{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.79482.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1623558"}},{"@id":"https://doi.org/10.1016/j.physletb.2017.12.021","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2017","description":"In ultrarelativistic heavy-ion collisions, the event-by-event variation of the elliptic flow $v_2$ reflects fluctuations in the shape of the initial state of the system. This allows us to systematically study events corresponding to the same centrality but different initial geometry. This selection technique, Event Shape Engineering, has been used in the analysis of charge-dependent two- and three-particle correlations in Pb\u2014Pb collisions at $\\sqrt{s_{\\rm NN}} = 2.76$ TeV. The two-particle correlator $\\langle \\cos(\\varphi_{\\alpha} - \\varphi_{\\beta}) \\rangle$, calculated for different combinations of charges $\\alpha$ and $\\beta$, is almost independent of $v_2$ (for a given centrality), while the three-particle correlator $\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_2) \\rangle$ scales almost linearly both with the event $v_2$ and charged-particle pseudorapidity density. The charge dependence of the three-particle correlator is often interpreted as evidence for the Chiral Magnetic Effect (CME), a parity violating effect of the strong interaction. However, its measured dependence on $v_2$ points to a large non-CME contribution to the correlator. Comparing the results with Monte Carlo calculations including a magnetic field due to the spectators, the upper limit of the CME signal contribution to the three-particle correlator in the 10-50% centrality interval is found to be 26-33% at 95% confidence level.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t1","@type":"Dataset","description":"$v_2\\{EP\\}$ with $|\\Delta\\eta| > 2.0$ as a function of centrality for unbiased events in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} =...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t2","@type":"Dataset","description":"$v_2\\{EP\\}$ with $|\\Delta\\eta| > 2.0$ as a function of centrality for shape selected events (0-10% $q_2$) in Pb-Pb collisions at...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t3","@type":"Dataset","description":"$v_2\\{EP\\}$ with $|\\Delta\\eta| > 2.0$ as a function of centrality for shape selected events (10-20% $q_2$) in Pb-Pb collisions at...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t4","@type":"Dataset","description":"$v_2\\{EP\\}$ with $|\\Delta\\eta| > 2.0$ as a function of centrality for shape selected events (20-30% $q_2$) in Pb-Pb collisions at...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t5","@type":"Dataset","description":"$v_2\\{EP\\}$ with $|\\Delta\\eta| > 2.0$ as a function of centrality for shape selected events (30-40% $q_2$) in Pb-Pb collisions at...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t6","@type":"Dataset","description":"$v_2\\{EP\\}$ with $|\\Delta\\eta| > 2.0$ as a function of centrality for shape selected events (40-50% $q_2$) in Pb-Pb collisions at...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t7","@type":"Dataset","description":"$v_2\\{EP\\}$ with $|\\Delta\\eta| > 2.0$ as a function of centrality for shape selected events (50-60% $q_2$) in Pb-Pb collisions at...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t8","@type":"Dataset","description":"$v_2\\{EP\\}$ with $|\\Delta\\eta| > 2.0$ as a function of centrality for shape selected events (60-70% $q_2$) in Pb-Pb collisions at...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t9","@type":"Dataset","description":"$v_2\\{EP\\}$ with $|\\Delta\\eta| > 2.0$ as a function of centrality for shape selected events (70-80% $q_2$) in Pb-Pb collisions at...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t10","@type":"Dataset","description":"$v_2\\{EP\\}$ with $|\\Delta\\eta| > 2.0$ as a function of centrality for shape selected events (80-90% $q_2$) in Pb-Pb collisions at...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t11","@type":"Dataset","description":"$v_2\\{EP\\}$ with $|\\Delta\\eta| > 2.0$ as a function of centrality for shape selected events (90-100% $q_2$) in Pb-Pb collisions at...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t12","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (opposite charge pairs) with $|\\Delta\\eta| > 2.0$ as a function of centrality for...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t13","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (opposite charge pairs) with $|\\Delta\\eta| > 2.0$ as a function of centrality for...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t14","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (opposite charge pairs) with $|\\Delta\\eta| > 2.0$ as a function of centrality for...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t15","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (opposite charge pairs) with $|\\Delta\\eta| > 2.0$ as a function of centrality for...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t16","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (opposite charge pairs) with $|\\Delta\\eta| > 2.0$ as a function of centrality for...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t17","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (opposite charge pairs) with $|\\Delta\\eta| > 2.0$ as a function of centrality for...","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t18","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (opposite charge pairs) with $|\\Delta\\eta| > 2.0$ as a function of centrality for...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t19","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (opposite charge pairs) with $|\\Delta\\eta| > 2.0$ as a function of centrality for...","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t20","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (opposite charge pairs) with $|\\Delta\\eta| > 2.0$ as a function of centrality for...","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t21","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (opposite charge pairs) with $|\\Delta\\eta| > 2.0$ as a function of centrality for...