Abstract
We present the next-to-leading-order event-by-event EKRT model predictions for the centrality dependence of the charged hadron multiplicity in the pseudorapidity interval $|\eta|\le 0.5$, and for the centrality dependence of the charged hadron flow harmonics $v_n\{2\}$ obtained from 2-particle cumulants, in $\sqrt{s_{NN}}=5.44$ TeV Xe+Xe collisions at the CERN Large Hadron Collider. Our prediction for the 0-5 \% central charged multiplicity is $dN_{\rm ch}/d\eta =1218\pm 46$. We also predict $v_n\{2\}$ in Xe+Xe collisions to increase more slowly from central towards peripheral collisions than those in a Pb+Pb system. We find that at $10 \dots 50$\% centralities $v_2\{2\}$ is smaller and $v_3\{2\}$ is larger than in the Pb+Pb system while $v_4\{2\}$ is of the same magnitude in both systems. We also find that the ratio of flow harmonics in Xe+Xe collisions and in Pb+Pb collisions shows a slight sensitivity to the temperature dependence of the shear-viscosity-to-entropy ratio. As we discuss here, the new nuclear mass-number systematics especially in the flow harmonics serves as a welcome further constraint for describing the space-time evolution of a heavy-ion system and for determining the shear viscosity and other transport properties of strongly interacting matter.
Highlights
Ultrarelativistic heavy-ion collisions at the CERN Large Hadron Collider (LHC) and BNL Relativistic Heavy Ion Collider (RHIC) probe the collectivity in quantum chromodynamics (QCD) by producing strongly interacting QCD matter at high temperatures and vanishing net-baryon number densities
We present the event-by-event next-to-leading-order perturbative-QCD + saturation + viscous hydrodynamics (EKRT) model predictions for the centrality dependence of the charged hadron multiplicity in the pseudorapidity interval |η| 0.5, and for the from two-particle cumulants, in c√esnNtrNal=ity5d.4e4peTnedVenXcee+oXf ethceolclihsaiorgnesdathtahderoCnERfloNwLhaargrme HonaidcrsonvnC{2o}lliodbetra.iOneudr prediction for the 0–5 % central charged multiplicity is dNch/dη = 1218 ± 46
We find that the ratio of flow harmonics in Xe+Xe collisions and in Pb+Pb collisions shows a slight sensitivity to the temperature dependence of the shear-viscosity–to–entropy ratio
Summary
Ultrarelativistic heavy-ion collisions at the CERN Large Hadron Collider (LHC) and BNL Relativistic Heavy Ion Collider (RHIC) probe the collectivity in quantum chromodynamics (QCD) by producing strongly interacting QCD matter at high temperatures and vanishing net-baryon number densities. On the one hand, one needs QCD-based predictive modeling to describe the production of the system at various collision energies and nuclei [1,2,3,4,5,6,7,8,9,10,11] Combining this with a fluid-dynamical spacetime evolution, event by event, enables the computation of a multitude of small transverse-momentum (pT ) finalstate observables [12,13,14,15,16,17,18,19,20,21,22,23].
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