{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.165859.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2848254"}},{"@id":"https://doi.org/10.1038/s41467-025-67795-1","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2025","description":"$p_{\\mathrm{T}}$-differential $v_2$ measured with the two-particle correlation method for mesons ($\\mathrm{\\pi}^{\\pm}, \\mathrm{K}^{\\pm}, \\mathrm{K_{S}^{0}}$) and baryons ($\\mathrm{p}(\\bar{\\mathrm{p}}), \\Lambda(\\bar{\\Lambda})$) in high-multiplicity p--Pb collisions at $\\sqrt{s_{\\mathrm{NN}}} = 5.02$ TeV and pp collisions at $\\sqrt{s} = 13$ TeV. The multiplicity, $\\langle N_{\\rm ch} \\rangle$, represents the average number of reconstructed, efficiency-corrected charged particles with transverse momentum in the range $0.2 &lt; p_{\\rm T} &lt; 3.0$ GeV/$c$, measured at midrapidity ($|\\eta| &lt; 0.8$). This work demonstrates the distinctive grouping of anisotropic flow for baryons and mesons in high-multiplicity proton--lead and proton--proton collisions at the Large Hadron Collider (LHC).","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.165859.v1/t1","@type":"Dataset","description":"$v_2${2, $1.1&lt;|\\Delta\\eta|&lt; 7.8$} of $\\mathrm{\\pi}^{\\pm}$ as a function of $p_{\\mathrm{T}}$ in high-multiplicity p--Pb collisions at $\\sqrt{s_{\\mathrm{NN}}} = 5.02$ TeV.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.165859.v1/t2","@type":"Dataset","description":"$v_2${2, $1.1&lt;|\\Delta\\eta|&lt; 7.8$} of $\\mathrm{K}^{\\pm}$ as a function of $p_{\\mathrm{T}}$ in high-multiplicity p--Pb collisions at $\\sqrt{s_{\\mathrm{NN}}} = 5.02$ TeV.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.165859.v1/t3","@type":"Dataset","description":"$v_2${2, $1.1&lt;|\\Delta\\eta|&lt; 7.8$} of p + $\\rm\\overline p$ as a function of $p_{\\mathrm{T}}$ in high-multiplicity p--Pb collisions at $\\sqrt{s_{\\mathrm{NN}}} =...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.165859.v1/t4","@type":"Dataset","description":"$v_2${2, $1.1&lt;|\\Delta\\eta|&lt; 7.8$} of $\\rm K^0_\\rm S$ as a function of $p_{\\mathrm{T}}$ in high-multiplicity p--Pb collisions at $\\sqrt{s_{\\mathrm{NN}}} = 5.02$...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.165859.v1/t5","@type":"Dataset","description":"$v_2${2, $1.1&lt;|\\Delta\\eta|&lt; 7.8$} of $\\Lambda$ + $\\overline \\Lambda$ as a function of $p_{\\mathrm{T}}$ in high-multiplicity p--Pb collisions at $\\sqrt{s_{\\mathrm{NN}}} =...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.165859.v1/t6","@type":"Dataset","description":"$v_2${2, $1.1&lt;|\\Delta\\eta|&lt; 6.4$} of $\\mathrm{\\pi}^{\\pm}$ as a function of $p_{\\mathrm{T}}$ in high-multiplicity pp collisions at $\\sqrt{s_{\\mathrm{NN}}} = 13$ TeV.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.165859.v1/t7","@type":"Dataset","description":"$v_2${2, $1.1&lt;|\\Delta\\eta|&lt; 6.4$} of $\\rm K^+$ + $\\rm K^-$ as a function of $p_{\\mathrm{T}}$ in high-multiplicity pp collisions at $\\sqrt{s_{\\mathrm{NN}}}...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.165859.v1/t8","@type":"Dataset","description":"$v_2${2, $1.1&lt;|\\Delta\\eta|&lt; 6.4$} of p + $\\rm\\overline p$ as a function of $p_{\\mathrm{T}}$ in high-multiplicity pp collisions at $\\sqrt{s_{\\mathrm{NN}}} =...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.165859.v1/t9","@type":"Dataset","description":"$v_2${2, $1.1&lt;|\\Delta\\eta|&lt; 6.4$} of $\\rm K^0_\\rm S$ as a function of $p_{\\mathrm{T}}$ in high-multiplicity pp collisions at $\\sqrt{s_{\\mathrm{NN}}} = 13$...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.165859.v1/t10","@type":"Dataset","description":"$v_2${2, $1.1&lt;|\\Delta\\eta|&lt; 6.4$} of $\\Lambda$ + $\\overline \\Lambda$ as a function of $p_{\\mathrm{T}}$ in high-multiplicity pp collisions at $\\sqrt{s_{\\mathrm{NN}}} =...","name":"Table 10"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2848254?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/165859"}],"inLanguage":"en","name":"Observation of partonic flow in proton-proton and proton-nucleus collisions","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2848254?version=1","version":1}