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t22","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (opposite charge pairs) with $|\\Delta\\eta| > 2.0$ as a function of centrality for...","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t23","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (same charge pairs) with $|\\Delta\\eta| > 2.0$ as a function of centrality for...","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t24","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (same charge pairs) with $|\\Delta\\eta| > 2.0$ as a function of centrality for...","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t25","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (same charge pairs) with $|\\Delta\\eta| > 2.0$ as a function of centrality for...","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t26","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (same charge pairs) with $|\\Delta\\eta| > 2.0$ as a function of centrality for...","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t27","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (same charge pairs) with $|\\Delta\\eta| > 2.0$ as a function of centrality for...","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t28","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (same charge pairs) with $|\\Delta\\eta| > 2.0$ as a function of centrality for...","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t29","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (same charge pairs) with $|\\Delta\\eta| > 2.0$ as a function of centrality for...","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t30","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (same charge pairs) with $|\\Delta\\eta| > 2.0$ as a function of centrality for...","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t31","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (same charge pairs) with $|\\Delta\\eta| > 2.0$ as a function of centrality for...","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t32","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (same charge pairs) with $|\\Delta\\eta| > 2.0$ as a function of centrality for...","name":"Table 32"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t33","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (same charge pairs) with $|\\Delta\\eta| > 2.0$ as a function of centrality for...","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t34","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} - \\varphi_{\\beta}) \\rangle$ (opposite charge pairs) as a function of centrality for unbiased events in Pb-Pb collisions at...","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t35","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} - \\varphi_{\\beta}) \\rangle$ (opposite charge pairs) as a function of centrality for shape selected events (0-10% $q_2$) in...","name":"Table 35"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t36","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} - \\varphi_{\\beta}) \\rangle$ (opposite charge pairs) as a function of centrality for shape selected events (10-20% $q_2$) in...","name":"Table 36"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t37","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} - \\varphi_{\\beta}) \\rangle$ (opposite charge pairs) as a function of centrality for shape selected events (20-30% $q_2$) in...","name":"Table 37"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t38","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} - \\varphi_{\\beta}) \\rangle$ (opposite charge pairs) as a function of centrality for shape selected events (30-40% $q_2$) in...","name":"Table 38"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t39","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} - \\varphi_{\\beta}) \\rangle$ (opposite charge pairs) as a function of centrality for shape selected events (40-50% $q_2$) in...","name":"Table 39"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t40","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} - \\varphi_{\\beta}) \\rangle$ (opposite charge pairs) as a function of centrality for shape selected events (50-60% $q_2$) in...","name":"Table 40"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t41","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} - \\varphi_{\\beta}) \\rangle$ (opposite charge pairs) as a function of centrality for shape selected events (60-70% $q_2$) in...","name":"Table 41"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t42","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} - \\varphi_{\\beta}) \\rangle$ (opposite charge pairs) as a function of centrality for shape selected events (70-80% $q_2$) in...","name":"Table 42"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t43","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} - \\varphi_{\\beta}) \\rangle$ (opposite charge pairs) as a function of centrality for shape selected events (80-90% $q_2$) in...","name":"Table 43"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t44","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} - \\varphi_{\\beta}) \\rangle$ (opposite charge pairs) as a function of centrality for shape selected events (90-100% $q_2$) in...","name":"Table 44"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t45","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} - \\varphi_{\\beta}) \\rangle$ (same charge pairs) as a function of centrality for unbiased events in Pb-Pb collisions at...","name":"Table 45"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t46","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} - \\varphi_{\\beta}) \\rangle$ (same charge pairs) as a function of centrality for shape selected events (0-10% $q_2$) in...","name":"Table 46"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t47","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} - \\varphi_{\\beta}) \\rangle$ (same charge pairs) as a function of centrality for shape selected events (10-20% $q_2$) in...","name":"Table 47"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t48","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} - \\varphi_{\\beta}) \\rangle$ (same charge pairs) as a function of centrality for shape selected events (20-30% $q_2$) in...","name":"Table 