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 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.

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 Approaching the QCD phase diagram for Nf = 2+1 and Nf = 2 + 1 + 1 quark flavors

2015 ◽  
Vol 599 ◽  
pp. 012015 ◽  
Author(s):  
Christian A Welzbacher ◽  
Christian S Fischer ◽  
Jan Luecker
Keyword(s):  
Phase Diagram ◽  
Qcd Phase Diagram ◽  
Quark Flavors

scholarly journals GAUGE THEORY ON A SPACE WITH LINEAR LIE TYPE FUZZINESS

2013 ◽  
Vol 28 (08) ◽  
pp. 1350021 ◽  
Author(s):  
MOHAMMAD KHORRAMI ◽  
AMIR H. FATOLLAHI ◽  
AHMAD SHARIATI
Keyword(s):  
Gauge Theory ◽  
Standard Model ◽  
Field Strength ◽  
Gauge Field ◽  
Field Component ◽  
Lattice Gauge Theory ◽  
Fourier Space ◽  
Lattice Gauge ◽  
The Standard Model

The U(1) gauge theory on a space with Lie type noncommutativity is constructed. The construction is based on the group of translations in Fourier space, which in contrast to space itself is commutative. In analogy with lattice gauge theory, the object playing the role of flux of field strength per plaquette, as well as the action, is constructed. It is observed that the theory, in comparison with ordinary U(1) gauge theory, has an extra gauge field component. This phenomena is reminiscent of similar ones in formulation of SU (N) gauge theory in space with canonical noncommutativity, and also appearance of gauge field component in discrete direction of Connes' construction of the Standard Model.

The compressed baryonic matter experiment at FAIR

Open Physics ◽  
2012 ◽  
Vol 10 (6) ◽  
Author(s):  
Peter Senger
Keyword(s):  
Phase Diagram ◽  
Phase Transitions ◽  
Equation Of State ◽  
High Energy ◽  
Baryonic Matter ◽  
Lepton Pairs ◽  
Chiral Phase ◽  
Qcd Phase Diagram ◽  
Compressed Baryonic Matter ◽  
Large Acceptance

AbstractThe Compressed Baryonic Matter (CBM) experiment will be one of the major scientific pillars of the future Facility for Antiproton and Ion Research (FAIR) in Darmstadt. The goal of the CBM research program is to explore the QCD phase diagram in the region of high baryon densities using high-energy nucleus-nucleus collisions. This includes the study of the equation-of-state of nuclear matter at high densities, and the search for the deconfinement and chiral phase transitions. The CBM detector is designed to measure both bulk observables with large acceptance and rare diagnostic probes such as charmed particles and vector mesons decaying into lepton pairs.

scholarly journals EVOLUTION OF THE STRUCTURE FACTORS IN PURE SU(N) LATTICE GAUGE THEORY AND EFFECTIVE SPIN MODELS

2005 ◽  
Vol 20 (15) ◽  
pp. 3459-3468 ◽  
Author(s):  
ALEXEI BAZAVOV ◽  
BERND A. BERG ◽  
ALEXANDER VELYTSKY
Keyword(s):  
Gauge Theory ◽  
Rapid Heating ◽  
Lattice Gauge Theory ◽  
Debye Screening ◽  
Spin Models ◽  
Effective Spin ◽  
Mass Estimation ◽  
Qcd Vacuum ◽  
Lattice Gauge ◽  
Structure Factors

We consider model A dynamics for a quench from the disordered into the ordered phase of SU (3) lattice gauge theory and the analogue 3d 3-state Potts model. For the gauge model this corresponds to a rapid heating from the confined to the deconfined phase. The exponential growth factors of low-lying structure function modes are numerically calculated. The linear theory of spinodal decomposition is used to determine the critical modes. This allows for the Debye screening mass estimation in an effective phenomeno-logical model. The quench leads to competing vacuum domains, which make the equilibration of the QCD vacuum after the heating non-trivial. The influence of such domains on the gluonic energy density is studied.

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