1,894 research outputs found

    Nuclear effects in photoproduction of heavy quarks and vector mesons in ultraperipheral PbPb and pPb collisions at the LHC

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    The comparison of photoproduction cross sections for ccˉc\bar{c} and b-b(bar) in PbPb and pPb collisions can give sensitivity to nuclear shadowing effects. The photoproduction of vector mesons is even more sensitive to the underlying gluon distributions. In this study we present the cross sections and rapidity dependence of the photoproduction of heavy quarks and exclusive production of vector mesons in ultraperipheral pPb and PbPb collisions at the Large Hadron Collider at sqrt(s_NN)=5 TeV and sqrt(s_NN)=2.76TeV,respectively.Thepotentialsofusingtheseprocessesforconstrainingnucleargluonshadowingareexplored.Itisfoundthatphotoproductionof TeV, respectively. The potentials of using these processes for constraining nuclear gluon shadowing are explored. It is found that photoproduction of J/\psiand and \Upsilon$ in PbPb collisions in particular exhibit very good sensitivity to gluon shadowing.Comment: 4 pages, 4 figure

    Constraining Gluon Shadowing Using Photoproduction in Ultraperipheral pA and AA Collisions

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    Photoproduction of heavy quarks and exclusive production of vector mesons in ultraperipheral proton-nucleus and nucleus-nucleus collisions depend significantly on nuclear gluon distributions. In the present study we investigate quantitatively the extent of the applicability of these processes at the Large Hadron Collider (LHC) in constraining the shadowing component of nuclear gluon modifications.Comment: 15 pages, 10 figures. arXiv admin note: substantial text overlap with arXiv:1104.428

    Computer simulation of arterial blood flow under external acceleration

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    http://www.worldcat.org/oclc/2505940

    Compensation in undoped and halogen doped CdTe crystals

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    A theoretical model is proposed which allows the calculation of the concentration of defects in pure and halogen compensated cadmium telluride grown by the THM method. All associations and ionization reactions are described in terms of the law of mass action. The ionization energies of the defects are taken from the energy level diagram established by taking into account the latest experimental data. The concentrations of the different defects calculated for chlorine doped material are in good agreement with that measured using a time of flight method
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