{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.145839.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2692198"}},{"@id":"https://doi.org/10.1007/JHEP12(2023)067","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2023","description":"The Chiral Magnetic Wave (CMW) phenomenon is essential to provide insights into the strong interaction in QCD, the properties of the quark-gluon plasma, and the topological characteristics of the early universe, offering a deeper understanding of fundamental physics in high-energy collisions. Measurements of the charge-dependent anisotropic flow coefficients are studied in Pb-Pb collisions at center-of-mass energy per nucleon-nucleon collision $\\sqrt{s_{\\mathrm{NN}}}=$ 5.02 TeV to probe the CMW. In particular, the slope of the normalized difference in elliptic ($v_{2}$) and triangular ($v_{3}$) flow coefficients of positively and negatively charged particles as a function of their event-wise normalized number difference, is reported for inclusive and identified particles. The slope $r_{3}^{\\rm Norm}$ is found to be larger than zero and to have a magnitude similar to $r_{2}^{\\rm Norm}$, thus pointing to a large background contribution for these measurements. Furthermore, $r_{2}^{\\rm Norm}$ can be described by a blast wave model calculation that incorporates local charge conservation. In addition, using the event shape engineering technique yields a fraction of CMW ($f_{\\rm CMW}$) contribution to this measurement which is compatible with zero. This measurement provides the very first upper limit for $f_{\\rm CMW}$, and in the 10-60% centrality interval it is found to be 26% (38%) at 95% (99.7%) confidence level.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.145839.v1/t1","@type":"Dataset","description":"Normalized $\\Delta\\it{v}_{2}$ slope of charged hadrons as a function of centrality in Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.145839.v1/t2","@type":"Dataset","description":"Normalized $\\Delta\\it{v}_{2}$ slope of kaons as a function of centrality in Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.145839.v1/t3","@type":"Dataset","description":"Normalized $\\Delta\\it{v}_{2}$ slope of pions as a function of centrality in Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.145839.v1/t4","@type":"Dataset","description":"Normalized $\\Delta\\it{v}_{2}$ slope of protons as a function of centrality in Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.145839.v1/t5","@type":"Dataset","description":"Normalized $\\Delta\\it{v}_{3}$ slope of charged hadrons as a function of centrality in Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.145839.v1/t6","@type":"Dataset","description":"Normalized $\\Delta\\it{v}_{3}$ slope of kaons as a function of centrality in Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.145839.v1/t7","@type":"Dataset","description":"Normalized $\\Delta\\it{v}_{3}$ slope of pions as a function of centrality in Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.145839.v1/t8","@type":"Dataset","description":"Normalized $\\Delta\\it{v}_{3}$ slope of protons as a function of centrality in Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.145839.v1/t9","@type":"Dataset","description":"Delta Integral Covariance as function of $v_2$ in 0-10% Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.145839.v1/t10","@type":"Dataset","description":"Delta Integral Covariance as function of $v_2$ in 10-20% Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.145839.v1/t11","@type":"Dataset","description":"Delta Integral Covariance as function of $v_2$ in 20-30% Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.145839.v1/t12","@type":"Dataset","description":"Delta Integral Covariance as function of $v_2$ in 30-40% Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.145839.v1/t13","@type":"Dataset","description":"Delta Integral Covariance as function of $v_2$ in 40-50% Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.145839.v1/t14","@type":"Dataset","description":"Delta Integral Covariance as function of $v_2$ in 50-60% Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV.","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.145839.v1/t15","@type":"Dataset","description":"$f_{CMW}$ as function of CENTRALITY in Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV.","name":"Table 15"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2692198?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/145839"}],"inLanguage":"en","name":"Probing the Chiral Magnetic Wave with charge-dependent flow measurements in Pb-Pb collisions at the LHC","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2692198?version=1","version":1}