7 research outputs found

    Nonperturbative and perturbative aspects of photo- and electroproduction of vector mesons

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    We discuss various aspects of vector meson production, first analysing the interplay between perturbative and nonperturbative aspects of the QCD calculation. Using a general method adapted to incorporate both perturbative and nonpertubative aspects, we show that nonperturbative effects are important for all experimentally available values of the photon virtuality Q2. We compare the huge amount of experimental information now available with our theoretical results obtained using a specific nonperturbative model without free parameters, showing that quite simple features are able to explain the data.Comment: 19 page

    The XMM-Newton Serendipitous Survey: I - The role of XMM-Newton Survey Science Centre

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    This paper describes the performance of XMM-Newton for serendipitous surveys and summarises the scope and potential of the XMM-Newton Serendipitous Survey. The role of the Survey Science Centre (SSC) in the XMM-Newton project is outlined. The SSC's follow-up and identification programme for the XMM-Newton serendipitous survey is described together with the presentation of some of the first results

    Muoproduction of J / psi and the gluon distribution of the nucleon

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    Ashman J, Badelek B, Baum G, et al. Muoproduction of J/Psi and the gluon distribution of the nucleon. Z.Phys. C. 1992;56(1):21-28

    Elastic and Proton-Dissociative Photoproduction of J/ψJ/\psi Mesons at HERA

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    Cross sections for elastic and proton-dissociative photoproduction of J/ψ mesons are measured with the H1 detector in positron-proton collisions at HERA. The data were collected at ep centre-of-mass energies s√≈318 GeV and s√≈225 GeV , corresponding to integrated luminosities of L=130 pb−1 and L=10.8 pb−1 , respectively. The cross sections are measured as a function of the photon-proton centre-of-mass energy in the range 25<W Îłp <110 GeV. Differential cross sections dσ/dt, where t is the squared four-momentum transfer at the proton vertex, are measured in the range |t|<1.2 GeV2 for the elastic process and |t|<8 GeV2 for proton dissociation. The results are compared to other measurements. The W Îłp and t-dependences are parametrised using phenomenological fits
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