scholarly journals Role of vector interaction and axial anomaly in the PNJL modeling of the QCD phase diagram

2013 ◽  
Vol 719 (1-3) ◽  
pp. 131-135 ◽  
Author(s):  
Nino Bratovic ◽  
Tetsuo Hatsuda ◽  
Wolfram Weise
Keyword(s):  
Phase Diagram ◽  
Axial Anomaly ◽  
Qcd Phase Diagram ◽  
Vector Interaction

scholarly journals Updates on the QCD phase diagram from lattice

2021 ◽  
Vol 31 (1) ◽  
Author(s):  
Sayantan Sharma
Keyword(s):  
Phase Diagram ◽  
Lattice Gauge Theory ◽  
Topological Properties ◽  
Chiral Phase ◽  
Qcd Phase Diagram ◽  
Qcd Vacuum ◽  
Lattice Gauge ◽  
Massless Quark ◽  
Quark Flavors

AbstractDifferent aspects of the phase diagram of strongly interacting matter described by quantum chromodynamics (QCD), which have emerged from the recent studies using lattice gauge theory techniques, are discussed. A special emphasis is given on understanding the role of the anomalous axial U(1) symmetry in determining the order of the finite temperature chiral phase transition in QCD with two massless quark flavors and tracing its origin to the topological properties of the QCD vacuum.

scholarly journals The QCD Phase-Diagram Obtained from the NJL and the Extended-NJL Models for Quark and Hadron Phases

2017 ◽  
Vol 45 ◽  
pp. 1760059
Author(s):  
Clebson A. Graeff ◽  
Débora P. Menezes
Keyword(s):  
Phase Transition ◽  
Phase Diagram ◽  
Equations Of State ◽  
Original Formulation ◽  
Qcd Phase Diagram ◽  
Hadron Phase ◽  
Vector Interaction ◽  
Njl Model ◽  
Quark Phase

We analyse the hadron/quark phase transition described by the Nambu-Jona-Lasinio (NJL) model [quark phase] and the extended Nambu-Jona-Lasinio model (eNJL) [hadron phase]. While the original formulation of the NJL model is not capable of describing hadronic properties due to its lack of confinement, it can be extended with a scalar-vector interaction so it exhibits this property, the so-called eNJL model. As part of this analysis, we obtain the equations of state within the SU(2) versions of both models for the hadron and the quark phases and determine the binodal surface.

More on the QCD phase diagram at finite temperatures

1988 ◽  
Vol 38 (10) ◽  
pp. 3266-3276 ◽  
Author(s):  
R. V. Gavai ◽  
J. Potvin ◽  
S. Sanielevici
Keyword(s):  
Phase Diagram ◽  
Qcd Phase Diagram

scholarly journals Universal Off-Equilibrium Scaling of Critical Cumulants in the QCD Phase Diagram

2016 ◽  
Vol 117 (22) ◽  
Author(s):  
Swagato Mukherjee ◽  
Raju Venugopalan ◽  
Yi Yin
Keyword(s):  
Phase Diagram ◽  
Qcd Phase Diagram

scholarly journals Mass and radius constraints for compact stars and the QCD phase diagram

2014 ◽  
Vol 496 ◽  
pp. 012002 ◽  
Author(s):  
David B Blaschke ◽  
Hovik A Grigorian ◽  
David E Alvarez-Castillo ◽  
Alexander S Ayriyan
Keyword(s):  
Phase Diagram ◽  
Compact Stars ◽  
Qcd Phase Diagram

scholarly journals On SU(3) Effective Models and Chiral Phase Transition

2015 ◽  
Vol 2015 ◽  
pp. 1-15 ◽  
Author(s):  
Abdel Nasser Tawfik ◽  
Niseem Magdy
Keyword(s):  
Phase Transition ◽  
Phase Diagram ◽  
Lattice Qcd ◽  
High Energy ◽  
Particle Model ◽  
Chiral Phase ◽  
Chiral Phase Transition ◽  
Thermal Models ◽  
Qcd Phase Diagram ◽  
Freeze Out

Sensitivity of Polyakov Nambu-Jona-Lasinio (PNJL) model and Polyakov linear sigma-model (PLSM) has been utilized in studying QCD phase-diagram. From quasi-particle model (QPM) a gluonic sector is integrated into LSM. The hadron resonance gas (HRG) model is used in calculating the thermal and dense dependence of quark-antiquark condensate. We review these four models with respect to their descriptions for the chiral phase transition. We analyze the chiral order parameter, normalized net-strange condensate, and chiral phase-diagram and compare the results with recent lattice calculations. We find that PLSM chiral boundary is located in upper band of the lattice QCD calculations and agree well with the freeze-out results deduced from various high-energy experiments and thermal models. Also, we find that the chiral temperature calculated from HRG is larger than that from PLSM. This is also larger than the freeze-out temperatures calculated in lattice QCD and deduced from experiments and thermal models. The corresponding temperature and chemical potential are very similar to that of PLSM. Although the results from PNJL and QLSM keep the same behavior, their chiral temperature is higher than that of PLSM and HRG. This might be interpreted due the very heavy quark masses implemented in both models.

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