Site Energies of Active and Inactive Pheophytins in the Reaction Center of Photosystem II from Chlamydomonas Reinhardtii

31 Pags. The definitive version is available at: http://pubs.acs.org/journal/jpcbfkIt is widely accepted that the primary electron acceptor in various Photosystem II (PSII) reaction centers (RCs) is pheophytin a (Pheo a) within the D1 protein (PheoD1), while PheoD2 (within the D2 protein) is photochemically inactive. The Pheo site energies, however, have remained elusive, due to inherent spectral congestion. While most researchers over the last two decades assigned the Qy-states of PheoD1 and PheoD2 bands near 678–684 nm and 668–672 nm, respectively, recent modeling [Raszewski et al. Biophys. J. 2005, 88, 986–998; Cox et al. J. Phys. Chem. B 2009, 113, 12364–12374] of the electronic structure of the PSII RC reversed the location of the active and inactive Pheos, suggesting that the mean site energy of PheoD1 is near 672 nm, whereas PheoD2 (~677.5 nm) and ChlD1 (~680 nm) have the lowest energies (i.e., the PheoD2-dominated exciton is the lowest excited state). In contrast, chemical pigment exchange experiments on isolated RCs suggested that both pheophytins have their Qy absorption maxima at 676–680 nm [Germano et al. Biochem. 2001, 40, 11472–11482; Germano et al. Biophys. J. 2004, 86, 1664–1672]. To provide more insight into the site energies of both PheoD1 and PheoD2 (including the corresponding Qx transitions, which are often claimed to be degenerate at 543 nm) and to attest that the above two assignments are most likely incorrect, we studied a large number of isolated RC preparations from spinach and wild-type Chlamydomonas reinhardtii (at different levels of intactness) as well as the Chlamydomonas reinhardtii mutant (D2-L209H), in which the active branch PheoD1 is genetically replaced with chlorophyll a (Chl a). We show that the Qx-/Qy-region site-energies of PheoD1 and PheoD2 are ~545/680 nm and ~541.5/670 nm, respectively, in good agreement with our previous assignment [Jankowiak et al. J. Phys. Chem. B 2002, 106, 8803–8814]. The latter values should be used to model excitonic structure and excitation energy transfer dynamics of the PSII RCs.Partial support to B.N. (involved in calculations) was provided by the NSF EPSCoR Grant. V.Z. (involved in writing the manuscript) acknowledges support by NSERC. R.T.S., R.P., and M.S. were involved in the design and preparation of D2-mutant and RCs. They acknowledge support from USDOE, Photosynthetic Antennae Research Center (R.T.S.), MICIN (Grant AGL2008-00377) in Spain (R.P.), and the U.S. Department of Energy’s Photosynthetic Systems Program within the Chemical Sciences, Geosciences, and Biosciences Division of the Office of Basic Energy Sciences under NREL Contract #DE-AC36-08-GO28308 (M.S.).Peer reviewe

Combination of convalescent plasma therapy and repurposed drugs to treat severe COVID-19 patient with multimorbidity.

Combination of convalescent plasma therapy and repurposed drugs such as dexamethasone and remdesivir could be beneficial for severe COVID-19 patients with obesity and chronic diseases such as diabetes and hypertension

Burden of injuries in Nepal, 1990–2017: Findings from the Global Burden of Disease Study 2017