48"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t49","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} - \\varphi_{\\beta}) \\rangle$ (same charge pairs) as a function of centrality for shape selected events (30-40% $q_2$) in...","name":"Table 49"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t50","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} - \\varphi_{\\beta}) \\rangle$ (same charge pairs) as a function of centrality for shape selected events (40-50% $q_2$) in...","name":"Table 50"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t51","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} - \\varphi_{\\beta}) \\rangle$ (same charge pairs) as a function of centrality for shape selected events (50-60% $q_2$) in...","name":"Table 51"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t52","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} - \\varphi_{\\beta}) \\rangle$ (same charge pairs) as a function of centrality for shape selected events (60-70% $q_2$) in...","name":"Table 52"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t53","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} - \\varphi_{\\beta}) \\rangle$ (same charge pairs) as a function of centrality for shape selected events (70-80% $q_2$) in...","name":"Table 53"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t54","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} - \\varphi_{\\beta}) \\rangle$ (same charge pairs) as a function of centrality for shape selected events (80-90% $q_2$) in...","name":"Table 54"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t55","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} - \\varphi_{\\beta}) \\rangle$ (same charge pairs) as a function of centrality for shape selected events (90-100% $q_2$) in...","name":"Table 55"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t56","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (opposite - same) with $|\\Delta\\eta| > 2.0$ as a function of $v_2\\{EP\\}$ for...","name":"Table 56"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t57","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (opposite - same) with $|\\Delta\\eta| > 2.0$ as a function of $v_2\\{EP\\}$ for...","name":"Table 57"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t58","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (opposite - same) with $|\\Delta\\eta| > 2.0$ as a function of $v_2\\{EP\\}$ for...","name":"Table 58"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t59","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (opposite - same) with $|\\Delta\\eta| > 2.0$ as a function of $v_2\\{EP\\}$ for...","name":"Table 59"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t60","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (opposite - same) with $|\\Delta\\eta| > 2.0$ as a function of $v_2\\{EP\\}$ for...","name":"Table 60"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t61","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (opposite - same) with $|\\Delta\\eta| > 2.0$ as a function of $v_2\\{EP\\}$ for...","name":"Table 61"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t62","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (opposite - same) with $|\\Delta\\eta| > 2.0$ as a function of $v_2\\{EP\\}$ for...","name":"Table 62"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t63","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (opposite - same) with $|\\Delta\\eta| > 2.0$ multiplied by the charged-particle density, $dN/d\\eta$,...","name":"Table 63"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t64","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (opposite - same) with $|\\Delta\\eta| > 2.0$ multiplied by the charged-particle density, $dN/d\\eta$,...","name":"Table 64"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t65","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (opposite - same) with $|\\Delta\\eta| > 2.0$ multiplied by the charged-particle density, $dN/d\\eta$,...","name":"Table 65"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t66","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (opposite - same) with $|\\Delta\\eta| > 2.0$ multiplied by the charged-particle density, $dN/d\\eta$,...","name":"Table 66"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t67","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (opposite - same) with $|\\Delta\\eta| > 2.0$ multiplied by the charged-particle density, $dN/d\\eta$,...","name":"Table 67"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t68","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (opposite - same) with $|\\Delta\\eta| > 2.0$ multiplied by the charged-particle density, $dN/d\\eta$,...","name":"Table 68"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t69","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (opposite - same) with $|\\Delta\\eta| > 2.0$ multiplied by the charged-particle density, $dN/d\\eta$,...","name":"Table 69"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t70","@type":"Dataset","description":"$p_1$ parameter from a linear fit to $\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 2\\Psi_{2}) \\rangle$ (opposite - same) with $|\\Delta\\eta| >...","name":"Table 70"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t71","@type":"Dataset","description":"CME fraction extracted from the slope parameter of fits to data and MC\u2014Glauber model as a function of centrality in...","name":"Table 71"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t72","@type":"Dataset","description":"CME fraction extracted from the slope parameter of fits to data and MC\u2014KLN CGC model as a function of centrality...","name":"Table 72"},{"@id":"https://doi.org/10.17182/hepdata.79482.v1/t73","@type":"Dataset","description":"CME fraction extracted from the slope parameter of fits to data and EKRT model as a function of centrality in...","name":"Table 73"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1623558?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/79482"}],"inLanguage":"en","name":"Constraining the magnitude of the Chiral Magnetic Effect with Event Shape Engineering in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 2.76$ TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1623558?version=1","version":1}