{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.134676.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2670243"}},{"@id":"https://doi.org/10.1103/PhysRevC.109.024914","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2023","description":"Two-particle Bose-Einstein momentum correlation functions for charged-hadron pairs in lead-lead collisions at a center-of-mass energy per nucleon pair of $\\sqrt{s_{_{\\mathrm{NN}}}} = 5.02$ TeV are studied. The data sample, containing $4.27\\times 10^{9}$ events corresponding to an integrated luminosity of 0.607 $\\mathrm{nb}^{-1}$, was collected by the CMS experiment in 2018. The experimental results are discussed in terms of a Levy-type source distribution. The parameters of this distribution are extracted as functions  of particle pair average transverse mass and collision centrality. These parameters include the correlation strength parameter, the Levy index or shape parameter ($\\alpha$), and the Levy scale parameter ($R$). The source shape, characterized by $\\alpha$, is found to be neither Cauchy nor Gaussian, implying the need for a full Levy analysis. Similarly to what was previously found for systems characterized by Gaussian source radii, a hydrodynamical scaling is also observed for the Levy $R$ parameter.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.134676.v1/t1","@type":"Dataset","description":"The correlation function $C_2(q)$ of negatively charged hadron pairs with $1.00&lt;K_{\\mathrm{T}}&lt;1.05$ GeV/$c$ in the 10-20% centrality bin.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.134676.v1/t2","@type":"Dataset","description":"The double-ratio correlation function $DR(q)$ of negatively charged hadron pairs with $1.30&lt;K_{\\mathrm{T}}&lt;1.35$ GeV/$c$ in the 20-30% centrality bin.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.134676.v1/t3","@type":"Dataset","description":"The two-particle correlation function of negatively charged hadron pairs with $0.9&lt;K_{\\mathrm{T}}&lt;1.3$ GeV/$c$ in the 0-100% centrality range, calculated using MC...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.134676.v1/t4","@type":"Dataset","description":"The Levy scale parameter $R$ versus the transverse mass $m_{\\mathrm{T}}$ in different centrality classes for negatively and positively charged hadron...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.134676.v1/t5","@type":"Dataset","description":"The $1/R^2$ distribution vs. transverse mass $m_{\\mathrm{T}}$ in different centrality classes for negatively and positively charged hadron pairs.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.134676.v1/t6","@type":"Dataset","description":"The linear-fit parameter $A$ versus $\\langle N_{\\text{part}}\\rangle$ for positively and negatively charged hadron pairs. The bin range on $\\langle N_{\\text{part}}\\rangle$...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.134676.v1/t7","@type":"Dataset","description":"The linear-fit parameter $B$ versus $\\langle N_{\\text{part}}\\rangle$ for positively and negatively charged hadron pairs. The bin range on $\\langle N_{\\text{part}}\\rangle$...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.134676.v1/t8","@type":"Dataset","description":"The Levy scale parameter $R$ versus $\\langle N_{\\text{part}}\\rangle^{1/3}$ in different $m_{\\mathrm{T}}$ classes for negatively and positively charged hadron pairs. The...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.134676.v1/t9","@type":"Dataset","description":"The Levy stability index $\\alpha$ versus the transverse mass $m_{\\mathrm{T}}$ in different centrality classes for negatively and positively charged hadron...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.134676.v1/t10","@type":"Dataset","description":"The average Levy stability index $\\langle \\alpha \\rangle$ versus $\\langle N_{\\text{part}}\\rangle$ for both positively and negatively charged hadron pairs. The...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.134676.v1/t11","@type":"Dataset","description":"The correlation strength $\\lambda$ versus the transverse mass $m_{\\mathrm{T}}$ in different centrality classes for negatively and positively charged hadron pairs.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.134676.v1/t12","@type":"Dataset","description":"The correlation strength (re-scaled with the square of the pion fraction) $\\lambda ^*$ versus the transverse mass $m_{\\mathrm{T}}$ in different...","name":"Table 12"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2670243?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/134676"}],"inLanguage":"en","name":"Two-particle Bose-Einstein correlations and their L\u00e9vy parameters in PbPb collisions at $\\sqrt{s_\\mathrm{NN}}$ = 5.02 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2670243?version=1","version":1}