Background: Nepal is a low-income country undergoing rapid political, economic and social development. To date, there has been little evidence published on the burden of injuries during this period of transition.Methods: The Global Burden of Disease Study (GBD) is a comprehensive measurement of population health outcomes in terms of morbidity and mortality. We analysed the GBD 2017 estimates for deaths, years of life lost, years lived with disability, incidence and disability-adjusted life years (DALYs) from injuries to ascertain the burden of injuries in Nepal from 1990 to 2017.Results: There were 16 831 (95% uncertainty interval 13 323 to 20 579) deaths caused by injuries (9.21% of all-cause deaths (7.45% to 11.25%)) in 2017 while the proportion of deaths from injuries was 6.31% in 1990. Overall, the injury-specific age-standardised mortality rate declined from 88.91 (71.54 to 105.31) per 100 000 in 1990 to 70.25 (56.75 to 85.11) per 100 000 in 2017. In 2017, 4.11% (2.47% to 6.10%) of all deaths in Nepal were attributed to transport injuries, 3.54% (2.86% to 4.08%) were attributed to unintentional injuries and 1.55% (1.16% to 1.85%) were attributed to self-harm and interpersonal violence. From 1990 to 2017, road injuries, falls and self-harm all rose in rank for all causes of death.Conclusions: The increase in injury-related deaths and DALYs in Nepal between 1990 and 2017 indicates the need for further research and prevention interventions. Injuries remain an important public health burden in Nepal with the magnitude and trend of burden varying over time by cause-specific, sex and age group. Findings from this study may be used by the federal, provincial and local governments in Nepal to prioritise injury prevention as a public health agenda and as evidence for country-specific interventions

Variation in grain zinc and iron concentrations, grain yield and associated traits of biofortified bread wheat genotypes in Nepal

Wheat (Triticum aestivum L.) is one of the major staples in Nepal providing the bulk of food calories and at least 30% of Fe and Zn intake and 20% of dietary energy and protein consumption; thus, it is essential to improve its nutritional quality. To select high-yielding genotypes with elevated grain zinc and iron concentration, the sixth, seventh, eighth, and ninth HarvestPlus Yield Trials (HPYTs) were conducted across diverse locations in Nepal for four consecutive years: 2015–16, 2016–17, 2017–18, and 2018–19, using 47 biofortified and 3 non-biofortified CIMMYT-bred, bread wheat genotypes: Baj#1, Kachu#1, and WK1204 (local check). Genotypic and spatial variations were found in agro-morphological traits; grain yield and its components; and the grain zinc and iron concentration of tested genotypes. Grain zinc concentration was highest in Khumaltar and lowest in Kabre. Likewise, grain iron concentration was highest in Doti and lowest in Surkhet. Most of the biofortified genotypes were superior for grain yield and for grain zinc and iron concentration to the non-biofortified checks. Combined analyses across environments showed moderate to high heritability for both Zn (0.48–0.81) and Fe (0.46–0.79) except a low heritability for Fe observed for 7th HPYT (0.15). Grain yield was positively correlated with the number of tillers per m2, while negatively correlated with days to heading and maturity, grain iron, grain weight per spike, and thousand grain weight. The grain zinc and iron concentration were positively correlated, suggesting that the simultaneous improvement of both micronutrients is possible through wheat breeding. Extensive testing of CIMMYT derived high Zn wheat lines in Nepal led to the release of five biofortified wheat varieties in 2020 with superior yield, better disease resistance, and 30–40% increased grain Zn and adaptable to a range of wheat growing regions in the country – from the hotter lowland, or Terai, regions to the dry mid- and high-elevation areas

Excitation energy transfer and charge separation dynamics in photosystem II: hole-burning study

Doctor of PhilosophyDepartment of ChemistryRyszard J. JankowiakThe constituents of oxygen-evolving photosystem II core complexes—antenna proteins (CP43 and CP47) and reaction center (RC)—have been the subject of many studies over the years. However, the various issues related to electronic structure, including the origin/composition of the lowest-energy traps, origin of various emission bands, excitation energy transfer (EET), primary charge separation (CS) processes and pigment site energies remain yet to be fully resolved. Exploiting our state-of-the-art techniques such as low-T absorption, fluorescence, and hole burning (HB) spectroscopies, we resolved some of the issues particularly related to CP47 and isolated RC protein complexes. For example, we demonstrated that the fluorescence origin band maximum (~695 nm) originates from the lowest-energy state ~693 nm of intact CP47. In intact CP47 in contrast to destablished protein complexes, the band (~695 nm) does not shift in the temperature range of 5–77 K unless hole-burning takes place. We also studied a large number of isolated RC preparations from spinach, and wild-type Chlamydomonas reinhardtii (at different levels of intactness), as well as its mutant (D2-L209H), in which the active branch pheophytin (PheoD1) has been genetically replaced with chlorophyll a (Chl a). We showed that the Qx-/Qy-region site-energies of PheoD1 and PheoD2 are ~545/680 nm and ~541.5/670 nm, respectively, in good agreement with our previous assignment [Jankowiak et al. J. Phys. Chem. B 2002, 106, 8803]. Finally, we demonstrated that the primary electron donor in isolated algal RCs from C. reinhardtii (referred to as RC684) is PD1 and/or PD2 of the special Chl pair (analogous to PL and PM, the special BChl pair of the bacterial RC) and not ChlD1. However, the latter can also be the primary electron donor (minor pathway) in RC684 depending on the realization of the energetic disorder. We further demonstrate that transient HB spectra in RC684 are very similar to P+QA - PQA spectra measured in PSII core, providing the first evidence that RC684 represent intact isolated RC that also possesses the secondary electron acceptor, QA. In summary, a new insight into possible charge separation pathways in isolated PSII RCs has been provided

