Acclimation to temperature and irradiance modulates PSII charge recombination

Acclimation of wild type and the chlorina F2 mutant of barley to either high light or low temperature results in a 2- to 3-fold increase in non-photochemical quenching which occurred independently of either energy-dependent quenching (qE), xanthophyll cycle-mediated antenna quenching or state transitions. Results of in vivo thermoluminescence measurements used to address this conundrum indicated that excitation pressure regulates the temperature gap for S(2)Q(B)(-) and S(2)Q(A)(-) charge recombinations within photosystem II reaction centers. This is discussed in terms of photoprotection through non-radiative charge recombination.     

Monomeric light harvesting complexes enhance excitation energy transfer from LHCII to PSII and control their lateral spacing in thylakoids

Proper assembly of plant photosystem II, in the appressed region of thylakoids, allows for both efficient light harvesting and the dissipation of excitation energy absorbed in excess. The core moiety of wild type supercomplex is associated with monomeric antennae that, in turn, bind peripheral trimeric LHCII complexes. Acclimation to light environment dynamics involves structural plasticity within PSII-LHCs supercomplexes, including depletion in LHCII and CP24. Here, we report on the acclimation of NoM, an Arabidopsis mutant lacking monomeric LHCs but retaining LHCII trimer. Lack of monomeric LHCs impaired the operation of both photosynthetic electron transport and state transitions, despite the fact that NoM underwent a compensatory over-accumulation of the LHCII complement compared to the wild type. Mutant plants displayed stunted growth compared to the wild type when probed over a range of light conditions. When exposed to short-term excess light, NoM showed higher photosensitivity and enhanced singlet oxygen release than the wild type, whereas long-term acclimation under stress conditions was unaffected. Analysis of pigment-binding supercomplexes showed that the absence of monomeric LHCs did affect the macro-organisation of photosystems: large PSI-LHCII megacomplexes were more abundant in NoM, whereas the assembly of PSII-LHCs supercomplexes was impaired. Observation by electron microscopy (EM) and image analysis of thylakoids highlighted impaired granal stacking and membrane organisation, with a heterogeneous distribution of PSII and LHCII compared to the wild type. It is concluded that monomeric LHCs are critical for the structural and functional optimisation of the photosynthetic apparatus.     

Protein oligomerization modulates raft partitioning and apical sorting of GPI-anchored proteins

An essential but insufficient step for apical sorting of glycosylphosphatidylinositol (GPI)-anchored proteins (GPI-APs) in epithelial cells is their association with detergent-resistant microdomains (DRMs) or rafts. In this paper, we show that in MDCK cells both apical and basolateral GPI-APs associate with DRMs during their biosynthesis. However, only apical and not basolateral GPI-APs are able to oligomerize into high molecular weight complexes. Protein oligomerization begins in the medial Golgi, concomitantly with DRM association, and is dependent on protein-protein interactions. Impairment of oligomerization leads to protein missorting. We propose that oligomerization stabilizes GPI-APs into rafts and that this additional step is required for apical sorting of GPI-APs. Two alternative apical sorting models are presented.     

Investigation of the molecular mechanism of the blue-light-specific excitation energy quenching in the plant antenna complex LHCII

Excitation of the major photosynthetic antenna complex of plants, LHCII, with blue light (470 nm) provides an advantage to plants, as it gives rise to chlorophyll a fluorescence lifetimes shorter than with excitation with red light (635 nm). This difference is particularly pronounced in fluorescence emission wavelengths longer than 715 nm. Illumination of LHCII preparation with blue light additionally induces fluorescence quenching, which develops on a minute timescale. This effect is much less efficient when induced by red light, despite the equalized energy absorbed in both the spectral regions. Simultaneous analysis of the fluorescence and photoacoustic signals in LHCII demonstrated that the light-driven fluorescence quenching is not associated with an increase in heat emission. Instead, a reversible light-induced conformational transformation of the protein takes place, as demonstrated by the FTIR technique. These findings are discussed in terms of the blue-light-specific excitation energy quenching in LHCII, which may have photoprotective applications.     

