22 research outputs found

    Star formation and AGN activity in the most luminous LINERs in the local universe

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    This work presents the properties of 42 objects in the group of the most luminous, highest star formation rate LINERs at z = 0.04 - 0.11. We obtained long-slit spectroscopy of the nuclear regions for all sources, and FIR data (Herschel and IRAS) for 13 of them. We measured emission line intensities, extinction, stellar populations, stellar masses, ages, AGN luminosities, and star-formation rates. We find considerable differences from other low-redshift LINERs, in terms of extinction, and general similarity to star forming (SF) galaxies. We confirm the existence of such luminous LINERs in the local universe, after being previously detected at z ~ 0.3 by Tommasin et al. (2012). The median stellar mass of these LINERs corresponds to 6 - 7 Ɨ\times 1010^{10}MāŠ™_{\odot} which was found in previous work to correspond to the peak of relative growth rate of stellar populations and therefore for the highest SFRs. Other LINERs although showing similar AGN luminosities have lower SFR. We find that most of these sources have LAGN ~ LSF suggesting co-evolution of black hole and stellar mass. In general among local LINERs being on the main-sequence of SF galaxies is related to their AGN luminosity.Comment: submitted to MNRA

    Light-Induced Changes within Photosystem II Protects Microcoleus sp. in Biological Desert Sand Crusts against Excess Light

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    The filamentous cyanobacterium Microcoleus vaginatus, a major primary producer in desert biological sand crusts, is exposed to frequent hydration (by early morning dew) followed by desiccation during potentially damaging excess light conditions. Nevertheless, its photosynthetic machinery is hardly affected by high light, unlike ā€œmodelā€ organisms whereby light-induced oxidative stress leads to photoinactivation of the oxygen-evolving photosystem II (PSII). Field experiments showed a dramatic decline in the fluorescence yield with rising light intensity in both drying and artificially maintained wet plots. Laboratory experiments showed that, contrary to ā€œmodelā€ organisms, photosynthesis persists in Microcoleus sp. even at light intensities 2ā€“3 times higher than required to saturate oxygen evolution. This is despite an extensive loss (85ā€“90%) of variable fluorescence and thermoluminescence, representing radiative PSII charge recombination that promotes the generation of damaging singlet oxygen. Light induced loss of variable fluorescence is not inhibited by the electron transfer inhibitors 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU), 2,5-dibromo-3-methyl-6-isopropylbenzoquinone (DBMIB), nor the uncoupler carbonyl cyanide-p-trifluoromethoxyphenylhydrazone (FCCP), thus indicating that reduction of plastoquinone or O2, or lumen acidification essential for non-photochemical quenching (NPQ) are not involved. The rate of QAāˆ’ re-oxidation in the presence of DCMU is enhanced with time and intensity of illumination. The difference in temperatures required for maximal thermoluminescence emissions from S2/QAāˆ’ (Q band, 22Ā°C) and S2,3/QBāˆ’ (B band, 25Ā°C) charge recombinations is considerably smaller in Microcoleus as compared to ā€œmodelā€ photosynthetic organisms, thus indicating a significant alteration of the S2/QAāˆ’ redox potential. We propose that enhancement of non-radiative charge recombination with rising light intensity may reduce harmful radiative recombination events thereby lowering 1O2 generation and oxidative photodamage under excess illumination. This effective photo-protective mechanism was apparently lost during the evolution from the ancestor cyanobacteria to the higher plant chloroplast

    Formation of Alkanes by Aerobic Carbonā€“Carbon Bond Coupling Reactions Catalyzed by a Phosphovanadomolybdic Acid

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    The valorization of alkanes is possible via carbonā€“carbon coupling reactions. A series of dialkyl cobalt complexes [(RCH_2)_2Co^(III)(bpy)_2]ClO_4 (R = H, Me, Et, and Ph) were reacted with the H_5PV_2Mo_(10)O_(40) polyoxometalate as a catalyst, leading to a selective oxidative carbonā€“carbon bond coupling reaction. The reaction is initiated by electron transfer from [(RCH_2)_2Co^(III)(bpy)_2]^+ to H_5PV^V_2Mo_(10)O_(40) to yield an intermediate [(RCH_2)_2Co^(IV)(bpy)_2]^(2+)ā€“H_5PV^(IV)V^VMo_(10)O_(40), as identified by a combination of EPR and X-ray photoelectron spectroscopy experiments. The reaction is catalytic with O_2 as terminal oxidant representing an aerobic Cā€“C bond coupling reaction

    Absorption changes in high light-exposed <i>Microcoleus</i> cells.