Site Energies of Active and Inactive Pheophytins in the Reaction Center of Photosystem II from Chlamydomonas Reinhardtii

31 Pags. The definitive version is available at: http://pubs.acs.org/journal/jpcbfkIt is widely accepted that the primary electron acceptor in various Photosystem II (PSII) reaction centers (RCs) is pheophytin a (Pheo a) within the D1 protein (PheoD1), while PheoD2 (within the D2 protein) is photochemically inactive. The Pheo site energies, however, have remained elusive, due to inherent spectral congestion. While most researchers over the last two decades assigned the Qy-states of PheoD1 and PheoD2 bands near 678–684 nm and 668–672 nm, respectively, recent modeling [Raszewski et al. Biophys. J. 2005, 88, 986–998; Cox et al. J. Phys. Chem. B 2009, 113, 12364–12374] of the electronic structure of the PSII RC reversed the location of the active and inactive Pheos, suggesting that the mean site energy of PheoD1 is near 672 nm, whereas PheoD2 (~677.5 nm) and ChlD1 (~680 nm) have the lowest energies (i.e., the PheoD2-dominated exciton is the lowest excited state). In contrast, chemical pigment exchange experiments on isolated RCs suggested that both pheophytins have their Qy absorption maxima at 676–680 nm [Germano et al. Biochem. 2001, 40, 11472–11482; Germano et al. Biophys. J. 2004, 86, 1664–1672]. To provide more insight into the site energies of both PheoD1 and PheoD2 (including the corresponding Qx transitions, which are often claimed to be degenerate at 543 nm) and to attest that the above two assignments are most likely incorrect, we studied a large number of isolated RC preparations from spinach and wild-type Chlamydomonas reinhardtii (at different levels of intactness) as well as the Chlamydomonas reinhardtii mutant (D2-L209H), in which the active branch PheoD1 is genetically replaced with chlorophyll a (Chl a). We show that the Qx-/Qy-region site-energies of PheoD1 and PheoD2 are ~545/680 nm and ~541.5/670 nm, respectively, in good agreement with our previous assignment [Jankowiak et al. J. Phys. Chem. B 2002, 106, 8803–8814]. The latter values should be used to model excitonic structure and excitation energy transfer dynamics of the PSII RCs.Partial support to B.N. (involved in calculations) was provided by the NSF EPSCoR Grant. V.Z. (involved in writing the manuscript) acknowledges support by NSERC. R.T.S., R.P., and M.S. were involved in the design and preparation of D2-mutant and RCs. They acknowledge support from USDOE, Photosynthetic Antennae Research Center (R.T.S.), MICIN (Grant AGL2008-00377) in Spain (R.P.), and the U.S. Department of Energy’s Photosynthetic Systems Program within the Chemical Sciences, Geosciences, and Biosciences Division of the Office of Basic Energy Sciences under NREL Contract #DE-AC36-08-GO28308 (M.S.).Peer reviewe

On stabilization of a neutral aromatic ligand by π–cation interactions in monoclonal antibodies

