{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.88289.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1759853"}},{"@id":"https://doi.org/10.1140/epjc/s10052-020-7834-9","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2020","description":"Anisotropies in the initial energy density distribution of the quark-gluon plasma created in high energy heavy ion collisions lead to anisotropies in the azimuthal distributions of the final-state particles known as collective anisotropic flow. Fourier harmonic decomposition is used to quantify these anisotropies. The higher-order harmonics can be induced by the same order anisotropies (linear response) or by the combined influence of several lower order anisotropies (nonlinear response) in the initial state. The mixed higher-order anisotropic flow and nonlinear response coefficients of charged particles are measured as functions of transverse momentum and centrality in PbPb collisions at nucleon-nucleon center-of-mass energies $\\sqrt{\\smash[b]{s_{_{\\mathrm{NN}}}}} = 2.76$ and $5.02$ TeV with the CMS detector. The results are compared with viscous hydrodynamic calculations using several different initial conditions, as well as microscopic transport model calculations. None of the models provides a simultaneous description of the mixed higher-order flow harmonics and nonlinear response coefficients.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t1","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_4\\{\\Psi_{22}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 0-20%...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t2","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_5\\{\\Psi_{23}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 0-20%...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t3","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_6\\{\\Psi_{222}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 0-20%...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t4","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_6\\{\\Psi_{33}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 0-20%...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t5","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_7\\{\\Psi_{223}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 0-20%...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t6","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_4\\{\\Psi_{22}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 20-60%...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t7","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_5\\{\\Psi_{23}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 20-60%...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t8","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_6\\{\\Psi_{222}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 20-60%...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t9","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_6\\{\\Psi_{33}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 20-60%...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t10","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_7\\{\\Psi_{223}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 20-60%...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t11","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_4\\{\\Psi_{22}\\}$ from the scalar-product method at 2.76 TeV as a function of PT in the 0-20%...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t12","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_5\\{\\Psi_{23}\\}$ from the scalar-product method at 2.76 TeV as a function of PT in the 0-20%...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t13","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_6\\{\\Psi_{222}\\}$ from the scalar-product method at 2.76 TeV as a function of PT in the 0-20%...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t14","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_6\\{\\Psi_{33}\\}$ from the scalar-product method at 2.76 TeV as a function of PT in the 0-20%...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t15","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_7\\{\\Psi_{223}\\}$ from the scalar-product method at 2.76 TeV as a function of PT in the 0-20%...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t16","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_4\\{\\Psi_{22}\\}$ from the scalar-product method at 2.76 TeV as a function of PT in the 20-60%...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t17","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_5\\{\\Psi_{23}\\}$ from the scalar-product method at 2.76 TeV as a function of PT in the 20-60%...","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t18","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_6\\{\\Psi_{222}\\}$ from the scalar-product method at 2.76 TeV as a function of PT in the 20-60%...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t19","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_6\\{\\Psi_{33}\\}$ from the scalar-product method at 2.76 TeV as a function of PT in the 20-60%...","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t20","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_7\\{\\Psi_{223}\\}$ from the scalar-product method at 2.76 TeV as a function of PT in the 20-60%...","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t21","@type":"Dataset","description":"The overall flow harmonic $v_4\\{\\Psi_{4}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 0-20%...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t22","@type":"Dataset","description":"The overall flow harmonic $v_5\\{\\Psi_{5}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 0-20%...","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t23","@type":"Dataset","description":"The overall flow harmonic $v_6\\{\\Psi_{6}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 0-20%...","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t24","@type":"Dataset","description":"The overall flow harmonic $v_6\\{\\Psi_{6}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 0-20%...","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t25","@type":"Dataset","description":"The overall flow harmonic $v_7\\{\\Psi_{7}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 0-20%...","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t26","@type":"Dataset","description":"The overall flow harmonic $v_4\\{\\Psi_{4}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 20-60%...","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t27","@type":"Dataset","description":"The overall flow harmonic $v_5\\{\\Psi_{5}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 20-60%...","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t28","@type":"Dataset","description":"The overall flow harmonic $v_6\\{\\Psi_{6}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 