Abstract

The behavior of strange matter in the frame of the SU(3) Polyakov-loop extended Nambu--Jona-Lasinio (PNJL) model including the ${U}_{A}(1)$ anomaly is considered. We discuss the appearance of a peak in the ratio of the number of strange mesons to nonstrange mesons known as the ``horn.'' The PNJL model gives a schematic description of the chiral phase transition and meson properties at finite temperature and density. By using the model, we can show that the splitting of kaon and antikaon masses appears as a result of the introduction of density. This may explain the difference in the ${K}^{+}/{\ensuremath{\pi}}^{+}$ ratio and the ${K}^{\ensuremath{-}}/{\ensuremath{\pi}}^{\ensuremath{-}}$ ratio at low $\sqrt{{s}_{NN}}$ and their tendency to the same value at high $\sqrt{{s}_{NN}}$. We also show that the rise in the ratio ${K}^{+}/{\ensuremath{\pi}}^{+}$ appears near the critical endpoint when we build the ${K}^{+}/{\ensuremath{\pi}}^{+}$ ratio along the phase-transition diagram and it can be considered as a critical region signal.

Highlights

  • The study of matter formed during the collision of heavy ions at high energies is currently of significant interest in highenergy physics

  • The strangeness enhancement in heavy-ion collisions has been suggested as the quark-gluon plasma (QGP) signal long ago [44,45]

  • The reason is that the probability of the process gg → ssin QGP increases due the high density of gluons and due the chiral symmetry restoration in the strange sector (s mass becomes lower)

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Summary

INTRODUCTION

The study of matter formed during the collision of heavy ions at high energies is currently of significant interest in highenergy physics. Investigations at energies from 7 to 200 AGeV were made by the (Relativistic Heavy Ion Collider Beam Energy Scan) [2] and it was shown that the data can be placed on the same curve [1,3,4,5] Such enhancement was observed in the ratio of other positive charged strange particles to the positive charged nonstrange pions. The microscopic transport model that includes only the hadron phase and does not include the quark-gluon phase cannot reproduce experimental data [8,9,10,11,12] and, as a result, in the works [3,13] the authors suggest that such a peak in the ratio can be explained as the onset of deconfinement. The effective potential U ( , ̄ ; T ) depends on temperature T , the Polyakov loop field and its complex conjugate , which can be obtained through the expectation value of the Polyakov line [23,24]:

Nc Trc
FINITE BARYON DENSITY
CONCLUSION
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