10 research outputs found

    Light Spectrum and Decay Constants in Full QCD with Wilson Fermions

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    We present results from an analysis of the light spectrum and the decay constants f_{\pi} and f_V^{-1} in Full QCD with n_f=2 Wilson fermions at a coupling of beta=5.6 on a 16^3x32 lattice.Comment: 3 pages, LaTeX with 4 eps figures, Talk presented at LATTICE96(spectrum

    An Estimate of alpha_S from Bottomonium in Unquenched QCD

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    We estimate the strong coupling constant from the perturbative expansion of the plaquette. The scale is set by the 2S-1S and 1P-1S splittings in bottomonium which are computed in NRQCD on dynamical gauge configurations with nf=2 degenerate Wilson quarks at intermediate masses. We have increased the statistics of our spectrum calculation in order to reliably extrapolate in the sea-quark mass. We find a value of alpha_MS(m_Z) = 0.1118(26) which is somewhat lower than previous estimates within NRQCD.Comment: LATTICE98(heavyqk

    Preliminary Calculation of αs\alpha_s from Green Functions with Dynamical Quarks

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    We present preliminary results on the computation of the QCD running coupling constant in the MOM~\widetilde{MOM} scheme and Landau gauge with two flavours of dynamical Wilson quarks. Gluon momenta range up to about 7 GeV (β=\beta = 5.6, 5.8 and 6.0) with a constant dynamical-quark mass. This range already allows to exhibit some evidence for a sizable 1/μ21/\mu^2 correction to the asymptotic behaviour, as in the quenched approximation, although a fit without power corrections is still possible with a reasonable χ2\chi^2. Following the conclusions of our quenched study, we take into account 1/μ21/\mu^2 correction to the asymptotic behaviour. We find ΛMSˉNf=2=264(27)MeV×[a1(5.6,0.1560)/2.19GeV]\Lambda_{\rm \bar{MS}}^{N_f=2} = 264(27) {\rm MeV} \times [{a^{-1}(5.6,0.1560)}/{2.19 {\rm GeV}}] , which leads to αs(MZ)=0.113(3)(4)\alpha_s(M_Z) = 0.113(3)(4). The latter result has to be taken as a preliminary indication rather than a real prediction in view of the systematic errors still to be controlled. Still, being two sigmas below the experimental result makes it very encouraging.Comment: 14 pages, 3 figs., 2 tabs., revte

    Unquenching the Quark Model and Screened Potentials

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    The low-lying spectrum of the quark model is shown to be robust under the effects of `unquenching'. In contrast, the use of screened potentials is shown to be of limited use in models of hadrons. Applications to unquenching the lattice Wilson loop potential and to glueball mixing in the adiabatic hybrid spectrum are also presented.Comment: 6 pages, 3 ps figures, revtex. Version to appear in J. Phys.

    QCD with dynamical Wilson fermions—First results from SESAM

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    First results of a recently started simulation of full QCD with two flavours of sea-quarks at a coupling of β=5.6\beta = 5.6 on a 163×3216^3 \times 32 lattice are presented. Emphasis is laid on the statistical significance that can be achieved by an ``integrated luminosity'' of 140 TFlop×\timeshrs, for Hybrid Monte Carlo simulations at four intermediate values of mπmρ\frac{m_{\pi}}{m_{\rho}}. The simulation takes place on the Quadrics QH2 at DESY/Zeuthen and DFG/Bielefeld. The performance is optimized by means of BiCGStab and the chronological inversion method of Brower et al. We discuss the systematic errors arising from lack of the molecular dynamic's reversibility on the 32-bit QH2. For plaquette and meson correlators we find integrated autocorrelation times of <20< 20 units of molecular dynamics time and exponential autocorrelation times of about 5050 units. Using these results we perform preliminary measurements of the central potential and π\pi and ρ\rho correlators on independent configurations and obtain first estimates of the lattice spacings at three values of the dynamical hopping parameter.Comment: Contributions by Th.Lippert and H.Hoeber to LAT95, Melbourne, July 1995. 8 pages, 1 ps-file, tar-compressed and uuencode

    Hadrons and nuclei

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