6,703 research outputs found

    Non-trivial Center Dominance in High Temperature QCD

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    We investigate the properties of quarks and gluons above the chiral phase transition temperature Tc,T_c, using the RG improved gauge action and the Wilson quark action with two degenerate quarks mainly on a 323×1632^3\times 16 lattice. In the one-loop perturbation theory, the thermal ensemble is dominated by the gauge configurations with effectively Z(3)Z(3) center twisted boundary conditions, making the thermal expectation value of the spatial Polyakov loop take a non-trivial Z(3)Z(3) center. This is in agreement with our lattice simulation of high temperature QCD. We further observe that the temporal propagator of massless quarks at extremely high temperature β=100.0 (T≃1058Tc)\beta=100.0 \, (T \simeq10^{58} T_c) remarkably agrees with the temporal propagator of free quarks with the Z(3)Z(3) twisted boundary condition for t/Lt≥0.2t/L_t \geq 0.2, but differs from that with the Z(3)Z(3) trivial boundary condition. As we increase the mass of quarks mqm_q, we find that the thermal ensemble continues to be dominated by the Z(3)Z(3) twisted gauge field configurations as long as mq≤3.0 Tm_q \le 3.0 \, T and above that the Z(3)Z(3) trivial configurations come in. The transition is essentially identical to what we found in the departure from the conformal region in the zero-temperature many-flavor conformal QCD on a finite lattice by increasing the mass of quarks. We argue that the behavior is consistent with the renormalization group analysis at finite temperature.Comment: 16 pages, 9 figures; 4 tables, an appendix adde

    O(αsa)O(\alpha_{s}a) matching coefficients for axial vector current and ΔB\Delta B==2 operator

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    We present a calculation of the perturbative matching coefficients including mixing with higher dimensional operators for the temporal component of the heavy-light axial current, A4A_{4}, and the ΔB=2\Delta B=2 operator, OSO_S. For A4static,NRQCDA_{4}^{\scriptsize static, NRQCD}, calculations with various RG-improved gauge actions are peformed. Matching coefficients with NRQCD and heavy-clover actions are also compared.Comment: LATTICE99 (Heavy Quarks), 3 pages, 2 figures, espcrc2.st
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