Abstract

Like fluctuations, non-diagonal correlators of conserved charges provide a tool for the study of chemical freeze-out in heavy ion collisions. They can be calculated in thermal equilibrium using lattice simulations, and be connected to moments of event-by-event net-particle multiplicity distributions. We calculate them from continuum extrapolated lattice simulations at $\mu_B=0$, and present a finite-$\mu_B$ extrapolation, comparing two different methods. In order to relate the grand canonical observables to the experimentally available net-particle fluctuations and correlations, we perform a Hadron Resonance Gas (HRG) model analysis, which allows us to completely break down the contributions from different hadrons. We then construct suitable hadronic proxies for fluctuations ratios, and study their behavior at finite chemical potentials. We also study the effect of introducing acceptance cuts, and argue that the small dependence of certain ratios on the latter allows for a direct comparison with lattice QCD results, provided that the same cuts are applied to all hadronic species. Finally, we perform a comparison for the constructed quantities for experimentally available measurements from the STAR Collaboration. Thus, we estimate the chemical freeze-out temperature to 165 MeV using a strangeness-related proxy. This is a rather high temperature for the use of the Hadron Resonance Gas, thus, further lattice studies are necessary to provide first principle results at intermediate $\mu_B$.

Highlights

  • The study of the phase diagram of quantum chromodynamics (QCD) has been the object of intense effort from both theory and experiment in the last decades

  • We study the effect of introducing acceptance cuts, and argue that the small dependence of certain ratios on the latter allows for a direct comparison with lattice QCD results, provided that the same cuts are applied to all hadronic species

  • The transition from a hadron gas to a deconfined quark gluon plasma (QGP) was shown by lattice QCD calculations to be a broad crossover [1] at T ≃ 155 MeV [1,2,3,4]

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Summary

Pásztor

Nondiagonal correlators of conserved charges provide a tool for the study of chemical freeze-out in heavy ion collisions. They can be calculated in thermal equilibrium using lattice simulations, and be connected to moments of event-by-event net-particle multiplicity distributions. In order to relate the grand canonical observables to the experimentally available netparticle fluctuations and correlations, we perform a hadron resonance gas model analysis, which allows us to completely break down the contributions from different hadrons. We estimate the chemical freeze-out temperature to 165 MeV using a strangeness-related proxy This is a rather high temperature for the use of the hadron resonance gas; further lattice studies are necessary to provide first principle results at intermediate μB

INTRODUCTION
LATTICE QCD AND THE GRAND CANONICAL ENSEMBLE
RESULTS
Taylor method
Sector method
CORRELATORS IN THE HRG MODEL
Correlators of measured particle species
Breakdown of the measured and nonmeasured contributions
Isospin randomization
PROXIES
FINITE CHEMICAL POTENTIAL AND KINEMATIC CUTS
COMPARISON TO EXPERIMENTAL RESULTS
VIII. CONCLUSIONS
Full Text
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