Effects of blue light deficiency on acclimation of light energy partitioning in PSII and CO2 assimilation capacity to high irradiance in spinach leaves

Blue light effects on the acclimation of energy partitioningcharacteristics in PSII and CO₂ assimilation capacity in spinachto high growth irradiance were investigated. Plants were grownhydroponically in different light treatments that were a combinationof two light qualities and two irradiances, i.e. white lightand blue-deficient light at photosynthetic photon flux densities(PPFDs) of 100 and 500 µmol m^–2 s^–1. The CO₂assimilation rate, the quantum efficiency of PSII (PSII) andthermal dissipation activity / in young, fully expanded leaves were measured under 1,600 µmol m^–2 s^–1white light. The CO₂ assimilation rate and PSII were higher,while / was lower in plants grown under high irradiancethan in plants grown under low irradiance. These responses wereobserved irrespective of the presence or absence of blue lightduring growth. The extent of the increase in the CO₂ assimilationrate and PSII and the decrease in / by high growth irradiance was smaller under blue light-deficient conditions. These resultsindicate that blue light helps to boost the acclimation responsesof energy partitioning in PSII and CO₂ assimilation to highirradiance. Similarly, leaf N, Cyt f and Chl contents per unitleaf area increased by high growth irradiance, and the extentof the increment in leaf N, Cyt f and Chl was smaller underblue light-deficient conditions. Regression analysis showedthat the differences in energy partitioning in PSII and CO₂assimilation between plants grown under high white light andhigh blue-deficient light were closely related to the differencein leaf N.     

Comparison of cytoplasmic ribosomal proteins of gateway barley and its mutant

The proteins of the cytoplasmic ribosomes isolated from dry embryos of Gateway barley and its virescens mutant were compared by two-dimensional polyacrylamide gel electrophoresis (2D-PAGE). The monosomes of both the lines gave similar patterns with 60 basic proteins. Upon dissociation of the monosomes, for the mutant, the basic proteins of the large subunits migrated more slowly than those of the normal and lacked three proteins but had three additional spots. Also, the proteins of the small subunits differed. The mutant lacked three of the proteins present in the normal but had three additional spots. Therefore, the large and small subunits contained a total of 34 and 41 basic proteins, respectively, in both the lines. There were several spots with identical electrophoretic mobilities in the small and large subunits of these two lines.     

The medium reorganization energy for the charge transfer reactions in proteins

A low static dielectric permittivity of proteins causes the low reorganization energies for the charge transfer reactions inside them. This reorganization energy does not depend on the pre-existing intraprotein electric field. The charge transferred inside the protein interacts with its aqueous surroundings; for many globular proteins, the effect of this surroundings on the reorganization energy is comparable with the effect of reorganization of the protein itself while for the charge transfer in the middle of membrane the aqueous phase plays a minor role. Reorganization energy depends strongly on the system considered, and hence there is no sense to speak on the "protein reorganization energy" as some permanent characteristic parameter. We employed a simple algorithm for calculation of the medium reorganization energy using the numerical solution of the Poisson-Boltzmann equation. Namely, the reaction field energy was computed in two versions - all media having optical dielectric permittivity, and all the media with the static one; the difference of these two quantities gives the reorganization energy. We have calculated reorganization energies for electron transfer in cytochrome c, various ammine-ruthenated cytochromes c, azurin, ferredoxin, cytochrome c oxidase, complex of methylamine dehydrogenase with amicyanin, and for proton transfer in α-chymotrypsin. It is shown that calculation of the medium reorganization energy can be a useful tool in analysis of the mechanisms of the charge transfer reactions in proteins.     

Picosecond time-resolved fluorescence study of chlorophyll organisation and excitation energy distribution in chloroplasts from wild-type barley and a mutant lacking chlorophyll b.

Picosecond time-resolved fluorescence spectroscopy has been used to investigate the fluorescence emission from wild-type barley chloroplasts and from chloroplasts of the barley mutant, chlorina f-2, which lacks the light-harvesting chlorophyll a/b-protein complex. Cation-controlled regulation of the distribution of excitation energy was studied in isolated chloroplasts at the Fo and Fm levels. It was found that: (a) The fluorescence decay curves were distinctly non-exponential, even at low excitation intensities (less than 2 x 10(14) photons . cm(-2). (b) The fluorescence decay curves could, however, be described by a dual exponential decay law. The wild-type barley chloroplasts gave a short-lived fluorescence component of approximately 140 ps and a long-lived component of 600 ps (Fo) or 1300 ps (Fm) in the presence of Mg2+; in comparison, the mutant barley yielded a short-lived fluorescence component of approx. 50 ps and a long-lived component of 194 ps (Fo) and 424 ps (Fm). (c) The absence of the light-harvesting chlorophyll a/b-protein complex in the mutant results in a low fluorescence quantum yield which is unaffected by the cation composition of the medium. (d) The fluorescence yield changes seen in steady-state experiments on closing Photosystem II reaction centres (Fm/Fo) or on the addition of MgCl2 (+Mg2+/-Mg2+) were in overall agreement with those calculated from the time-resolved fluorescence measurements. The results suggest that the short-lived fluorescence component is partly attributable to the chlorophyll a antenna of Photosystem I, and, in part, to those light-harvesting-Photosystem II pigment combinations which are strongly coupled to the Photosystem I antenna chlorophyll. The long-lived fluorescence component can be ascribed to the light-harvesting-Photosystem II pigment combinations not coupled with the antenna of Photosystem I. In the case of the mutant, the two components appear to be the separate emissions from the Photosystem I and Photosystem II antenna chlorophylls.     

