of Photosystem I-Light-harvesting Chlorophyll II Membranes from Spinach Thylakoids: IMPLICATIONS FOR THE ORGANIZATION OF THE PS I ANTENNAE IN HIGHER PLANTS*

Styrene-maleic acid copolymer was used to effect a non-detergent partial solubilization of thylakoids from spinach. A high density membrane fraction, which was not solubilized by the copolymer, was isolated and was highly enriched in the Photosystem (PS) I-light-harvesting chlorophyll (LHC) II supercomplex and depleted of PS II, the cytochrome b₆/f complex, and ATP synthase. The LHC II associated with the supercomplex appeared to be energetically coupled to PS I based on 77 K fluorescence, P₇₀₀ photooxidation, and PS I electron transport light saturation experiments. The chlorophyll (Chl) a/b ratio of the PS I-LHC II membranes was 3.2 ± 0.9, indicating that on average, three LHC II trimers may associate with each PS I. The implication of these findings within the context of higher plant PS I antenna organization is discussed.