9,408 research outputs found

    Discovery and characterization of pentose-specific transporters in Saccharomyces cerevisiae

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    Saccharomyces cerevisiae is considered one of the most promising organisms for ethanol production from lignocellulosic feedstock. Unfortunately, pentose sugars, which make up to 30% of lignocellulose, cannot be utilized by S. cerevisiae. Pentoses can only enter yeast cells through hexose transporters, which have two orders of magnitude lower affinities for pentose sugars. Additionally, inefficient pentose uptake has been shown to be the limiting step for some D-xylose metabolizing yeast strains. In this thesis, we report the discovery of seven active pentose transporters from pentose assimilating fungal species Pichia stipitis and Neurospora crassa based on sequence homology with the glucose/xylose/H+ symporter (GXS1) in Candida intermedia. These transporters were cloned and heterologously expressed in S. cerevisiae and their sugar uptake activities were studied by analysis of intracellular sugar accumulation using HPLC. Among the seven active transporters, one L-arabinose-specific and two D-xylose-specific transporters were identified. These transporters were functionally expressed and properly localized in S. cerevisiae as indicated by HPLC analysis and immunofluorescence microscopy, respectively. Kinetic parameters of the transporters were determined using a 14C-labeled sugar uptake assay. Sugar uptake assay in un-buffered cell suspension indicated the sugar uptake through these three transporters was not coupled with proton uptake, revealing that these three sugar transporters are facilitators. Introduction of these pentose-specific transporters may facilitate pentose sugar utilization in S. cerevisiae by improving pentose uptake. More efficient utilization of pentose sugars will lower the cost for lignocellulosic ethanol production

    Determination of f0−σf_0-\sigma mixing angle through Bs0→J/Ψ f0(980)(σ)B_s^0 \to J/\Psi~f_0(980)(\sigma) decays

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    We study Bs0→J/ψf0(980)B_s^0 \to J/\psi f_0(980) decays, the quark content of f0(980)f_0(980) and the mixing angle of f0(980)f_0(980) and σ(600)\sigma(600). We calculate not only the factorizable contribution in QCD facorization scheme but also the nonfactorizable hard spectator corrections in QCDF and pQCD approach. We get consistent result with the experimental data of Bs0→J/ψf0(980)B_s^0 \to J/\psi f_0(980) and predict the branching ratio of Bs0→J/ψσB_s^0 \to J/\psi \sigma. We suggest two ways to determine f0−σf_0-\sigma mixing angle θ\theta. Using the experimental measured branching ratio of Bs0→J/ψf0(980)B_s^0 \to J/\psi f_0(980) , we can get the f0−σf_0-\sigma mixing angle θ\theta with some theoretical uncertainties. We suggest another way to determine f0−σf_0-\sigma mixing angle θ\theta using both of experimental measured decay branching ratios Bs0→J/ψf0(980)(σ)B_s^0 \to J/\psi f_0(980) (\sigma) to avoid theoretical uncertainties.Comment: arXiv admin note: substantial text overlap with arXiv:0707.263

    The study of B→J/Ψη(′)B\to J/\Psi \eta^{(\prime)} decays and determination of η−η′\eta-\eta^{\prime} mixing angle

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    We study B→J/Ψη(′)B\to J/\Psi \eta^{(\prime)} decays and suggest two methods to determine the η−η′\eta-\eta^{\prime} mixing angle. We calculate not only the factorizable contribution in QCD facorization scheme but also the nonfactorizable hard spectator corrections in pQCD approach. We get the branching ratio of B→J/ΨηB\to J/\Psi \eta which is consistent with recent experimental data and predict the branching ratio of B→J/Ψη′B\to J/\Psi \eta^{\prime} to be 7.59×10−67.59\times 10^{-6}. Two methods for determining η−η′\eta-\eta^{\prime} mixing angle are suggested in this paper. For the first method, we get the η−η′\eta-\eta^{\prime} mixing angle to be about −13.1∘-13.1^{\circ}, which is in consistency with others in the literature. The second method depends on less parameters so can be used to determine the η−η′\eta-\eta^{\prime} mixing angle with better accuracy but needs, as an input, the branching ratio for B→J/Ψη′B\to J/\Psi \eta^{\prime}which should be measured in the near future.Comment: 16pages,4figure
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