The recombination landscape in Arabidopsis thaliana F2 populations

Recombination during meiosis shapes the complement of alleles segregating in the progeny of hybrids, and has important consequences for phenotypic variation. We examined allele frequencies, as well as crossover (XO) locations and frequencies in over 7000 plants from 17 F(2) populations derived from crosses between 18 Arabidopsis thaliana accessions. We observed segregation distortion between parental alleles in over half of our populations. The potential causes of distortion include variation in seed dormancy and lethal epistatic interactions. Such a high occurrence of distortion was only detected here because of the large sample size of each population and the number of populations characterized. Most plants carry only one or two XOs per chromosome pair, and therefore inherit very large, non-recombined genomic fragments from each parent. Recombination frequencies vary between populations but consistently increase adjacent to the centromeres. Importantly, recombination rates do not correlate with whole-genome sequence differences between parental accessions, suggesting that sequence diversity within A. thaliana does not normally reach levels that are high enough to exert a major influence on the formation of XOs. A global knowledge of the patterns of recombination in F(2) populations is crucial to better understand the segregation of phenotypic traits in hybrids, in the laboratory or in the wild.     

Oligomerization and pigmentation dependent excitation energy transfer in fucoxanthin-chlorophyll proteins

The ultrafast caroteonid to chlorophyll a energy transfer dynamics of the isolated fucoxanthin-chlorophyll proteins FCPa and FCPb from the diatom Cyclotella meneghiniana was investigated in a comprehensive study using transient absorption in the visible and near infrared spectral region as well as static fluorescence spectroscopy. The altered oligomerization state of both antenna systems results in a more efficient energy transfer for FCPa, which is also reflected in the different chlorophyll a fluorescence quantum yields. We therefore assume an increased quenching in the higher oligomers of FCPb. The influence of the carotenoid composition was investigated using FCPa and FCPb samples grown under different light conditions and excitation wavelengths at the blue (500 nm) and red (550 nm) wings of the carotenoid absorption. The different light conditions yield in altered amounts of the xanthophyll cycle pigments diadinoxanthin and diatoxanthin. Since no significant dynamic changes are observed for high light and low light samples, the contribution of the xanthophyll cycle pigments to the energy transfer is most likely negligible. On the contrary, the observed dynamics change drastically for the different excitation wavelengths. The analyses of the decay associated spectra of FCPb suggest an altered energy transfer pathway. For FCPa even an additional time constant was found after excitation at 500 nm. It is assigned to the intrinsic lifetime of either the xanthophyll cycle carotenoids or more probable the blue absorbing fucoxanthins. Based on our studies we propose a detailed model explaining the different excitation energy transfer pathways in FCPa.     

Differential temperature effects on dissipation of excess light energy and energy partitioning in lut2 mutant of Arabidopsis thaliana under photoinhibitory conditions

Photosynthesis Research - The high-light-induced alterations in photosynthetic performance of photosystem II (PSII) and photosystem I (PSI) as well as effectiveness of dissipation of excessive...     

Role of membrane organization in the Mg+2-mediated regulation of excitation energy transfer in barley chloroplasts

Photosystem II fluorescence of barley chloroplasts has been monitored to understand the role of membrane organization in the cation mediated regulation of excitation energy transfer from photosystem II to photosystem I. Membrane organization has been perturbed by adding 60 mM benzyl alcohol which is known to increase the membrane fluidity and decrease its thickness. An addition of 60 mM benzyl alcohol increases the fluorescence at 683 nm (excitation at 436 mn) by 43% whereas 5 mM Mg⁺² increased the fluorescence by 38%. An addition of 5 mM Mg⁺² to benzyl alcohol treated chloroplasts resulted in only a small increase in the fluorescence (6.5%). Circular dichroic measurements showed that 5 mM Mg⁺² decreased the circular dichroic signals suggesting an alteration in the orientation of the chromophores. However, the effect was insignificant on the benzyl alcohol treated chloroplast membranes. Benzyl alcohol itself had large effect on the circular dichroic signals. Based on these results, it appears that a change in the orientation of photosystem I and photosystem II, rather than their segregation, is responsible for the cation-induced increase in the photosystem II fluorescence.     

