109 research outputs found

    Light Quenched Hadron Spectrum and Decay Constants on different Lattices

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    We present a study of O(2000){\cal O}(2000) (quenched) lattice configurations from the APE collaboration, for 6.0β6.46.0\le\beta\le 6.4 using both the Wilson and the SW-Clover fermion action. We determine the light hadronic spectrum and meson decay constants. We extract the inverse lattice spacing using data at the simulated values of the quark mass. We find an agreement with the experimental data of 5\sim 5% for mesonic masses and 10\sim 10%-15% for baryonic masses and pseudoscalar decay constants. A larger deviation is present for the vector decay constants.Comment: 3 pages, Talk presented at LATTICE96(spectrum

    Current Renormalisation Constants with an O(a)-improved Fermion Action

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    Using chiral Ward identities, we determine the renormalisation constants of bilinear quark operators for the Sheikholeslami-Wohlert action lattice at beta=6.2. The results are obtained with a high degree of accuracy. For the vector current renormalisation constant we obtain Z_V=0.817(2)(8), where the first error is statistical and the second is due to mass dependence of Z_V. This is close to the perturbative value of 0.83. For the axial current renormalisation constant we obtain Z_A = 1.045(+10 -14), significantly higher than the value obtained in perturbation theory. This is shown to reduce the difference between lattice estimates and the experimental values for the pseudoscalar meson decay constants, but a significant discrepancy remains. The ratio of pseudoscalar to scalar renormalisation constants, Z_P/Z_S, is less well determined, but seems to be slightly lower than the perturbative value.Comment: 8 pages uuencoded compressed postscript file. Article to be submitted to Phys.Rev.

    RESULTS FOR THE B-MESON DECAY CONSTANT FROM THE APE COLLABORATION

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    The decay constant for the B-meson in the static limit is calculated using the Wilson and clover actions at various lattice spacings. We show that both the contamination of our results by excited states and the effects finite lattice spacing are at most the order of the statistical uncertainties. A comparison is made of our results and those obtained in other studies. Values for fBSstat/fBstatf^{stat}_{B_S}/f^{stat}_B and MBSMBM_{B_S} - M_B are also given.Comment: Contribution to Lattice'94, 3 pages PostScript, uuencoded compresse

    Light Quark Mass Determinations from the Lattice

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    This paper is a review of recent lattice determinations of the light quark masses. It describes the method employed to calculate quark masses in the lattice formulation, and the extrapolations required to reach the physical regime. This review is designed to be accessible to a general audience, not specifically lattice theorists.Comment: Invited review talk at QCD97, Montpellier (July '97). 8 pages, 2 figures. Requires espcrc2.sty Minor changes: a reference added and a table updated accordingl

    Fluctuations in the vicinity of the phase transition line for two flavor QCD

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    We study the susceptibilities of quark number, isospin number and electric charge in numerical simulations of lattice QCD at high temperature and density. We discuss the equation of state for 2 flavor QCD at non-zero temperature and density. Derivatives of lnZ\ln Z with respect to quark chemical potential (μq)(\mu_q) are calculated up to sixth order. From this Taylor series, the susceptibilities are estimated as functions of temperature and μq\mu_q. Moreover, we comment on the hadron resonance gas model, which explains well our simulation results below TcT_c.Comment: 3 pages, 5 figures, Talk presented at Lattice2004(non-zero

    Where is the chiral critical point in 3-flavor QCD?

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    We determine the location of the second order endpoint of the line of first order chiral phase transition in 3-flavor QCD at vanishing chemical potential. Using Ferrenberg-Swendsen reweighting for two values of the quark mass we determine the dependence of the transition line on the chemical potential and locate the chiral critical point. For both quantities we find a significant quark mass dependence.Comment: 3 pages, Lattice2003(nonzero), one reference exchange

    QCD at non-zero temperature and density from the lattice

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    The study of systems as diverse as the cores of neutron stars and heavy-ion collision experiments requires the understanding of the phase structure of QCD at non-zero temperature, T, and chemical potential, mu_q. We review some of the difficulties of performing lattice simulations of QCD with non-zero mu_q, and outline the re-weighting method used to overcome this problem. This method is used to determine the critical endpoint of QCD in the (mu_q,T) plane. We study the pressure and quark number susceptibility at small mu_q.Comment: 5 pages, talk presented by C.R. Allton at the QCD Downunder Conference, Barossa Valley and Adelaide, March 200

    The quark mass and μ\mu dependence of the QCD chiral critical point

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    In order to study the QCD chiral critical point we investigate Binder Cumulants of the chiral condensate. The results were obtained from simulations of 3 and 2+1 flavors of standard staggered fermions and 3 flavors of p4 improved staggered fermions. The quark masses used are close to the physical quark mass. To extract the dependence on quark mass and chemical potential we apply a new reweighting technique based on a Taylor expansion of the action. The reweighting accuracy is O(m){\cal O}(m) for the standard and O(m2){\cal O}(m^2), O(μ2){\cal O}(\mu^2) for the p4 action.Comment: 3 pages, 6 figures, Lattice2002(nonzerot

    Light quenched hadron spectrum and decay constants on different lattices

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    In this paper we study O(2000) (quenched) lattice configurations from the APE collaboration, for different lattice volumes and for 6.0 less than or equal to beta less than or equal to 6.4 using both the Wilson and the SW-Clover fermion actions, We determine the light hadronic spectrum and meson decay constants and study the mesonic dispersion relation. We extract the hadronic variable J and the strange quark mass in the continuum at the next-to-leading order obtaining m(s)()(mu = 2 GeV) = 122 +/- 20 MeV. A study is made of their dependence on lattice spacing, We implement a newly developed technique to extract the inverse lattice spacing using data at the simulated values of the quark mass (i.e. at masses around the strange quark mass)

    The continuum limit of fBf_B from the lattice in the static approximation

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    We present an analysis of the continuum extrapolation of fBf_B in the static approximation from lattice data. The method described here aims to uncover the systematic effects which enter in this extrapolation and has not been described before. Our conclusions are that we see statistical evidence for scaling of fBstatf_B^{stat} for inverse lattice spacings \gtap 2 GeV but not for \ltap 2 GeV. We observe a lack of {\em asymptotic} scaling for a variety of quantities, including fBstatf_B^{stat}, at all energy scales considered. This can be associated with finite lattice spacing systematics. Once these effects are taken into account, we obtain a value of 230(35) MeV for fBstatf_B^{stat} in the continuum where the error represents uncertainties due to both the statistics and the continuum extrapolation. In this method there is no error due to uncertainties in the renormalization constant connecting the lattice and continuum effective theories.Comment: 33 pages, latex text file and postscript figures all uuencoded into a single file, ROME preprint 94/104
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