{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.93057.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1743581"}},{"@id":"https://doi.org/10.1140/epjc/s10052-019-7489-6","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2020","description":"CERN-LHC. To assess the properties of the quark\u2013gluon plasma formed in ultrarelativistic ion collisions, the ATLAS experiment at the LHC measures a correlation between the mean transverse momentum and the flow harmonics. The analysis uses data samples of lead--lead and proton--lead collisions obtained at the centre-of-mass energy per nucleon pair of 5.02~TeV, corresponding to total integrated luminosities of $22~\\mu\\text{b}^{-1}$ and $28~\\text{nb}^{-1}$, respectively. The measurement is performed using a modified Pearson correlation coefficient with the charged-particle tracks on an event-by-event basis. The modified Pearson correlation coefficients for the 2$^{\\mathrm{nd}}$-, 3$^{\\mathrm{rd}}$-, and 4$^{\\mathrm{th}}$-order flow harmonics are measured in the lead--lead collisions as a function of event centrality quantified as the number of charged particles or the number of nucleons participating in the collision. The measurements are performed for several intervals of the charged-particle transverse momentum. The correlation coefficients for all studied harmonics exhibit a strong centrality evolution, which only weakly depends on the charged-particle momentum range. In the proton--lead collisions, the modified Pearson correlation coefficient measured for the 2$^{\\mathrm{nd}}$-order flow harmonics shows only weak centrality dependence. The lead-lead data is qualitatively described by the predictions based on the hydrodynamical model.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.93057.v1/t1","@type":"Dataset","description":"The $c_{k}$ for the 0.5-2 GeV $p_{T}$ range as a function of event multiplicity $N_{ch}$ in Pb+Pb collisions.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.93057.v1/t2","@type":"Dataset","description":"The $c_{k}$ for the 0.5-5 GeV $p_{T}$ range as a function of event multiplicity $N_{ch}$ in Pb+Pb collisions.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.93057.v1/t3","@type":"Dataset","description":"The $c_{k}$ for the 1-2 GeV $p_{T}$ range as a function of event multiplicity $N_{ch}$ in Pb+Pb collisions.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.93057.v1/t4","@type":"Dataset","description":"The $c_{k}$ for the 0.3-2 GeV $p_{T}$ range as a function of event multiplicity $N_{ch}$ in p+Pb collisions.","name":"Table 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