{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.65771.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1311487"}},{"@id":"https://doi.org/10.1140/epjc/s10052-014-3157-z","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2016","description":"CERN-LHC. The measurements are performed for charged particles with transverse momenta 0.5<pT<20 GeV and in the pseudorapidity range |eta|<2.5. The anisotropy is characterized by the Fourier coefficients, vn, of the charged-particle azimuthal angle distribution for n = 2-4. The Fourier coefficients are evaluated using multi-particle cumulants calculated with the generating function method. Results on the transverse momentum, pseudorapidity and centrality dependence of the vn coefficients are presented. The elliptic flow, v2, is obtained from the two-, four-, six- and eight-particle cumulants while higher-order coefficients, v3 and v4, are determined with two- and four-particle cumulants. A comparison to vn measurements obtained using different analysis methods and previously reported by the LHC experiments is also shown. Results of measurements of flow fluctuations evaluated with multi-particle cumulants are shown as a function of transverse momentum and the collision centrality.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t1","@type":"Dataset","description":"The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 0-2%.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t2","@type":"Dataset","description":"The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 2-5%.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t3","@type":"Dataset","description":"The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 5-10%.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t4","@type":"Dataset","description":"The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 10-15%.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t5","@type":"Dataset","description":"The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 15-20%.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t6","@type":"Dataset","description":"The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 20-25%.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t7","@type":"Dataset","description":"The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 25-30%.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t8","@type":"Dataset","description":"The second flow harmonic measured with the two-particle cumulants as a function of transverse 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.","name":"Table 161"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t162","@type":"Dataset","description":"The ratio of second flow harmonics measured with the six- and four-particle cumulants as a function of .","name":"Table 162"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t163","@type":"Dataset","description":"The ratio of second flow harmonics measured with the eight- and four-particle cumulants as a function of .","name":"Table 163"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t164","@type":"Dataset","description":"The second flow harmonic measured with the Event Plane method as a function of .","name":"Table 164"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t165","@type":"Dataset","description":"The triangular flow harmonic measured with the Event Plane method as a function of .","name":"Table 165"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t166","@type":"Dataset","description":"The triangular flow harmonic measured with the two-particle cumulants as a function of .","name":"Table 166"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t167","@type":"Dataset","description":"The triangular flow harmonic measured with the two-particle cumulants as a function of .","name":"Table 167"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t168","@type":"Dataset","description":"The quadrangular flow harmonic measured with the Event Plane method as a function of .","name":"Table 168"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t169","@type":"Dataset","description":"The quadrangular flow harmonic measured with the two-particle cumulants as a function of .","name":"Table 169"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t170","@type":"Dataset","description":"The quadrangular flow harmonic measured with the two-particle cumulants as a function of .","name":"Table 170"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t171","@type":"Dataset","description":"The second flow harmonic fluctiuations, F(v2), as a function of 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triangular flow harmonic fluctuations, F(v4), as a function of .","name":"Table 185"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t186","@type":"Dataset","description":"The second flow harmonic measured with the two-particle cumulats as a function of .","name":"Table 186"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t187","@type":"Dataset","description":"The second flow harmonic measured with the four-particle cumulats as a function of .","name":"Table 187"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t188","@type":"Dataset","description":"The second flow harmonic measured with the six-particle cumulats as a function of .","name":"Table 188"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t189","@type":"Dataset","description":"The second flow harmonic measured with the eight-particle cumulats as a function of .","name":"Table 189"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t190","@type":"Dataset","description":"The ratio of second flow harmonics measured 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210"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t211","@type":"Dataset","description":"The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin...","name":"Table 211"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t212","@type":"Dataset","description":"The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin...","name":"Table 212"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t213","@type":"Dataset","description":"The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin...","name":"Table 213"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t214","@type":"Dataset","description":"The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin...","name":"Table 214"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t215","@type":"Dataset","description":"The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin...","name":"Table 215"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t216","@type":"Dataset","description":"The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin...","name":"Table 216"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t217","@type":"Dataset","description":"The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin...","name":"Table 217"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t218","@type":"Dataset","description":"The second flow harmonic fluctuations, F(v2), as a function of .","name":"Table 218"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t219","@type":"Dataset","description":"The triangular flow harmonic fluctuations, F(v3), as a function of .","name":"Table 219"},{"@id":"https://doi.org/10.17182/hepdata.65771.v1/t220","@type":"Dataset","description":"The triangular flow harmonic fluctuations, F(v4), as a function of .","name":"Table 220"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1311487?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/65771"}],"inLanguage":"en","name":"Measurement of flow harmonics with multi-particle cumulants in Pb+Pb collisions at $\\sqrt{s_{NN}}=2.76$ TeV with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1311487?version=1","version":1}