658 research outputs found

    Theta dependence of CP^9 model

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    We apply to the CP9CP^9 model two recently proposed numerical techniques for simulation of systems with a theta term. The algorithms, successfully tested in the strong coupling limit, are applied to the weak coupling region. The results agree and errors have been evaluated and are at % level. The results scale well with the renormalization group equation and show that, for CP9CP^9 in presence of a theta term, CP symmetry is spontaneously broken at θ=π\theta=\pi in the continuum limit.Comment: 4 pages, 4 figure

    Perfect topological charge for asymptotically free theories

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    The classical equations of motion of the perfect lattice action in asymptotically free d=2d=2 spin and d=4d=4 gauge models possess scale invariant instanton solutions. This property allows the definition of a topological charge on the lattice which is perfect in the sense that no topological defects exist. The basic construction is illustrated in the d=2d=2 O(3) non--linear σ\sigma--model and the topological susceptibility is measured to high precision in the range of correlation lengths ξ∈(2−60)\xi \in (2 - 60). Our results strongly suggest that the topological susceptibility is not a physical quantity in this model.Comment: Contribution to Lattice'94, 3 pages PostScript, uuencoded compresse

    Light hadron spectrum and quark masses in QCD with two flavors of dynamical quarks

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    We present updated results of the CP-PACS calculation of the light hadron spectrum in Nf=2N_{\rm f}=2 full QCD. Simulations are made with an RG-improved gauge action and a tadpole-improved clover quark action for sea quark masses corresponding to mPS/mV≈0.8m_{\rm PS}/m_{\rm V} \approx 0.8--0.6 and the lattice spacing a=0.22a=0.22--0.09 fm. A comparison of the full QCD spectrum with new quenched results, obtained with the same improved action, shows clearly the existence of sea quark effects in vector meson masses. Results for light quark masses in Nf=2N_{\rm f}=2 QCD are also presented.Comment: Latex 3 pages, 6 PostScript figures, Talk presented at LATTICE99(QCD Spectrum and Quark Masses

    Heavy Quarkonia from Anisotropic and Isotropic Lattices

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    We report on recent results for the spectrum of heavy quarkonia. Using coarse and anisotropic lattices we achieved an unprecedented control over statistical and systematic errors for higher excited states such as exotic hybrid states. In a parallel study on isotropic lattices we also investigate the effect of two dynamical flavours on the spin structure of charmonium and bottomonium for several symmetric lattices.Comment: LATTICE'99 (heavy quarks), 3 pages, 3 figure

    Eta meson mass and topology in QCD with two light flavors

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    We present results for the mass of the flavor singlet meson calculated on two-flavor full QCD configurations generated by the CP-PACS full QCD project. We also investigate topological charge fluctuations and their dependence on the sea quark mass.Comment: LATTICE99 (QCD Spectrum and Quark Masses), LaTeX(espcrc2.sty), 3 pages, 6 eps figure

    Hadron masses and decay constants in quenched QCD

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    We present results for the mass spectrum and decay constants using non-perturbatively O(a) improved Wilson fermions. Three values of β\beta and 30 different quark masses are used to obtain the chiral and continuum limits. Special emphasis will be given to the question of taking the chiral limit and the existence of non-analytic behavior predicted by quenched chiral perturbation theory.Comment: LATTICE99(spectrum), 3 pages, 6 figure

    String Breaking in Quenched QCD

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    We present preliminary quenched results on a new operator for the investigation of string-breaking within SU(2)-colour QCD. The ground-state of a spatially-separated static-light meson-antimeson pair is a combination of a state with two distinct mesons, expected to dominate for large separations, and a state where the light-quarks have annihilated, which contributes for short distances. The crossover between these two regimes provides a measure of the string-breaking scale length.Comment: LATTICE98(confine), 3 pages, 4 figure

    Heavy-light decay constants from clover heavy quark action in QCD with two flavors of dynamical quarks

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    We present results on an analysis of the decay constants f_B and f_Bs with two flavours of sea quark. The calculation has been carried out on 3 different bare gauge couplings and 4 sea quark masses at each gauge coupling, with m_pi/m_rho ranging from 0.8 to 0.6. We employ the Fermilab formalism to perform calculations with heavy quarks whose mass is in the range of the b-quark. A detailed comparison with a quenched calculation using the same action is made to elucidate the effects due to the sea quarks.Comment: Contribution to Lattice 99 (Heavy Quarks). Latex file, uses espcrc2.sty and epsf.sty. 3 pages, 3 encapsulated postscript figure

    Equation of state in finite-temperature QCD with improved Wilson quarks

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    We study finite-temperature phase transition and equation of state for two-flavor QCD at Nt=4N_t=4 using an RG-improved gauge action and a meanfield-improved clover quark action. The pressure is computed using the integral method. The O(4) scaling of chiral order parameter is also examined.Comment: LATTICE99(finite temperature), 3 page

    Full QCD Light Hadron Spectrum and Quark Masses: Final Results from CP-PACS

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    We present the final results of the CP-PACS calculation of the light hadron spectrum and quark masses with two flavors of dynamical quarks. Simulations are made with a renormalization-group improved gauge action and a mean-field improved clover quark action for sea quark masses corresponding to mPS/mV≈0.8m_{\rm PS}/m_{\rm V} \approx 0.8--0.6 and the lattice spacing a=0.22a=0.22--0.11 fm. For the meson spectrum in the continuum limit a clearly improved agreement with experiment is observed compared to the quenched case, demonstrating the importance of sea quark effects. For light quark masses we obtain mudMSˉ(2GeV)=3.44−0.22+0.14m_{ud}^{\bar{MS}}(2GeV)=3.44^{+0.14}_{-0.22} MeV and msMSˉ(2GeV)=88−6+4m_s^{\bar{MS}}(2GeV)=88^{+4}_{-6} MeV (KK-input) and msMSˉ(2GeV)=90−11+5m_s^{\bar{MS}}(2GeV)=90^{+5}_{-11} MeV (ϕ\phi-input), which are reduced by about 25% compared to the values in quenched QCD.Comment: Lattice 2000 (Spectrum), 4 pages, 3 figure
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