The QCD transition temperature: results with physical masses in the continuum limit II.
arXiv:0903.4155 · doi:10.1088/1126-6708/2009/06/088
Abstract
We extend our previous study [Phys. Lett. B643 (2006) 46] of the cross-over temperatures (T_c) of QCD. We improve our zero temperature analysis by using physical quark masses and finer lattices. In addition to the kaon decay constant used for scale setting we determine four quantities (masses of the Ωbaryon, K^*(892) and ϕ(1020) mesons and the pion decay constant) which are found to agree with experiment. This implies that --independently of which of these quantities is used to set the overall scale-- the same results are obtained within a few percent. At finite temperature we use finer lattices down to a <= 0.1 fm (N_t=12 and N_t=16 at one point). Our new results confirm completely our previous findings. We compare the results with those of the 'hotQCD' collaboration.
19 pages, 8 figures, 3 tables
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- Quark-hadron phase transition in massive gravity
- Influence of magnetic fields on the color screening masses
- Effect of charged particle's multiplicity fluctuations on flow harmonics in even-by-event hydrodynamics
- condensation, Nielsen's identity and effective potential of order parameter
- Screening properties of quark-gluon plasma obtained from distribution and correlation functions of the constituent quasiparticle model
- The QGP dynamics in relativistic heavy-ion collisions
- Gluonic Colour Singlets in QCD
- Chiral Symmetry Restoration using the Running Coupling Constant from the Light-Front Approach to QCD
- Monopoles, spectra of overlap fermions, and eta-prime meson in external magnetic fields
- Correlation corrections to the thermodynamic properties of spin asymmetric QGP matter
- Finite temperature QCD crossover at non-zero chemical potential: A Dyson-Schwinger approach
- The quest for the quark-gluon plasma from the perspective of dynamical models of relativistic heavy-ion collisions