Crossover-model approach to QCD phase diagram, equation of state and susceptibilities in the 2+1 and 2+1+1 flavor systems

We construct a simple model for describing the hadron-quark crossover transition by using lattice QCD (LQCD) data in the 2+1 flavor system, and draw the phase diagram in the 2+1 and 2+1+1 flavor systems through analyses of the equation of state (EoS) and the susceptibilities. In the present hadron-quark crossover (HQC) model is successful in reproducing LQCD data on the EoS and the flavor susceptibilities.We define the hadron-quark transition temperature. For the 2+1 flavor system, the transition line thus obtained is almost identical in planes that are created by temperature and the chemical potential for the baryon-number(B), the isospin(I), the hypercharge(Y), when the chemical potentials are smaller than 250 MeV. This BIY approximate equivalence persists also in the 2+1+1 flavor system. We plot the phase diagram also in planes that are created by temperature and the chemical potential for u,d,s quark number in order to investigate flavor dependence of transition lines. In the 2+1+1 flavor system, c quark does not affect the 2+1 flavor subsystem composed of u, d, s. The flavor off-diagonal susceptibilities are good indicators to see how hadrons survive as T increases, since the independent quark model hardly contributes to them.

[1]  W. Hager,et al.  and s , 2019, Shallow Water Hydraulics.

[2]  Z. Fodor,et al.  Calculation of the axion mass based on high-temperature lattice quantum chromodynamics , 2016, Nature.

[3]  M. Yahiro,et al.  Equation of state and transition temperatures in the quark-hadron hybrid model , 2016, 1604.05002.

[4]  Z. Fodor,et al.  Fluctuations and correlations in high temperature QCD , 2015, 1507.04627.

[5]  J. Kapusta,et al.  Matching excluded-volume hadron-resonance gas models and perturbative QCD to lattice calculations , 2014, 1404.7540.

[6]  M. Strickland,et al.  Three-loop pressure and susceptibility at finite temperature and density from hard-thermal-loop perturbation theory , 2014 .

[7]  M. Strickland,et al.  Three-loop HTLpt thermodynamics at finite temperature and chemical potential , 2014, 1402.6907.

[8]  Z. Fodor,et al.  Full result for the QCD equation of state with 2+1 flavors , 2013, 1309.5258.

[9]  Z. Fodor,et al.  Is there a flavor hierarchy in the deconfinement transition of QCD? , 2013, Physical review letters.

[10]  Y. Sakai,et al.  Confinement and $\mathbb {Z}_{3}$ symmetry in three-flavor QCD , 2013, 1301.4013.

[11]  Z. Fodor,et al.  QCD equation of state at nonzero chemical potential: continuum results with physical quark masses at order μ2 , 2012, 1204.6710.

[12]  Z. Fodor,et al.  Precision SU(3) lattice thermodynamics for a large temperature range , 2012, 1204.6184.

[13]  E. Megías,et al.  Polyakov loop and the hadron resonance gas model. , 2012, Physical review letters.

[14]  Z. Fodor,et al.  Fluctuations of conserved charges at finite temperature from lattice QCD , 2011, 1112.4416.

[15]  K. Kashiwa,et al.  Nonlocal Polyakov–Nambu–Jona-Lasinio model and imaginary chemical potential , 2011, 1106.5025.

[16]  Y. Sakai,et al.  Quark-mass dependence of the three-flavor QCD phase diagram at zero and imaginary chemical potential: Model prediction , 2011, 1105.3959.

[17]  R. Gatto,et al.  Deconfinement and Chiral Symmetry Restoration in a Strong Magnetic Background , 2010, 1012.1291.

[18]  Y. Sakai,et al.  Entanglement between deconfinement transition and chiral symmetry restoration (熱場の量子論とその応用) , 2010, 1006.3648.

[19]  Z. Fodor,et al.  Is there still any Tc mystery in lattice QCD? Results with physical masses in the continuum limit III , 2010, 1005.3508.

[20]  G. Nardulli,et al.  Chiral crossover, deconfinement and quarkyonic matter within a Nambu-Jona Lasinio model with the Polyakov loop , 2008, 0805.1509.

[21]  K. Fukushima Phase diagrams in the three-flavor Nambu-Jona-Lasinio model with the Polyakov loop , 2008, 0803.3318.

[22]  M. Yahiro,et al.  Critical endpoint in the Polyakov-loop extended NJL model , 2007, 0710.2180.

[23]  S. Ejiri Existence of the critical point in finite density lattice QCD , 2007, 0706.3549.

[24]  B. Schaefer,et al.  Phase structure of the Polyakov-quark-meson model , 2007, 0704.3234.

[25]  W. Weise,et al.  Polyakov loop, diquarks, and the two-flavor phase diagram , 2006, hep-ph/0609281.

[26]  Z. Fodor,et al.  The order of the quantum chromodynamics transition predicted by the standard model of particle physics , 2006, Nature.

[27]  Z. Fodor,et al.  The QCD transition temperature: Results with physical masses in the continuum limit , 2006, hep-lat/0609068.

[28]  W. Weise,et al.  Thermodynamics of the PNJL model , 2006, hep-ph/0609218.

[29]  C. Ratti,et al.  Phases of QCD: lattice thermodynamics and a field theoretical model , 2005, hep-ph/0506234.

[30]  E. Megías,et al.  Polyakov loop in chiral quark models at finite temperature , 2004, Physical Review D.

[31]  K. Fukushima Chiral effective model with the Polyakov loop , 2003, hep-ph/0310121.

[32]  A. Dumitru,et al.  Two-point functions for SU(3) Polyakov loops near T c , 2002, hep-ph/0204223.

[33]  U. Heinz,et al.  Massive gluons and quarks and the equation of state obtained from SU(3) lattice QCD , 1997, hep-ph/9710463.

[34]  M. Asakawa,et al.  What thermodynamics tells us about the QCD plasma , 1997 .