Event-by-Event Particle Ratio Fluctuations at LHC Energies

TL;DR

This Monte Carlo study investigates particle ratio fluctuations at LHC energies using the extit{hij} model, finding that fluctuation measures depend mainly on charged particle density across different collision systems and energies.

Contribution

It introduces a detailed simulation analysis of event-by-event particle ratio fluctuations at LHC energies, comparing model predictions with experimental data and exploring dependence on system size and particle density.

Findings

Model predictions agree with experimental data for central collisions.

Fluctuation measures scale with charged particle density across systems.

Deviations observed in peripheral collisions and low pT regions.

Abstract

A Monte Carlo study of identified particle ratio fluctuations at LHC energies is carried out in the frame work of \hij model using the fluctuation variable $\nu_{dyn}$. The simulated events for Pb-Pb collisions at $\sqrt{s}_{NN}$ = 2.76 and 5.02 TeV and Xe-Xe collisions at $\sqrt{s}_{NN}$ = 5.44 TeV are analyzed. From this study, it is observed that the values of $[\pi,K]$, $[p,K]$ and $[\pi,p]$ follow the similar trends of energy dependence as observed in the most central collision data by NA49, STAR and ALICE experiments. It is also observed that $\nu_{dyn}$ for all the three combinations of particles for semi-central and central collisions, the model predicted values of $\nu_{dyn}[A,B]$ for Pb-Pb collisions at $\sqrt{s}_{NN}$ = 2.76 TeV agree fairly well with those observed in ALICE experiment. For peripheral collisions, however, the model predicted values of $\nu_{dyn}[\pi,K]$ are somewhat smaller, whereas for $[p,K]$ and $[\pi,p]$ it predicts larger values as compared to the corresponding experimental values. The possible reasons for the observed differences are discussed. The $\nu_{dyn}$ values scaled with charged particle density when plotted against $\langle$N$_{part}$$\rangle$, exhibit a flat behaviour, as expected from the independent particle emission sources. For $[p,K]$ and $[\pi,p]$ combinations, a departure from the flat trend is, however, observed in central collisions in the case of low p$_{T}$ window when effect of jet quenching or resonances are considered. Furthermore, the study of $\nu_{dyn}[A,B]$ dependence on particle density for various collision systems (including proton-proton collisions) suggests that at LHC energies $\nu_{dyn}$ values for a given particle pair is simply a function of charged particle density, irrespective of system size, beam energy and collision centrality.