177 research outputs found
Thermodynamics and in-medium hadron properties from lattice QCD
Non-perturbative studies of the thermodynamics of strongly interacting
elementary particles within the context of lattice regularized QCD are being
reviewed. After a short introduction into thermal QCD on the lattice we report
on the present status of investigations of bulk properties. In particular, we
discuss the present knowledge of the phase diagram including recent
developments of QCD at non-zero baryon number density. We continue with the
results obtained so far for the transition temperature as well as the
temperature dependence of energy and pressure and comment on screening and the
heavy quark free energies. A major section is devoted to the discussion of
thermal modifications of hadron properties, taking special account of recent
progress through the use of the maximum entropy method.Comment: prepared for "Quark-Gluon Plasma III", R.Hwa (ed.
Further Evidence for an unstable H-Dibaryon?
We present preliminary results for the mass of the 6q flavor-singlet state
(, ) called H-dibaryon, calculated in quenched QCD on x30
and x30 lattices with improved gauge and fermion actions (Symanzik
improvement, Clover action). For both lattice sizes we applied the fuzzing
technique to enhance the overlap with the ground state. We observe a H-mass
above the threshold for strong decay. The difference in mass,
, increases with increasing lattice size.Comment: Poster at LATTICE99 (QCD Spectrum and Quark Masses), 3 pages, 4
figures, LaTeX2e using espcrc2.st
Quark Mass and Flavour Dependence of the QCD Phase Transition
We analyze the quark mass and flavour dependence of the QCD phase transition
temperature. When the lightest pseudo-scalar meson mass (m_PS) is larger than 2
GeV the critical temperature is controlled by the gluonic sector of QCD alone.
For smaller values of the lightest meson mass the pseudo-critical temperature
decreases slowly with m_PS. For a large regime of meson masses the
pseudo-critical temperature of 2-flavour QCD is about 10% larger than in the
3-flavour case. On lattices with temporal extent N_t=4 an extrapolation to the
chiral limit yields T_c = 173(8) MeV and 154(8) MeV for 2 and 3-flavour QCD,
respectively. We also analyze dynamical quark mass effects on the screening of
the heavy quark potential. A detailed analysis of the heavy quark free energy
in 3-flavour QCD shows that close to T_c screening effects are approximately
quark mass independent already for pseudo-scalar meson masses m_PS = 800 MeV
and screening sets in at distances r = 0.3 fm.Comment: 25 pages, LaTeX2e File, 11 EPS-file
The Phase Diagram of 2 flavour QCD with improved Actions
It has been proposed, that the chiral continuum limit of 2-flavour QCD with
Wilson fermions is brought about by a phase in which flavour and parity
symmetry are broken spontaneously at finite lattice spacing. At finite
temperature this phase should retract from the weak coupling limit to form 5
cusps. This scenario is studied with tree level Symanzik improved actions for
both gauge and fermion fields on lattices of size and .Comment: Talk given at Conference on Strong and Electroweak Matter (SEWM 98),
Copenhagen, Denmark, 2-5 Dec 199
Two Flavour QCD Phase Transition
Results on the phase transition in QCD with two flavours of light staggered
fermions from an ongoing simulation are presented. We find the restoration of
the chiral SU(2) x SU(2) symmetry, but not of the axial U_A(1) symmetry.Comment: LaTeX2e, amstex package. 4 pages, 2 figures. Talk presented at the
10th International Conference on Problems of Quantum Field Theory, Crime
Thermodynamics of two-colour QCD
We discuss the thermodynamics of two-colour QCD with four flavours of
staggered quarks on 8^3x4 and 16^3x4 lattices. In our simulations we use the
Naik action for the fermions and a (1,2) tree-level improved gauge action. We
analyze the deconfinement and chiral phase transitions for four different quark
masses (m=0.1,0.05,0.025,0.015). Contrary to three-colour QCD the peak in the
Polyakov loop susceptibility decreases with decreasing quark mass. This
reflects an early breaking of the string in the heavy quark potential, which we
verify explicitly by calculating the heavy quark potential at finite
temperature using Polyakov loop correlations.Comment: LATTICE98(hightemp), 3 pages, LaTeX2e File, 5 EPS-figures,
espcrc2.st
Free Meson Spectral Functions on the Lattice
We present results from an analytic calculation of thermal meson spectral
functions in the infinite temperature (free field) limit. We compare spectral
functions for various lattice fermion formulations used at present in studies
of in-medium properties of hadrons based on the maximum entropy method (MEM).
In particular, we will present a new calculation of spectral functions
performed with extended quark sources.Comment: 3 pages, Lattice2003(nonzero
Flavor and Quark Mass Dependence of QCD Thermodynamics
We calculate the transition temperature in 2 and 3-flavor QCD using improved
gauge and staggered fermion actions on lattices with temporal extent Nt=4. We
find Tc=173(8)MeV and 154(8)MeV for nf=2 and 3, respectively. In the case of
3-flavor QCD we present evidence that the chiral critical point, i.e. the
second order endpoint of the line of first order chiral phase transitions,
belongs to the universality class of the 3d Ising model.Comment: Talk given at Lattice 2000 (Finite Temperature), 4 pages, 6
EPS-figure
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