{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.76506.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1471287"}},{"@id":"https://doi.org/10.1016/j.physletb.2016.12.009","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2017","description":"CERN-LHC.  Measurements of two- and multi-particle angular correlations in pp collisions at sqrt(s) = 5, 7, and 13 TeV are presented as a function of charged-particle multiplicity. The data, corresponding to integrated luminosities of 1.0 inverse picobarn (5 TeV), 6.2 inverse picobarns (7 TeV), and 0.7 inverse picobarns (13 TeV), were collected using the CMS detector at the LHC. The second-order (v[2]) and third-order (v[3]) azimuthal anisotropy harmonics of unidentified charged particles, as well as v[2] of K0 short and Lambda/anti-Lambda particles, are extracted from long-range two-particle correlations as functions of particle multiplicity and transverse momentum. For high-multiplicity pp events, a mass ordering is observed for the v[2] values of charged hadrons (mostly pions), K0 short, and Lambda/anti-Lambda, with lighter particle species exhibiting a stronger azimuthal anisotropy signal below pt of about 2 GeV/c. For 13 TeV data, the v[2] signals are also extracted from four- and six-particle correlations for the first time in pp collisions, with comparable magnitude to those from two-particle correlations. These observations are similar to those seen in pPb and PbPb collisions, and support the interpretation of a collective origin for the observed long-range correlations in high-multiplicity pp collisions.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.76506.v1/t1","@type":"Dataset","description":"The second-order Fourier coefficients, $V_{2\\Delta}(2, |\\Delta\\eta| > 2)$, as a function of $N_{offline}^{trk}$ for charged particles.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.76506.v1/t2","@type":"Dataset","description":"The second-order Fourier coefficients, $V_{2\\Delta}(2, |\\Delta\\eta| > 2)$, as a function of $N_{offline}^{trk}$ for charged particles, after correcting for back-to-back...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.76506.v1/t3","@type":"Dataset","description":"The second-order Fourier coefficients, $V_{3\\Delta}(2, |\\Delta\\eta| > 2)$, as a function of $N_{offline}^{trk}$ for charged particles.","name":"Table 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flow, $v_{2}(2, |\\Delta\\eta| > 2)$, as a function of $p_{T}$ for charged particles.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.76506.v1/t12","@type":"Dataset","description":"The elliptic flow, $v_{2}(2, |\\Delta\\eta| > 2)$, as a function of $p_{T}$ for charged particles.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.76506.v1/t13","@type":"Dataset","description":"The elliptic flow, $v_{2}(2, |\\Delta\\eta| > 2)$, as a function of $p_{T}$ for charged particles.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.76506.v1/t14","@type":"Dataset","description":"The elliptic flow after correcting for back-to-back jet correlations, $v_{2}^{sub}(2, |\\Delta\\eta| > 2)$, as a function of $p_{T}$ for charged...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.76506.v1/t15","@type":"Dataset","description":"The elliptic flow after correcting for back-to-back jet correlations, $v_{2}^{sub}(2, |\\Delta\\eta| > 2)$, as a function of $p_{T}$ for 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