{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.94869.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1778342"}},{"@id":"https://doi.org/10.1007/JHEP05(2020)085","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2020","description":"Anisotropic flow coefficients, $v_n$, non-linear flow mode coefficients, $\\chi_{n,mk}$, and correlations among different symmetry planes, $\\rho_{n,mk}$ are measured in Pb--Pb collisions at $\\sqrt{s_\\mathrm{NN}}=5.02$ TeV. Results obtained with multi-particle correlations are reported for the transverse momentum interval $0.2<p_\\mathrm{T}<5.0$ GeV/$c$ within the pseudorapidity interval $0.4<|\\eta|<0.8$ as a function of collision centrality. The $v_n$ coefficients and $\\chi_{n,mk}$ and $\\rho_{n,mk}$ are presented up to the ninth and seventh harmonic order, respectively. Calculations suggest that the correlations measured in different symmetry planes and the non-linear flow mode coefficients are dependent on the shear and bulk viscosity to entropy ratios of the medium created in heavy-ion collisions. The comparison between these measurements and those at lower energies and calculations from hydrodynamic models places strong constraints on the initial conditions and transport properties of the system.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.94869.v1/t1","@type":"Dataset","description":"Centrality dependence of flow harmonics from $v_2$ to $v_9$.","name":"v2"},{"@id":"https://doi.org/10.17182/hepdata.94869.v1/t2","@type":"Dataset","description":"Centrality dependence of flow harmonics from $v_2$ to $v_9$.","name":"v3"},{"@id":"https://doi.org/10.17182/hepdata.94869.v1/t3","@type":"Dataset","description":"Centrality dependence of flow harmonics from $v_2$ to $v_9$.","name":"v4"},{"@id":"https://doi.org/10.17182/hepdata.94869.v1/t4","@type":"Dataset","description":"Centrality dependence of flow harmonics from $v_2$ to $v_9$.","name":"v5"},{"@id":"https://doi.org/10.17182/hepdata.94869.v1/t5","@type":"Dataset","description":"Centrality dependence of flow harmonics from $v_2$ to $v_9$.","name":"v6"},{"@id":"https://doi.org/10.17182/hepdata.94869.v1/t6","@type":"Dataset","description":"Centrality dependence of flow harmonics from $v_2$ to $v_9$.","name":"v7"},{"@id":"https://doi.org/10.17182/hepdata.94869.v1/t7","@type":"Dataset","description":"Centrality dependence of flow harmonics from $v_2$ to $v_9$.","name":"v8"},{"@id":"https://doi.org/10.17182/hepdata.94869.v1/t8","@type":"Dataset","description":"Centrality dependence of flow harmonics from $v_2$ to $v_9$.","name":"v9"},{"@id":"https://doi.org/10.17182/hepdata.94869.v1/t9","@type":"Dataset","description":"Centrality dependence of linear and non-linear flow modes.","name":"v422"},{"@id":"https://doi.org/10.17182/hepdata.94869.v1/t10","@type":"Dataset","description":"Centrality dependence of linear and non-linear flow modes.","name":"v523"},{"@id":"https://doi.org/10.17182/hepdata.94869.v1/t11","@type":"Dataset","description":"Centrality dependence of linear and non-linear flow modes.","name":"v6222"},{"@id":"https://doi.org/10.17182/hepdata.94869.v1/t12","@type":"Dataset","description":"Centrality dependence of linear and non-linear flow modes.","name":"v633"},{"@id":"https://doi.org/10.17182/hepdata.94869.v1/t13","@type":"Dataset","description":"Centrality dependence of linear and non-linear flow modes.","name":"v624"},{"@id":"https://doi.org/10.17182/hepdata.94869.v1/t14","@type":"Dataset","description":"Centrality dependence of linear and non-linear flow modes.","name":"v7223"},{"@id":"https://doi.org/10.17182/hepdata.94869.v1/t15","@type":"Dataset","description":"Centrality dependence of symmetry-plane correlations.","name":"rho422"},{"@id":"https://doi.org/10.17182/hepdata.94869.v1/t16","@type":"Dataset","description":"Centrality dependence of symmetry-plane correlations.","name":"rho523"},{"@id":"https://doi.org/10.17182/hepdata.94869.v1/t17","@type":"Dataset","description":"Centrality dependence of symmetry-plane correlations.","name":"rho633"},{"@id":"https://doi.org/10.17182/hepdata.94869.v1/t18","@type":"Dataset","description":"Centrality dependence of symmetry-plane correlations.","name":"rho624"},{"@id":"https://doi.org/10.17182/hepdata.94869.v1/t19","@type":"Dataset","description":"Centrality dependence of non-linear flow mode coefficients.","name":"chi422"},{"@id":"https://doi.org/10.17182/hepdata.94869.v1/t20","@type":"Dataset","description":"Centrality dependence of non-linear flow mode coefficients.","name":"chi6222"},{"@id":"https://doi.org/10.17182/hepdata.94869.v1/t21","@type":"Dataset","description":"Centrality dependence of non-linear flow mode coefficients.","name":"chi633"},{"@id":"https://doi.org/10.17182/hepdata.94869.v1/t22","@type":"Dataset","description":"Centrality dependence of non-linear flow mode coefficients.","name":"chi624"},{"@id":"https://doi.org/10.17182/hepdata.94869.v1/t23","@type":"Dataset","description":"Centrality dependence of non-linear flow mode coefficients.","name":"chi7223"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1778342?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/94869"}],"inLanguage":"en","name":"Higher harmonic non-linear flow modes of charged hadrons in Pb-Pb collisions at $\\sqrt{s_{\\rm{NN}}}$ = 5.02 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1778342?version=1","version":1}