20-60%...","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t29","@type":"Dataset","description":"The overall flow harmonic $v_6\\{\\Psi_{6}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 20-60%...","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t30","@type":"Dataset","description":"The overall flow harmonic $v_7\\{\\Psi_{7}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 20-60%...","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t31","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_4\\{\\Psi_{22}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 0-20%...","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t32","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_5\\{\\Psi_{23}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 0-20%...","name":"Table 32"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t33","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_6\\{\\Psi_{222}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 0-20%...","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t34","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_6\\{\\Psi_{33}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 0-20%...","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t35","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_7\\{\\Psi_{223}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 0-20%...","name":"Table 35"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t36","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_4\\{\\Psi_{22}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 20-60%...","name":"Table 36"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t37","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_5\\{\\Psi_{23}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 20-60%...","name":"Table 37"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t38","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_6\\{\\Psi_{222}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 20-60%...","name":"Table 38"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t39","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_6\\{\\Psi_{33}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 20-60%...","name":"Table 39"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t40","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_7\\{\\Psi_{223}\\}$ from the scalar-product method at 5.02 TeV as a function of PT in the 20-60%...","name":"Table 40"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t41","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{422}$ from the scalar-product method at 5.02 TeV as a function of PT in the 0-20% centrality...","name":"Table 41"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t42","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{523}$ from the scalar-product method at 5.02 TeV as a function of PT in the 0-20% centrality...","name":"Table 42"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t43","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{6222}$ from the scalar-product method at 5.02 TeV as a function of PT in the 0-20% centrality...","name":"Table 43"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t44","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{633}$ from the scalar-product method at 5.02 TeV as a function of PT in the 0-20% centrality...","name":"Table 44"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t45","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{7223}$ from the scalar-product method at 5.02 TeV as a function of PT in the 0-20% centrality...","name":"Table 45"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t46","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{422}$ from the scalar-product method at 5.02 TeV as a function of PT in the 20-60% centrality...","name":"Table 46"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t47","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{523}$ from the scalar-product method at 5.02 TeV as a function of PT in the 20-60% centrality...","name":"Table 47"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t48","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{6222}$ from the scalar-product method at 5.02 TeV as a function of PT in the 20-60% centrality...","name":"Table 48"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t49","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{633}$ from the scalar-product method at 5.02 TeV as a function of PT in the 20-60% centrality...","name":"Table 49"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t50","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{7223}$ from the scalar-product method at 5.02 TeV as a function of PT in the 20-60% centrality...","name":"Table 50"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t51","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{422}$ from the scalar-product method at 2.76 TeV as a function of PT in the 0-20% centrality...","name":"Table 51"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t52","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{523}$ from the scalar-product method at 2.76 TeV as a function of PT in the 0-20% centrality...","name":"Table 52"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t53","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{6222}$ from the scalar-product method at 2.76 TeV as a function of PT in the 0-20% centrality...","name":"Table 53"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t54","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{633}$ from the scalar-product method at 2.76 TeV as a function of PT in the 0-20% centrality...","name":"Table 54"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t55","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{7223}$ from the scalar-product method at 2.76 TeV as a function of PT in the 0-20% centrality...","name":"Table 55"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t56","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{422}$ from the scalar-product method at 2.76 TeV as a function of PT in the 20-60% centrality...","name":"Table 56"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t57","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{523}$ from the scalar-product method at 2.76 TeV as a function of PT in the 20-60% centrality...","name":"Table 57"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t58","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{6222}$ from the scalar-product method at 2.76 TeV as a function of PT in the 20-60% centrality...","name":"Table 58"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t59","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{633}$ from the scalar-product method at 2.76 TeV as a function of PT in the 20-60% centrality...","name":"Table 59"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t60","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{7223}$ from the scalar-product method at 2.76 TeV as a function of PT in the 20-60% centrality...","name":"Table 60"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t61","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_4\\{\\Psi_{22}\\}$ from the scalar-product method at 5.02 TeV as a function of centrality.","name":"Table 61"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t62","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_5\\{\\Psi_{23}\\}$ from the scalar-product method at 5.02 TeV as a function of centrality.","name":"Table 62"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t63","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_6\\{\\Psi_{222}\\}$ from the scalar-product method at 5.02 TeV as a function of centrality.","name":"Table 63"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t64","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_6\\{\\Psi_{33}\\}$ from the scalar-product method at 5.02 TeV as a function of centrality.","name":"Table 64"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t65","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_7\\{\\Psi_{223}\\}$ from the scalar-product method at 5.02 TeV as a function of centrality.","name":"Table 65"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t66","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_4\\{\\Psi_{22}\\}$ from the scalar-product method at 2.76 TeV as a function of centrality.","name":"Table 66"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t67","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_5\\{\\Psi_{23}\\}$ from the scalar-product method at 2.76 TeV as a function of centrality.","name":"Table 67"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t68","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_6\\{\\Psi_{222}\\}$ from the scalar-product method at 2.76 TeV as a function of centrality.","name":"Table 68"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t69","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_6\\{\\Psi_{33}\\}$ from the scalar-product method at 2.76 TeV as a function of centrality.","name":"Table 69"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t70","@type":"Dataset","description":"Mixed higher-order flow harmonic $v_7\\{\\Psi_{223}\\}$ from the scalar-product method at 2.76 TeV as a function of centrality.","name":"Table 70"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t71","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{422}$ from the scalar-product method at 5.02 TeV as a function of centrality.","name":"Table 71"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t72","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{523}$ from the scalar-product method at 5.02 TeV as a function of centrality.","name":"Table 72"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t73","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{6222}$ from the scalar-product method at 5.02 TeV as a function of centrality.","name":"Table 73"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t74","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{633}$ from the scalar-product method at 5.02 TeV as a function of centrality.","name":"Table 74"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t75","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{7223}$ from the scalar-product method at 5.02 TeV as a function of centrality.","name":"Table 75"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t76","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{422}$ from the scalar-product method at 2.76 TeV as a function of centrality.","name":"Table 76"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t77","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{523}$ from the scalar-product method at 2.76 TeV as a function of centrality.","name":"Table 77"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t78","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{6222}$ from the scalar-product method at 2.76 TeV as a function of centrality.","name":"Table 78"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t79","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{633}$ from the scalar-product method at 2.76 TeV as a function of centrality.","name":"Table 79"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t80","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{7223}$ from the scalar-product method at 2.76 TeV as a function of centrality.","name":"Table 80"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t81","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{422}$ from the scalar-product method at 5.02 TeV as a function of centrality.","name":"Table 81"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t82","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{523}$ from the scalar-product method at 5.02 TeV as a function of centrality.","name":"Table 82"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t83","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{6222}$ from the scalar-product method at 5.02 TeV as a function of centrality.","name":"Table 83"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t84","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{633}$ from the scalar-product method at 5.02 TeV as a function of centrality.","name":"Table 84"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t85","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{7223}$ from the scalar-product method at 5.02 TeV as a function of centrality.","name":"Table 85"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t86","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{422}$ from the scalar-product method at 2.76 TeV as a function of centrality.","name":"Table 86"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t87","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{523}$ from the scalar-product method at 2.76 TeV as a function of centrality.","name":"Table 87"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t88","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{6222}$ from the scalar-product method at 2.76 TeV as a function of centrality.","name":"Table 88"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t89","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{633}$ from the scalar-product method at 2.76 TeV as a function of centrality.","name":"Table 89"},{"@id":"https://doi.org/10.17182/hepdata.88289.v1/t90","@type":"Dataset","description":"Nonlinear response coefficient $\\chi_{7223}$ from the scalar-product method at 2.76 TeV as a function of centrality.","name":"Table 90"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1759853?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/88289"}],"inLanguage":"en","name":"Mixed higher-order anisotropic flow and nonlinear response coefficients of charged particles in PbPb collisions at $\\sqrt{s_\\mathrm{NN}} =$ 2.76 and 5.02 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1759853?version=1","version":1}