Scaling properties of fractional momentum loss of high-pT hadrons in nucleus-nucleus collisions at $\sqrt{s_{_{NN}}}$ from 62.4 GeV to 2.76 TeV
A. Adare, S. Afanasiev, C. Aidala, N.N. Ajitanand, Y. Akiba, R., Akimoto, H. Al-Bataineh, J. Alexander, M. Alfred, H. Al-Ta'ani, A. Angerami,, K. Aoki, N. Apadula, L. Aphecetche, Y. Aramaki, R. Armendariz, S.H. Aronson,, J. Asai, H. Asano, E.C. Aschenauer, E.T. Atomssa

TL;DR
This paper investigates how the fractional momentum loss of high-pT hadrons in heavy ion collisions scales with various collision parameters, revealing common patterns at high energies that shed light on parton energy loss mechanisms.
Contribution
It introduces a detailed analysis of the scaling properties of fractional momentum loss across different energies and collision systems, highlighting universal behaviors at high particle densities.
Findings
$S_{loss}$ follows a power-law with multiple variables above its maximum.
At high energies and densities, $S_{loss}$ scales universally with $dN_{ch}/d a$ and $ E_{Bj} au_0$.
The $p_T$ at maximum $S_{loss}$ varies with centrality and energy.
Abstract
Measurements of the fractional momentum loss () of high-transverse-momentum-identified hadrons in heavy ion collisions are presented. Using in AuAu and CuCu collisions at and 200 GeV measured by the PHENIX experiment at the Relativistic Heavy Ion Collider and and charged hadrons in PbPb collisions measured by the ALICE experiment at the Large Hadron Collider, we studied the scaling properties of as a function of a number of variables: the number of participants, , the number of quark participants, , the charged-particle density, , and the Bjorken energy density times the equilibration time, . We find that the where has its maximum, varies both with centrality and collision energy. Above the maximum,…
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