International audienceIt has been shown that anti-PAH mAb can bind a particular cross-reactant by adopting two distinct "red" and "blue" conformations of its binding sites [N.M. Grubor et al. PNAS 102, 2005, 7453-7458]. In the case of red conformation of pyrene (Py)/anti-PAH mAb (with a broad fluorescence (0,0)-band with fwhm ~140 cm(-1)), the central role in complex formation was played by π-π interactions. The nature of the blue-shifted conformation with very narrow fluorescence (0,0)-band (fwhm ~75 cm(-1)) was left unclear due to the lack of suitable data for comparison. In this work, we suggest spectroscopic and modeling results obtained for the blue conformation of Py in several mAb (including 4D5 mAb) are consistent with π-cation interactions, underscoring the importance of π-cation interaction in ligand binding and stabilization in agreement with earlier modeling studies [J-L. Pellequer, et al. J. Mol. Biol. 302, 2000, 691-699]. We propose considerable narrowing of the fluorescence origin band of ligand in the protein environment could be regarded as a simple indicator of π-cation interactions. Since 4D5 mAb forms only the blue-shifted conformation, while anti-PAH and 8E11 mAbs form both blue- and red-shifted conformations, we suggest mAb interactions, with Py molecules lacking H-bonding functionality, may induce distinct conformations of mAb binding sites that allow binding by π-π and/or π-cation interactions

Insight into the Electronic Structure of the CP47 Antenna Protein Complex of Photosystem II: Hole Burning and Fluorescence Study

16 Pag., 12 Fig.We report low temperature (T) optical spectra of the isolated CP47 antenna complex from Photosystem II (PSII) with a low-T fluorescence emission maximum near 695 nm and not, as previously reported, at 690−693 nm. The latter emission is suggested to result from three distinct bands: a lowest-state emission band near 695 nm (labeled F1) originating from the lowest-energy excitonic state A1 of intact complexes (located near 693 nm and characterized by very weak oscillator strength) as well as emission peaks near 691 nm (FT1) and 685 nm (FT2) originating from subpopulations of partly destabilized complexes. The observation of the F1 emission is in excellent agreement with the 695 nm emission observed in intact PSII cores and thylakoid membranes. We argue that the band near 684 nm previously observed in singlet-minus-triplet spectra originates from a subpopulation of partially destabilized complexes with lowest-energy traps located near 684 nm in absorption (referred to as AT2) giving rise to FT2 emission. It is demonstrated that varying contributions from the F1, FT1, and FT2 emission bands led to different maxima of fluorescence spectra reported in the literature. The fluorescence spectra are consistent with the zero-phonon hole action spectra obtained in absorption mode, the profiles of the nonresonantly burned holes as a function of fluence, as well as the fluorescence line-narrowed spectra obtained for the Qy band. The lowest Qy state in absorption band (A1) is characterized by an electron−phonon coupling with the Huang−Rhys factor S of 1 and an inhomogeneous width of 180 cm−1. The mean phonon frequency of the A1 band is 20 cm−1. In contrast to previous observations, intact isolated CP47 reveals negligible contribution from the triplet-bottleneck hole, i.e., the AT2 trap. It has been shown that Chls in intact CP47 are connected via efficient excitation energy transfer to the A1 trap near 693 nm and that the position of the fluorescence maximum depends on the burn fluence. That is, the 695 nm fluorescence maximum shifts blue with increasing fluence, in agreement with nonresonant hole burned spectra. The above findings provide important constraints and parameters for future excitonic calculations, which in turn should offer new insight into the excitonic structure and composition of low-energy absorption traps.This work was performed at K-State and was supported by a U.S. Department of Energy (US-DOE) EPSCoR grant (R.J.) (DE-FG02-08ER46504) and the supplements from the Office of Basic Energy Sciences (US-DOE) and the Kansas Technology Enterprise Corporation. Partial support was also provided by the Office of Science, US-DOE (M.S.; NREL Contract DE-AC36-08GO28308), and the PN I+D+I of Spain (R.P.; AGL2008-00377). V.Z. acknowledges support by NSERC Discovery Grant.Peer reviewe

Spectroscopic Study of the CP43′ Complex and the PSI–CP43′ Supercomplex of the Cyanobacterium Synechocystis PCC 6803

