{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.62177.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1116150"}},{"@id":"https://doi.org/10.1016/j.physletb.2012.12.066","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2015","description":"CERN-LHC.  The elliptic, v2, triangular, v3, and quadrangular, v4, azimuthal anisotropic flow coefficients are measured for unidentified charged particles, pions and (anti-)protons in Pb-Pb collisions at sqrt(sNN) = 2.76 TeV recorded in 2010 with the ALICE detector at the Large Hadron Collider.  Results obtained with the event plane and four-particle cumulant methods are reported for the pseudo-rapidity range |eta| < 0.8 at different collision centralities and as a function of transverse momentum, pT, out to pT = 20 GeV.  The observed non-zero elliptic and triangular flow depends only weakly on transverse momentum for pT > 8 GeV.  The small pT dependence of the difference between elliptic flow results obtained from the event plane and four-particle cumulant methods suggests a common origin of flow fluctuations up to pT = 8 GeV.  The magnitude of the (anti-)proton elliptic and triangular flow is larger than that of pions out to at least pT = 8 GeV indicating that the particle type dependence persists out to high pT.\nUpdate Note (07/09/2015): Additional tables from ALICE-PUBLIC-2015-003 (http://cds.cern.ch/record/2045885) were added.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.62177.v1/t1","@type":"Dataset","description":"Elliptic flow (v2) estimated with Event Plane method (with eta gap of 2.0) measured for unidentified charged particles as a...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.62177.v1/t2","@type":"Dataset","description":"Elliptic flow (v2) estimated with four-particle cumulants measured for unidentified charged particles as a function of transverse momentum for various...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.62177.v1/t3","@type":"Dataset","description":"Triangular flow (v3) estimated with Event Plane method (with eta gap of 2.0) measured for unidentified charged particles as a...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.62177.v1/t4","@type":"Dataset","description":"Quadrangular flow (v4) measured with respect to symmetry plane Psi4, estimated with Event Plane method (with eta gap of 2.0),...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.62177.v1/t5","@type":"Dataset","description":"Quadrangular flow (v4) measured with respect to symmetry plane Psi2, estimated with Event Plane method (with eta gap of 2.0),...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.62177.v1/t6","@type":"Dataset","description":"Comparison of the ALICE results on v2, v3 and v4 obtained with the event plane method, measured for unidentified charged...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.62177.v1/t7","@type":"Dataset","description":"Relative event-by-event elliptic flow fluctuations for unidentified charged particles versus transverse momentum for different centrality classes.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.62177.v1/t8","@type":"Dataset","description":"Unidentified charged particle v2, v3, and v4 integrated over the transverse momentum range 10 < pT < 20 GeV as...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.62177.v1/t9","@type":"Dataset","description":"Elliptic flow (v2) estimated with Event Plane method (with eta gap of 2.0) of charged pion and proton as a...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.62177.v1/t10","@type":"Dataset","description":"Triangular flow (v3) estimated with Event Plane method (with eta gap of 2.0) of charged pion and proton as a...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.62177.v1/t11","@type":"Dataset","description":"$v_{2}$ vs $p_{T}$, centrality 0-5%.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.62177.v1/t12","@type":"Dataset","description":"$v_{2}$ vs $p_{T}$, centrality 5-10%.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.62177.v1/t13","@type":"Dataset","description":"$v_{2}$ vs $p_{T}$, centrality 10-20%.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.62177.v1/t14","@type":"Dataset","description":"$v_{2}$ vs $p_{T}$, centrality 20-30%.","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.62177.v1/t15","@type":"Dataset","description":"$v_{2}$ vs $p_{T}$, centrality 30-40%.","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.62177.v1/t16","@type":"Dataset","description":"$v_{2}$ vs $p_{T}$, centrality 40-50%.","name":"Table 16"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1116150?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/62177"}],"inLanguage":"en","name":"Anisotropic flow of charged hadrons, pions and (anti-)protons measured at high transverse momentum in Pb-Pb collisions at $\\snn=2.76$ TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1116150?version=1","version":1}