Abstract

In this work, we have studied the isothermal compressibility ($\kappa_T$) as a function of temperature, baryon chemical potential and centre-of-mass energy ($\sqrt{s_{NN}}$) using hadron resonance gas (HRG) and excluded-volume hadron resonance gas (EV-HRG) models. A mass cut-off dependence of isothermal compressibility has been studied for a physical resonance gas. Further, we study the effect of heavier resonances ($>$ 2 GeV) on the isothermal compressibility by considering the Hagedorn mass spectrum, ${\rho}(m)\sim{\exp(bm)}/{(m^2+m_0^2)^{5/4}}$. Here, the parameters, $b$ and $m_0$ are extracted after comparing the results of recent lattice QCD simulations at finite baryonic chemical potential. We find a significant difference between the results obtained in EV-HRG and HRG models at a higher temperatures and higher baryochemical potentials. The inclusion of the Hagedorn mass spectrum in the partition function for hadron gas has a large effect at a higher temperature. A higher mass cut-off in the Hagedorn mass spectrum takes the isothermal compressibility to a minimum value, which occurs near the Hagedorn temperature ($T_H$). We show explicitly that at the future low energy accelerator facilities like FAIR (CBM), Darmstadt and NICA, Dubna the created matter would be incompressible compared to the high energy facilities like RHIC and LHC.

Highlights

  • Ultrarelativistic heavy-ion colliders such as the Relativistic Heavy Ion Collider (RHIC) and Large Hadron Collider (LHC) aim to produce matter at extreme conditions of temperature and/or energy density, where a phase transition is expected to take place from colorless hadronic matter to a colored phase of quarks and gluons known as quark-gluon plasma (QGP)

  • We describe an equation of state for the hadron gas (HG) based on the excluded-volume correction [24], where a hard-core size is assigned to all the baryons while mesons are treated as pointlike particles in the grand-canonical partition function

  • We have explicitly calculated the change in number density in the hadron resonance gas (HRG) model with μB = 0.5 GeV at T = 0.170 GeV for various mass cut-offs

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Summary

INTRODUCTION

Ultrarelativistic heavy-ion colliders such as the Relativistic Heavy Ion Collider (RHIC) and Large Hadron Collider (LHC) aim to produce matter at extreme conditions of temperature and/or energy density, where a phase transition is expected to take place from colorless hadronic matter to a colored phase of quarks and gluons known as quark-gluon plasma (QGP). When HRG is used to study the phase transition from hadron gas (HG) to QGP phase using Gibbs construction, an anomalous reversal of phase from QGP to HG is observed at large baryon chemical potential and/or temperature [24] This ambiguity is removed by giving a hard-core size to each baryon which results in strong repulsive interactions between a pair of baryons or antibaryons. A similar decrease is found in the shear viscosity–to– entropy ratio (η/s) when comparing the results obtained with HS [38,40,43,44] These findings prompt us to carry out a study of effect of Hagedorn mass spectrum on isothermal compressibility (κT ) of a hadron gas at very high temperature.

METHODOLOGY
Hadron resonance gas model
Excluded-volume hadron resonance gas Model
Hagedorn mass spectrum
RESULTS AND DISCUSSION
SUMMARY AND CONCLUSIONS
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