8 Pags. The definitive version, with Figs., is available at: http://pubs.acs.org/journal/jpcbfkThe PSI-CP43' supercomplex of the cyanobacterium Synechocystis PCC 6803, grown under iron-starvation conditions, consists of a trimeric core Photosystem I (PSI) complex and an outer ring of 18 CP43' light-harvesting complexes. We have investigated the electronic structure and excitation energy transfer (EET) pathways within the CP43' (also known as the isiA gene product) ring using low-temperature absorption, fluorescence, fluorescence excitation, and hole-burning (HB) spectroscopies. Analysis of the absorption spectra of PSI, CP43', and PSI-CP43' complexes suggests that there are 13 chlorophylls (Chls) per CP43' monomer, i.e., a number that was observed in the CP43 complex of Photosystem 11 (PSII) (Umena, Y. et al. Nature 2011, 473, 55-60). This is in contrast with the recent modeling studies of Zhang et al. (Biochim. Biophys. Acta 2010, 1797, 457-465), which suggested that IsiA likely contains 15 Chls. Modeling studies of various optical spectra of the CP43' ring using the uncorrelated EET model (Zazubovich, V.; Jankowiak, R J. Lumin. 2007, 127, 245-250) suggest that CP43' monomers (in analogy to the CP43 complexes of the PSII core) also possess two quasi-degenerate low-energy states, A' and B'. The site distribution functions of states A' and B' maxima/full width at half-maximum (fwhm) are at 684 nm/180 cm(-1) and 683 nm/80 cm(-1), respectively. Our analysis shows that pigments mostly contributing to the lowest-energy A' and B' states must be located on the side of the CP43' complex facing the PSI core, a finding that contradicts the model of Zhang et al. but is in agreement with the model suggested by Nield et al. (Biochemistry 2003, 42, 3180-3188). We demonstrate that the A'-A' and B'-B' EET between different monomers is possible, though with a slower rate than intramonomer A'-B' and/or B'-A' energy transfer.Peer reviewe

Spectroscopic Study of the CP43′ Complex and the PSI–CP43′ Supercomplex of the Cyanobacterium Synechocystis PCC 6803

8 Pags. The definitive version, with Figs., is available at: http://pubs.acs.org/journal/jpcbfkThe PSI-CP43' supercomplex of the cyanobacterium Synechocystis PCC 6803, grown under iron-starvation conditions, consists of a trimeric core Photosystem I (PSI) complex and an outer ring of 18 CP43' light-harvesting complexes. We have investigated the electronic structure and excitation energy transfer (EET) pathways within the CP43' (also known as the isiA gene product) ring using low-temperature absorption, fluorescence, fluorescence excitation, and hole-burning (HB) spectroscopies. Analysis of the absorption spectra of PSI, CP43', and PSI-CP43' complexes suggests that there are 13 chlorophylls (Chls) per CP43' monomer, i.e., a number that was observed in the CP43 complex of Photosystem 11 (PSII) (Umena, Y. et al. Nature 2011, 473, 55-60). This is in contrast with the recent modeling studies of Zhang et al. (Biochim. Biophys. Acta 2010, 1797, 457-465), which suggested that IsiA likely contains 15 Chls. Modeling studies of various optical spectra of the CP43' ring using the uncorrelated EET model (Zazubovich, V.; Jankowiak, R J. Lumin. 2007, 127, 245-250) suggest that CP43' monomers (in analogy to the CP43 complexes of the PSII core) also possess two quasi-degenerate low-energy states, A' and B'. The site distribution functions of states A' and B' maxima/full width at half-maximum (fwhm) are at 684 nm/180 cm(-1) and 683 nm/80 cm(-1), respectively. Our analysis shows that pigments mostly contributing to the lowest-energy A' and B' states must be located on the side of the CP43' complex facing the PSI core, a finding that contradicts the model of Zhang et al. but is in agreement with the model suggested by Nield et al. (Biochemistry 2003, 42, 3180-3188). We demonstrate that the A'-A' and B'-B' EET between different monomers is possible, though with a slower rate than intramonomer A'-B' and/or B'-A' energy transfer.Peer reviewe