Centrality-dependent chemical potentials of light hadrons and quarks based on transverse momentum spectra and particle yield ratios in Au-Au collisions

TL;DR

This study analyzes transverse momentum spectra and particle yield ratios in Au-Au collisions to extract chemical potentials of light hadrons and quarks, revealing energy-dependent behaviors and potential phase transition signals.

Contribution

It introduces a two-component Erlang distribution to fit spectra and derives chemical potentials from yield ratios across energies and centralities, highlighting a possible critical energy for phase transition.

Findings

Chemical potentials decrease with increasing collision energy.

Yield ratios show linear dependence on 1/√s_NN.

A potential phase transition point at 3.526 GeV.

Abstract

We describe the transverse momentum spectra of $\pi^\pm$, $K^\pm$, $p$, and $\bar{p}$ produced in different centralities gold-gold (Au-Au) collisions at different collision energies range from 7.7 to 62.4 GeV by a two-component Erlang distribution. The fitting results are consistent with the experimental data, and the centrality- and energy-dependent yield ratios of negative to positive particles are obtained from the normalization constants. Based on the yield ratios, the energy- and centrality-dependent chemical potentials of light hadrons and quarks are extracted. The study shows that the dependences of the three types of particle yield ratios on centrality are not significant, especially for $\pi$. The logarithms of the three yield ratios show obvious linear dependence on $1/\sqrt{s_{NN}}$ over a range from 7.7 to 62.4 GeV. The extracted chemical potentials show obvious dependence on energy, and decrease with the increase of energy. The dependences of the energy-dependent chemical potentials of light hadrons and quarks on centrality are relatively more obvious in low energy region. The derived curves of chemical potentials for all centralities, from the linear fits of the logarithms of yield ratios vs energy, have the extremum at the same energy of 3.526 GeV, which possibly is the critical energy of phase transition from a liquid-like hadron state to a gas-like quark state in the collision system. With the increase of energy, all types of chemical potentials become small and tend to zero at very high energy, which indicates that with the increase of energy, the hadronic interactions gradually fade and the partonic interactions gradually become greater.