{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.94802.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1762209"}},{"@id":"https://doi.org/10.1140/epjc/s10052-020-7624-4","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2020","description":"The two-particle azimuthal anisotropy coefficients, $v_{2}$ and $v_{3}$ are measured in $p$+Pb collisions at $\\sqrt{s_{NN}}=8.16$ TeV with the ATLAS detector at the Large Hadron Collider using a dataset with an integrated luminosity of 165 nb$^{\u22121}$ recorded in 2016. The results are shown as a function of particle $p_\\mathrm{T}$ and collision centrality. In addition to measurements in minimum bias events, results are shown from events selected by the presence of a high $p_\\mathrm{T}$ jet; this selection enhances the statistics of high $p_\\mathrm{T}$ particles. Furthermore, assuming a two componant model of particle production (from Hard Scatterings or from the Underlying Event), the relative contribution of particle pairs is determined for each of the four combinations.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.94802.v1/t1","@type":"Dataset","description":"Distribution of $v_{2}$ from MBT events plotted as a function of the A-particle $p_\\mathrm{T}$ for 0-5% centrality.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.94802.v1/t2","@type":"Dataset","description":"Distribution of $v_{2}$ from $p_{T}^{jet}>75$ GeV events plotted as a function of the A-particle $p_\\mathrm{T}$ for 0-5% centrality.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.94802.v1/t3","@type":"Dataset","description":"Distribution of $v_{2}$ from $p_{T}^{jet}>100$ GeV events plotted as a function of the A-particle $p_\\mathrm{T}$ for 0-5% centrality.","name":"Table 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