{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.180917.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/3123964"}}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2026","description":"The latest experimental studies related to the search for the Chiral Magnetic Effect (CME) in Pb--Pb collisions at $\\snn=5.02$~TeV~recorded with the ALICE detector at the Large Hadron Collider (LHC) are presented. Charge-dependent two-particle correlations relative to the reaction plane are measured for charged particles in the pseudorapidity range $|\\eta| < 0.8$ and the transverse-momentum range $0.2< p_{\\mathrm{T}} < 5$~GeV/$c$. Two approaches have been employed: in the first method, the contribution of the background to the measurement is varied using the event shape engineering (ESE), while the second relies on changing the contribution of the potential CME signal by measuring azimuthal correlations relative to the participant plane, where the background contributions are maximized, and spectator plane, where the CME signal contribution is maximized. Both methods yield results consistent with the absence of a CME signal within the measurement uncertainties. The result obtained from correlations relative to different symmetry planes, a technique applied for the first time at LHC energies, gives the possibility to test independently and confirm the upper limits from previous measurements, while the new limit from the ESE analysis offers improved constraint relative to previous attempts.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.180917.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 $\\sqrt{s_{\\rm NN}} =...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.180917.v1/t2","@type":"Dataset","description":"$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.180917.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.180917.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.180917.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.180917.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.180917.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.180917.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.180917.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.180917.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.180917.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.180917.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.180917.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.180917.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.180917.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.180917.v1/t16","@type":"Dataset","description":"$\\langle \\cos(\\varphi_{\\alpha} + \\varphi_{\\beta} - 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