4 research outputs found

    Searching for KvBLL calorons in SU(3) lattice gauge field ensembles

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    We discuss Kraan - van Baal - Lee - Lu (KvBLL) solutions of the classical Yang-Mills equations with temperature in the context of SU(3) lattice gauge theory. We present discretized lattice versions of KvBLL solutions and other dyonic structures, obtained by cooling in order to understand their variety and signature. An analysis of the zero modes of the lattice Dirac operator for different fermionic boundary conditions gives clear evidence for a KvBLL-like background of finite T lattice subensembles with Q = +/-1. Using APE-smearing we are able to study the topological charge density q(x) of the configurations and to corroborate this interpretation.Comment: Presented at LATTICE 2003 (topology) by C. Gattringer and E.M. Ilgenfritz, 6 page

    Dilepton production in proton-proton collisions at BEVALAC energies

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    The dilepton production in elementary ppe+eX{pp\to e^{+}e^{-}X} reactions at BEVALAC energies Tlab=1÷5T_{lab}=1\div 5 GeV is investigated. The calculations include direct e+e{e^{+}e^{-}} decays of the vector mesons ρ0\rho ^{0}, ω\omega , and ϕ\phi , Dalitz decays of the π0\pi ^{0}-, η\eta -, % \rho -, ω\omega -, and ϕ\phi -mesons, and of the baryon resonances % \Delta (1232),N(1520), ...... . The subthreshold vector meson production cross sections in pppp collisions are treated in a way sufficient to avoid double counting with the inclusive vector meson production. The vector meson dominance model for the transition form factors of the resonance Dalitz decays Re+eNR\to e^{+}e^{-}N is used in an extended form to ensure correct asymptotics which are in agreement with the quark counting rules. Such a modification gives an unified and consistent description of both RNγR\to N\gamma radiative decays and RNρ(ω)R\to N\rho (\omega) meson decays. The effect of multiple pion production on the experimental efficiency for the detection of the dilepton pairs is studied. We find the dilepton yield in reasonable agreement with the experimental data for the set of intermediate energies whereas at the highest energy Tlab=4.88T_{lab}=4.88 GeV the number of dilepton pairs is likely to be overestimated experimentally in the mass range M=300÷700M=300\div 700 MeV.Comment: 25 pages (IOP style), 5 figures, revised manuscript accepted for publication in JP
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