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    <p>Cells suspension was exposed to 1500 Āµmol photons m<sup>āˆ’2</sup> s<sup>āˆ’1</sup> for 40 min followed by 60 min recovery at 50 Āµmol photons m<sup>āˆ’2</sup> s<sup>āˆ’1</sup>, which resulted in the recovery of the Ftā€“Fo values (see <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0011000#pone-0011000-g003" target="_blank">Fig. 3B</a>). Elapsed time (min) from the beginning of the experiment is shown in the box. <b>Top panel</b>: Absorptions in the visible range during the entire experiment. <b>Bottom panel</b>: Absorptions changes calculated from the differences between the light exposed and zero time control. O.D.<sub>800</sub> was used for normalization. Wavelengths are indicated where maximal absorption differences were observed. Differential absorption measurements were made using a Cary 300bio UV-visible spectrophotometer (Varian, Palo Alto, USA). Integration time was set to 0.5 s, the slit to 2 nm and the wavelength increment to 2 nm.</p

    A schematic presentation of electron transport within PSII and the resulting TL bands.

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    <p>The Q<sub>A</sub> and Q<sub>B</sub> quinones, P<sub>680</sub> and the Mn cluster S-states are shown. Forward electron transport is represented by plain arrows and back electron transport by blue arrows. Changes in the peak temperature observed in TL experiments can be used as an estimate for the recombination energy of the Q<sub>B</sub><sup>āˆ’</sup>S<sub>2</sub>/Q<sub>B</sub>S<sub>1</sub> and Q<sub>B</sub><sup>āˆ’</sup>S<sub>3</sub>/Q<sub>B</sub>S<sub>2</sub> (B-band) or Q<sub>A</sub><sup>āˆ’</sup>S<sub>2</sub>/Q<sub>A</sub>S<sub>1</sub> (Q-band) redox pairs. To observe the Q band emission, reduction of the Q<sub>B</sub> site was blocked by herbicides that bind specifically to this site. The electron released from P<sub>680</sub> by light excitation at subzero temperatures can reach the Q<sub>A</sub> site and, in the presence of herbicides that bind to the Q<sub>B</sub> site, recombine upon warming with the oxidized S<sub>2</sub> state by back electron flow producing the Q band. Since the energy gap between Q<sub>A</sub><sup>āˆ’</sup> and P<sub>680</sub><i><sup>+</sup></i> is smaller than that from Q<sub>B</sub><sup>āˆ’</sup> to P<sub>680</sub><i><sup>+</sup></i> (B band), lower activation energy is required for this recombination and thus the Q band is observed at lower temperatures.</p

    Loss of variable fluorescence, even in the presence of DCMU, DBMIB and FCCP following excess light treatment.

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    <p><b>A.</b> Cells suspensions (7.5 Āµg chl ml<sup>āˆ’1</sup>) were exposed to 2000 Āµmol photons m<sup>āˆ’2</sup> s<sup>āˆ’1</sup>, 2.2 cm optical path, for the indicated times in the presence of 10 ĀµM DCMU, a concentration which completely blocked CO<sub>2</sub>-dependent O<sub>2</sub> evolution. Fv was measured after dark adaptation for 2 min using the FL 3000 fluorimeter; optical path 0.5 cm. After 15 min of excess illumination the light intensity was reduced to 50 Āµmol photons m<sup>āˆ’2</sup> s<sup>āˆ’1</sup> for 50 min. <b>B.</b> Fluorescence emission kinetics of dark-adapted cells in the presence or absence of 10 ĀµM DCMU. The cells were exposed for 950 s to 530 Āµmol photons m<sup>āˆ’2</sup> s<sup>āˆ’1</sup> of blue light using the IMAG-MAX PAM. Note that in its setup, this light intensity is the maximal but it is not saturating. <b>Insert:</b> Rate of fluorescence decline at the 150ā€“900 s range for cultures exposed to varying light intensities (100ā€“530 Āµmol photons m<sup>āˆ’2</sup> s<sup>āˆ’1</sup>). <b>C</b>. The experiment was performed as in (A), 2000 Āµmol photons m<sup>āˆ’2</sup> s<sup>āˆ’1</sup>, 2.2 cm optical path, but with 10 Āµg chl ml<sup>āˆ’1</sup> and 0.15 ĀµM DBMIB instead of DCMU. Note that DBMIB itself is a fluorescence quencher and the procedure used to minimize this effect is explained in the <a href="http://www.plosone.org/article/info:doi/10.1371/journal.pone.0011000#s4" target="_blank">Materials and Methods</a> section. <b>D.</b> Experiment performed as in (C) but in the presence of 10 ĀµM FCCP.</p
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