{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.77996.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1599077"}},{"@id":"https://doi.org/10.1140/epjc/s10052-017-4988-1","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2017","description":"CERN-LHC. Multi-particle cumulants and corresponding Fourier harmonics are measured for azimuthal angle distributions of charged particles in pp collisions at $\\sqrt{s}$ = 5.02 and 13 TeV and in p+Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV, and compared to the results obtained for low-multiplicity Pb+Pb collisions at $\\sqrt{s_{NN}}$ = 2.76 TeV. These measurements aim to assess the collective nature of particle production. The measurements of multi-particle cumulants confirm the evidence for collective phenomena in p+Pb and low-multiplicity Pb+Pb collisions. On the other hand, the pp results for four-particle cumulants do not demonstrate collective behaviour, indicating that they may be biased by contributions from non-flow correlations. A comparison of multi-particle cumulants and derived Fourier harmonics across different collision systems is presented as a function of the charged-particle multiplicity. For a given multiplicity, the measured Fourier harmonics are largest in Pb+Pb, smaller in p+Pb and smallest in pp collisions. The pp results show no dependence on the collision energy, nor on the multiplicity.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.77996.v1/t1","@type":"Dataset","description":"$c_2\\{4\\}$ cumulants for reference particles with 0.3 $&lt; p_T &lt;$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.77996.v1/t2","@type":"Dataset","description":"$c_2\\{4\\}$ cumulants for reference particles with 0.3 $&lt; p_T &lt;$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.77996.v1/t3","@type":"Dataset","description":"$c_2\\{4\\}$ cumulants for reference particles with 0.3 $&lt; p_T &lt;$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.77996.v1/t4","@type":"Dataset","description":"$c_2\\{4\\}$ cumulants for reference particles with 0.3 $&lt; p_T &lt;$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.77996.v1/t5","@type":"Dataset","description":"$c_2\\{4\\}$ cumulants for reference particles with 0.3 $&lt; p_T &lt;$ 3.0 GeV selected according to $N_{ch}(p_T &lt; 0.4 GeV)$ (EvSel_$N_{ch}$)...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.77996.v1/t6","@type":"Dataset","description":"$c_2\\{4\\}$ cumulants for reference particles with 0.3 $&lt; p_T &lt;$ 3.0 GeV selected according to $N_{ch}(p_T &lt; 0.4 GeV)$ (EvSel_$N_{ch}$)...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.77996.v1/t7","@type":"Dataset","description":"$c_2\\{4\\}$ cumulants for reference particles with 0.3 $&lt; p_T &lt;$ 3.0 GeV selected according to $N_{ch}(p_T &lt; 0.4 GeV)$ (EvSel_$N_{ch}$)...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.77996.v1/t8","@type":"Dataset","description":"$c_2\\{4\\}$ cumulants for reference particles with 0.3 $&lt; 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