The rate of charge recombination in Photosystem II

Loss by recombination of the charge separated state P(680+)Q(A-) limits the performance of Photosystem II (PS II) as a photochemical energy converter. Time constants reported in literature for this process are mostly either near 0.17 ms or near 1.4 ms. The shorter time is found in plant PS II when reduction of P(680+) by the secondary electron donor Tyrosine Z cannot occur because Y(Z) is already oxidized. The 1.4 ms recombination is seen in Y(Z)-less mutants of the cyanobacterium Synechocystis. However, the rate of P(680+)Q(A-) recombination that actually competes with the stabilization of the charge separation has not been previously reported. We have measured the kinetics of the flash-induced fluorescence yield changes in the microsecond time domain in Tris-washed spinach chloroplasts. In this way the kinetics and yield of P(680+) reduction by Y(Z) were obtained, and the rate of the competing P(680+)Q(A-) recombination could be evaluated. The recombination time was less than 0.5 ms; the best-fitting time constant was 0.1 ms. The presence of Y(Z)(ox) slightly decreased the efficiency of excitation trapping but did not seem to accelerate P(680+)Q(A-) recombination. The two P(680+)Q(A-) lifetimes in the literature probably reflect a significant difference between plant and cyanobacterial PS II.     

The rate of charge recombination in Photosystem II

Loss by recombination of the charge separated state P₆₈₀⁺Q_A⁻ limits the performance of Photosystem II (PS II) as a photochemical energy converter. Time constants reported in literature for this process are mostly either near 0.17 ms or near 1.4 ms. The shorter time is found in plant PS II when reduction of P₆₈₀⁺ by the secondary electron donor Tyrosine Z cannot occur because Y_Z is already oxidized. The 1.4 ms recombination is seen in Y_Z-less mutants of the cyanobacterium Synechocystis. However, the rate of P₆₈₀⁺Q_A⁻ recombination that actually competes with the stabilization of the charge separation has not been previously reported. We have measured the kinetics of the flash-induced fluorescence yield changes in the microsecond time domain in Tris-washed spinach chloroplasts. In this way the kinetics and yield of P₆₈₀⁺ reduction by Y_Z were obtained, and the rate of the competing P₆₈₀⁺Q_A⁻ recombination could be evaluated. The recombination time was less than 0.5 ms; the best-fitting time constant was 0.1 ms. The presence of Y_Z^ox slightly decreased the efficiency of excitation trapping but did not seem to accelerate P₆₈₀⁺Q_A⁻ recombination. The two P₆₈₀⁺Q_A⁻ lifetimes in the literature probably reflect a significant difference between plant and cyanobacterial PS II.     

Resolution of Holliday junction recombination intermediates by wild-type and mutant IntDOT proteins

CTnDOT encodes an integrase that is a member of the tyrosine recombinase family. The recombination reaction proceeds by sequential sets of genetic exchanges between the attDOT site in CTnDOT and an attB site in the chromosome. The exchanges are separated by 7 base pairs in each site. Unlike most tyrosine recombinases, IntDOT exchanges sites that contain different DNA sequences between the exchange sites to generate Holliday junctions (HJs) that contain mismatched bases. We demonstrate that IntDOT resolves synthetic HJs in vitro. Holliday junctions that contain identical sequences between the exchange sites are resolved into both substrates and products, while HJs that contain mismatches are resolved only to substrates. This result implies that resolution of HJs to products requires the formation of a higher-order nucleoprotein complex with natural sites containing IntDOT. We also found that proteins with substitutions of residues (V95, K94, and K96) in a putative alpha helix at the junction of the N and CB domains (coupler region) were defective in resolving HJs. Mutational analysis of charged residues in the coupler and the N terminus of the protein did not provide evidence for a charge interaction between the regions of the protein. V95 may participate in a hydrophobic interaction with another region of IntDOT.     

Purification and characterization of SopA and SopB proteins essential for F plasmid partitioning

Mini-F plasmid has the trans-acting genes sopA and sopB and the cis-acting site sopC which are essential for accurate partitioning of plasmid DNA molecules into both daughter cells. In this study, we purified independently SopA and SopB proteins, analyzed the in vitro DNA-binding activity of these proteins by the gel retardation assay, and determined the precise binding sites of DNA by the footprinting method. SopA binds to four repeated sequences (CTTTGC) located in the promoter-operator region of the sopAB operon. The SopA binding activity is enhanced by the addition of SopB protein. SopB protein itself does not bind to this DNA region. These results suggest that the complex of SopA and SopB proteins autoregulate the expression of the sopA-sopB operon. On the other hand, SopB protein binds to the sopC region, in which 12 direct repeats of 43-base pairs nucleotides exist. SopB protein recognizes the inverted repeats of 7 base pairs in each direct repeats. SopA protein does not affect the SopB binding activity to the sopC DNA segment.