Contrasting Features of Parton Energy Loss in Heavy-ion Collisions at RHIC and the LHC

TL;DR

This paper compares parton energy loss in heavy-ion collisions at RHIC and LHC, revealing different energy loss mechanisms and their dependence on medium density and particle transverse momentum.

Contribution

It identifies a transition from collisional to radiative energy loss dominance from RHIC to LHC energies based on $R_{AA}$ behavior and $p_T$ dependence.

Findings

$R_{AA}$ at LHC shows a $p_T$ dependence consistent with $\

Delta p_T$ proportional to $\

radiative energy loss dominates at LHC, while collisional dominates at RHIC.

Abstract

Energetic quarks and gluons lose energy as they traverse the hot and dense medium created in high-energy heavy-ion collisions at the BNL Relativistic Heavy Ion Collider (RHIC) and the CERN Large Hadron Collider (LHC). The nuclear modification factor ($R_{AA}$) of leading particles quantifies parton energy loss in such collisions, with the particle spectrum in $p+p$ collisions as a reference. Previous $R_{AA}$ measurements at RHIC energies have revealed an approximately constant trend at high transverse momenta ($p_{T}$), implying a scenario where parton energy loss, $\Delta p_{T}$, scales proportionally with $p_{T}$, a feature naively expected from energy loss dynamics in elastic collisions. In this study, we investigate the LHC $R_{AA}$ measurements which exhibit a pronounced $p_{T}$ dependence of $R_{AA}$ for various particle species, and our analysis attributes this behavior to $\Delta p_T$ being approximately proportional to $\sqrt{p_{T}}$. These distinct features are consistent with model calculations of dominant radiative energy loss dynamics at the LHC, in contrast to the dominance of collisional energy loss at RHIC. Additionally, the linear increase of fractional energy loss with medium density at different $p_{T}$ magnitudes affirms the previous empirical observation that the magnitude of the energy loss depends mostly on the initial entropy density, with no significant path-length dependence. Implications on the dynamical scenarios of parton energy loss and future experimental investigations will also be discussed.