116 research outputs found

    Direct determination of the gauge coupling derivatives for the energy density in lattice QCD

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    By matching Wilson loop ratios on anisotropic lattices we measure the coefficients \cs and \ct, which are required for the calculation of the energy density. The results are compared to that of an indirect method of determination. We find similar behaviour, the differences are attributed to different discretization errors.Comment: Talk presented at LATTICE97(finite temperature), 3 pages, 5 Postscript figure

    Scaling Properties of the Energy Density in SU(2) Lattice Gauge Theory

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    The lattice data for the energy density of SU(2)SU(2) gauge theory are calculated with \nop~derivatives of the coupling constants. These derivatives are obtained from two sources : i) a parametrization of the \nop~beta function in accord with the measured critical temperature and ΔÎČ−\Delta\beta-values and ii) a \nop~calculation of the presssure. We then perform a detailed finite size scaling analysis of the energy density near TcT_c. It is shown that at the critical temperature the energy density is scaling as a function of VT3VT^3 with the corresponding 3d3d Ising model critical exponents. The value of Ï”(Tc)/Tc4\epsilon(T_c)/T^4_c in the continuum limit is estimated to be 0.256(23). In the high temperature regime the energy density is approaching its weak coupling limit from below, at T/Tc≈2T/T_c \approx 2 it has reached only about 70%70\% of the limit.Comment: 15 pages + 9 figures, BI-TP 94/3

    Moments of charge fluctuations, pseudo-critical temperatures and freeze-out in heavy ion collisions

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    We discuss universal properties of higher order cumulants of net baryon number fluctuations and point out their relevance for the analysis of freeze-out and critical conditions in heavy ion collisions at LHC and RHIC.Comment: 4 pages, 5 EPS files, to appear in the proceedings of Quark Matter 2011, 23-28 May 2011, Annecy, Franc

    Thermodynamics of Four-Flavour QCD with Improved Staggered Fermions

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    We have calculated the pressure and energy density in four-flavour QCD using improved fermion and gauge actions. We observe a strong reduction of finite cut-off effects in the high temperature regime, similar to what has been noted before for the SU(3) gauge theory. Calculations have been performed on 163×416^3\times 4 and 16^4 lattices for two values of the quark mass, ma=0.05ma = 0.05 and 0.1. A calculation of the string tension at zero temperature yields a critical temperature Tc/σ=0.407±0.010T_c/\sqrt{\sigma} = 0.407 \pm 0.010 for the smaller quark mass value.Comment: 12 pages, LaTeX2e File, 11 encapsulated postscript file

    The beta function and equation of state for QCD with two flavors of quarks

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    We measure the pressure and energy density of two flavor QCD in a wide range of quark masses and temperatures. The pressure is obtained from an integral over the average plaquette or psi-bar-psi. We measure the QCD beta function, including the anomalous dimension of the quark mass, in new Monte Carlo simulations and from results in the literature. We use it to find the interaction measure, E-3p, yielding non-perturbative values for both the energy density E and the pressure p. uuencoded compressed PostScript file Revised version should work on more PostScript printers.Comment: 24 page

    A Study of Finite Temperature Gauge Theory in (2+1) Dimensions

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    We determine the critical couplings and the critical exponents of the finite temperature transition in SU(2) and SU(3) pure gauge theory in (2+1) dimensions. We also measure Wilson loops at T=0T=0 on a wide range of ÎČ\beta values using APE smearing to improve the signal. We extract the string tension σ\sigma from a fit to large distances, including a string fluctuation term. With these two entities we calculate Tc/σT_c/\sqrt{\sigma}.Comment: Talk presented at LATTICE96(finite temperature), not espcrc2 style: 7 pages, 4 ps figures, 22 k

    Non-perturbative determination of anisotropy coefficients in lattice gauge theories

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    We propose a new non-perturbative method to compute derivatives of gauge coupling constants with respect to anisotropic lattice spacings (anisotropy coefficients), which are required in an evaluation of thermodynamic quantities from numerical simulations on the lattice. Our method is based on a precise measurement of the finite temperature deconfining transition curve in the lattice coupling parameter space extended to anisotropic lattices by applying the spectral density method. We test the method for the cases of SU(2) and SU(3) gauge theories at the deconfining transition point on lattices with the lattice size in the time direction Nt=4N_t=4 -- 6. In both cases, there is a clear discrepancy between our results and perturbative values. A longstanding problem, when one uses the perturbative anisotropy coefficients, is a non-vanishing pressure gap at the deconfining transition point in the SU(3) gauge theory. Using our non-perturbative anisotropy coefficients, we find that this problem is completely resolved: we obtain Δp/T4=0.001(15)\Delta p/T^4 = 0.001(15) and −0.003(17)-0.003(17) on Nt=4N_t=4 and 6 lattices, respectively.Comment: 24pages,7figures,5table

    Lattice sum rules for the colour fields

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    We analyse the sum rules describing the action and energy in the colour fields around glueballs, torelons and static potentials.Comment: 9 pages LATEX, (typos corrected, to appear in Phys Rev D

    The non-zero baryon number formulation of QCD

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    We discuss the non-zero baryon number formulation of QCD in the quenched limit at finite temperature. This describes the thermodynamics of gluons in the background of static quark sources. Although a sign problem remains in this theory, our simulation results show that it can be handled quite well numerically. The transition region gets shifted to smaller temperatures and the transition region broadens with increasing baryon number. Although the action is in our formulation explicitly Z(3) symmetric the Polyakov loop expectation value becomes non-zero already in the low temperature phase and the heavy quark potential gets screened at non-vanishing number density already this phase.Comment: LATTICE99(Finite Temperature and Density), Latex2e using espcrc2.sty, 3 pages, 7 figure
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