{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.146740.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2784422"}},{"@id":"https://doi.org/10.1140/epjc/s10052-024-13243-1","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2024","description":"Properties of the underlying-event in $pp$ interactions are investigated primarily via the strange hadrons $K_{S}^{0}$, $\\Lambda$ and $\\bar\\Lambda$, \nas reconstructed using the ATLAS detector at the LHC in minimum-bias $pp$ collision data at $\\sqrt{s} = 13$ TeV.\nThe hadrons are reconstructed via the identification of the displaced two-particle vertices corresponding to the decay modes $K_{S}^{0}\\rightarrow\\pi^+\\pi^-$, \n$\\Lambda\\rightarrow\\pi^-p$ and $\\bar\\Lambda\\rightarrow\\pi^+\\bar{p}$. \nThese are used in the construction of underlying-event observables in azimuthal regions computed relative to the leading charged-particle jet in the event.\nEvents with a leading charged-particle jet in the range of $10 < p_{T} \\leq 40$ GeV are studied using the number of prompt charged particles in the transverse region.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.146740.v1/t1","@type":"Dataset","description":"Mean multiplicity of $K^{0}_{S}$ per unit $(\\eta, \\phi)$ in the away region vs. leading-jet $p_{T}$","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.146740.v1/t2","@type":"Dataset","description":"Statistical covariance between bins of Table 1","name":"Table 1 Covariance"},{"@id":"https://doi.org/10.17182/hepdata.146740.v1/t3","@type":"Dataset","description":"Mean multiplicity of $K^{0}_{S}$ per unit $(\\eta, \\phi)$ in the towards region vs. leading-jet $p_{T}$","name":"Table 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