2012/07/08 by R. Lacey, Roy A. Lacey, Yi Gu +15
Mathematics · Physics and Astronomy · #High-Energy Particle Collisions Research #Quantum Chromodynamics and Particle Interactions #Stochastic processes and statistical mechanics #nucl-ex #nucl-th
paper · pdf · doi:10.48550/arxiv.1207.1886
4 pages, 4 figures. Submitted for publication (Typos corrected in this version)
arxiv created 2012/07/14 · arxiv updated 2012/07/17
The anisotropy coefficient v2, for unidentified and identified charged hadrons [pions (π), kaons (K) and protons (p)] measured in Au+Au collisions at √sNN= 0.20 TeV (RHIC) and Pb+Pb collisions at √sNN= 2.76 TeV (LHC), are compared for several collision centralities (cent) and particle transverse momenta pT. In contrast to the measurements for charged hadrons, the comparisons indicate a sizable increase of v2(pT) for π,K and p, as well as a blueshift of proton v2(pT), from RHIC to LHC. When this blueshift is accounted for, the LHC data [for π, K, p] show excellent scaling of v2(KET) with the number of valence quarks (nq), for a broad range of transverse kinetic energies (KET) and collision centralities. These observations suggest a larger mean sound speed <cs(T)> for the plasma created in LHC collisions, and significant radial flow generation after its hadronization.