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Mr Kirill Melnikov (Johns Hopkins University)30/07/2009, 14:00Perturbative and Non-perturbative QCDI will describe recent developments in perturbative QCD focusing on progress in understanding one-loop corrections to multi-jet processes.Go to contribution page
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Dr Alexander Glazov (DESY)30/07/2009, 14:35Perturbative and Non-perturbative QCDRecent results from the H1 and ZEUS experiment at HERA will be presented.Go to contribution page
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Prof. Nikolaos Kidonakis (Kennesaw State University)30/07/2009, 15:10Perturbative and Non-perturbative QCDI present results for two-loop soft anomalous dimensions, which are derived from dimensionally regularized diagrams with eikonal quark lines and control soft-gluon emission in hard-scattering processes. Detailed results for the UV poles of the eikonal integrals will be shown for massive quarks, and the massless limit will also be taken. The construction of soft anomalous dimensions at...Go to contribution page
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Dr Bennie Ward (Baylor University)30/07/2009, 15:35Perturbative and Non-perturbative QCDIn the context of HERWIG6.5, we present Monte Carlo data showing the comparison between the parton shower generated by the standard DGLAP-CS kernels and that generated by the new IR-improved DGLAP-CS kernels recently developed by one of us(BFLW). This is done by implementing the new kernels in HERWIG6.5 to generate a new MC, HERWIRI1.0, for hadron-hadron interactions at high energies. Possible...Go to contribution page
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Yaquan Fang (University of Wisconsin)30/07/2009, 16:20Perturbative and Non-perturbative QCDThe large production rate of jets and photons at the LHC will provide an ideal opportunity for testing perturbative QCD, for constraining the gluon parton density function, as well as for searching for new physics. The finely segmented calorimeters, together with an efficient tracking system, allows for precision measurements of photons and jets. In this presentation, the di-jet,...Go to contribution page
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Dmitry Bandurin (Kansas State University)30/07/2009, 16:45Perturbative and Non-perturbative QCDA sample of photon plus 3-jet events collected in the D0 experiment with an integrated luminosity of 1fb-1 is used to determine the fraction of the events with double parton (DP) scattering fDP in a single ppbar collision at sqrt(s)=1.96TeV. The events are selected with photon candidate transverse momentum between 60 and 80GeV, leading jet pT above 25GeV and two additional jets with...Go to contribution page
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Dr Don Lincoln (Fermilab)30/07/2009, 17:10Perturbative and Non-perturbative QCDWe present the first measurement of dijet angular distributions in Run II of the Fermilab Tevatron Collider. The measurement is based on a dataset, corresponding to an integrated luminosity of approx 0.7 fb-1 taken with the D0 detector. Shapes of dijet angular distributions have been measured over a range of dijet masses, from 0.25 TeV and beyond 1TeV. The data are in good agreement...Go to contribution page
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Sabine Lammers (Indiana University)30/07/2009, 17:35Perturbative and Non-perturbative QCDWe present measurements of differential cross sections in inclusive Z/gamma plus jet production in a data sample of 1fb-1 collected with the D0 detector in proton antiproton collisions at sqrt(s)=1.96TeV. Measured variables include the Z/gamma transverse momentum (pT-Z), and rapidity (y-Z), the leading jet pT (pT-jet), and rapidity (y-jet), as well as various angles of the Z+jet...Go to contribution page
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