Thermodynamics and higher order moments in SU(3) linear -model with gluonic quasi-particles
arXiv:1411.1871 · doi:10.1088/0954-3899/42/1/015004
Abstract
In framework of linear -model (LSM) with three quark flavors, the chiral phase-diagram at finite temperature and density is investigated. At temperatures higher than the critical temperature (), we added to LSM the gluonic sector from the quasi-particle model (QPM), which assumes that the interacting gluons in the strongly interacting matter, the quark-gluon plasma (QGP), are phenomenologically the same as non-interacting massive quasi-particles. The dependence of the chiral condensates of strange and non-strange quarks on temperature and chemical potential is analysed. Then, we have calculated the thermodynamics in the new approach (combination of LSM and QPM). Confronting the results with recent lattice QCD simulations shows an excellent agreement in almost all thermodynamic quantities. The first and second order moments of particle multiplicity are studied in dependence on the chemical potential but at fixed temperature and on the chemical potential but at fixed temperature. These are implemented in characterizing the large fluctuations accompanying the chiral phase-transition. The results of first and second order moments are compared with the SU(3) Polyakov linear -model (PLSM). Also, the resulting phase-diagrams deduced in PLSM and LSMQPM are compared with each other.
arXiv commentto appear in J. Phys. G, 26 pages, 9 figures with 11 eps-graphs. arXiv admin note: text overlap with arXiv:1405.0577
References in corpus (24)
- Full result for the QCD equation of state with 2+1 flavors
- Chiral effective model with the Polyakov loop
- Phases of QCD: lattice thermodynamics and a field theoretical model
- Equation of state and QCD transition at finite temperature
- The Phase Structure of the Polyakov--Quark-Meson Model
- Phase diagrams in the three-flavor Nambu--Jona-Lasinio model with the Polyakov loop
- The Quark-Gluon Plasma in Equilibrium
- Chiral Phase Transition within Effective Models with Constituent Quarks
- Massive gluons and quarks and the equation of state obtained from SU(3) lattice QCD
- Equation of State for physical quark masses
- Chiral Symmetry Restoration at Nonzero Temperature in the SU(3) \times SU(3) Linear Sigma Model
- The three-flavor chiral phase structure in hot and dense QCD matter
- From QCD lattice calculations to the equation of state of quark matter
- A Family of Equations of State Based on Lattice QCD: Impact on Flow in Ultrarelativistic Heavy-Ion Collisions
- The QCD equation of state near T_0 within a quasi-particle model
- The critical surface of the SU(3)_L x SU(3)_R chiral quark model at non-zero baryon density
- QCD Equations of State and the QGP Liquid Model
- Quasiparticle Description of Hot QCD at Finite Quark Chemical Potential
- Degrees of freedom and the phase transitions of two flavor QCD
- On the QCD phase structure from effective models
- Polyakov linear SU(3) sigma model: features of higher order moments in dense and thermal hadronic medium
- Quasi-particle model of strongly interacting matter
- Fluctuations in the vicinity of the phase transition line for two flavor QCD
- Conserved Charge Fluctuations in a Chiral Hadronic Model including Hadrons and Quarks
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- Quark-hadron phase structure of QCD matter from SU() Polyakov linear sigma model
- QCD Phase-transition and chemical freezeout in nonzero magnetic field at NICA
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