{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.156174.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2878694"}},{"@id":"https://doi.org/10.1103/t5kp-vsv7","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2025","description":"Charged hadron elliptic anisotropies ($v_2$) are presented over a wide transverse momentum ($p_\\text{T}$) range for proton-lead (pPb) and lead-lead (PbPb) collisions at nucleon-nucleon center-of-mass energies of 8.16 and 5.02 TeV, respectively. The data were recorded by the CMS experiment and correspond to integrated luminosities of 186 nb$^{-1}$ and 0.607 nb$^{-1}$ for the pPb and PbPb systems, respectively. A four-particle cumulant analysis is performed using subevents separated in pseudorapidity to effectively suppress non-collective effects. At high $p_\\text{T}$ ($p_\\text{T}$$\\gt$ 8 GeV), significant positive $v_2$ values are observed that are similar between pPb and PbPb collisions at comparable charged particle multiplicities. This observation suggests a common origin for the multi-particle collectivity for high-$p_\\text{T}$ particles in the two systems.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.156174.v1/t1","@type":"Dataset","description":"The elliptic anisotropy $v_2\\{4\\}$ for charged hadron as a function of $p_T$ in pPb collisions at 8.16 TeV in $185...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.156174.v1/t2","@type":"Dataset","description":"The elliptic anisotropy $v_2\\{4\\}$ for charged hadron as a function of $p_T$ in PbPb collisions at 5.02 TeV in $185...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.156174.v1/t3","@type":"Dataset","description":"The elliptic anisotropy $v_2\\{4\\}$ as a function of $p_T$ with 4-subevent method compared between pPb collisions at 8.16 TeV and...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.156174.v1/t4","@type":"Dataset","description":"The elliptic anisotropy $v_2\\{4\\}$ as a function of $\\langle N_{trk}^{offline} \\rangle$ with 4-subevent method compared between pPb collisions at 8.16...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.156174.v1/t5","@type":"Dataset","description":"The elliptic anisotropy $v_2\\{4\\}$ as a function of $\\langle N_{trk}^{corrected} \\rangle$ with 4-subevent method compared between pPb collisions at 8.16...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.156174.v1/t6","@type":"Dataset","description":"The differential cumulant $d_2\\{4\\}$ as a function of $p_T$ in generator level HIJING for $60 \\le N_{trk}^{gen} <120$ are compared...","name":"Table 6"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2878694?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/156174"}],"inLanguage":"en","name":"Evidence for similar collectivity of high transverse momentum particles in pPb and PbPb collisions","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2878694?version=1","version":1}