{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.78365.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1507090"}},{"@id":"https://doi.org/10.1016/j.physletb.2017.07.017","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2017","description":"CERN-LHC. We present the charged-particle pseudorapidity density in Pb-Pb collisions at $\\sqrt{s_{_{\\mathrm{NN}}}}=5.02\\,\\mathrm{TeV}$ in centrality classes measured by ALICE.  The measurement covers a wide pseudorapidity range from $-3.5$ to $5$, which is sufficient for reliable estimates of the total number of charged particles produced in the collisions.  For the most central collisions we find $21\\,400\\pm 1\\,300$ while for the most peripheral we find $230\\pm 38$. This corresponds to an increase of $(27\\pm4)\\%$ over the results at $\\sqrt{s_{_{\\mathrm{NN}}}}=2.76\\,\\mathrm{TeV}$ previously reported by ALICE.  The energy dependence of the total number of charged particles produced in heavy-ion collisions is found to obey a modified power-law like behaviour.  The charged-particle\npseudorapidity density of the most central collisions is compared to model calculations - none of which fully describes the measured distribution. We also present an estimate of the rapidity density of charged particles. The width of that distribution is found to exhibit a remarkable proportionality to the beam rapidity, independent of the collision energy from the top SPS to LHC energies.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.78365.v1/t1","@type":"Dataset","description":"Charged-particle pseudorapidity density for ten centrality classes over a broad $\\eta$ range in Pb-Pb collisions at $\\sqrt{s_{_{\\mathrm{NN}}}}=5.02\\,\\mathrm{TeV}$. Boxes around the...","name":"DN/DETARAP"},{"@id":"https://doi.org/10.17182/hepdata.78365.v1/t2","@type":"Dataset","description":"Charged-particle pseudorapidity density at midrapidity in most perihperhal (80-90%) Pb-Pb collisions at $\\sqrt{s_{\\scriptscriptstyle\\mathrm{NN}}}=5.02\\,\\mathrm{TeV}$.","name":"DN/DETARAP(ETARAP=0)"},{"@id":"https://doi.org/10.17182/hepdata.78365.v1/t3","@type":"Dataset","description":"Total number of charged particles as a function of the mean number of participating nucleons [PRC88.044909]. The total charged-particle multiplicity...","name":"MULT"},{"@id":"https://doi.org/10.17182/hepdata.78365.v1/t4","@type":"Dataset","description":"Estimation of $\\mathrm{d}N_{\\mathrm{ch}}/\\mathrm{d}y$ for in the most central Pb-Pb collisions at $\\sqrt{s_{_{\\mathrm{NN}}}}=5.02\\,\\mathrm{TeV}$. Also shown is a fit of Gaussian distribution...","name":"DN/DYRAP"},{"@id":"https://doi.org/10.17182/hepdata.78365.v1/t5","@type":"Dataset","description":"Scaling behaviour as a function $\\sqrt{s_{_{\\mathrm{NN}}}}$ of the width of the charged-particle or -pion rapidity-density distribution with respect to the...","name":"SIGMA DN/DYRAP"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1507090?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/78365"}],"inLanguage":"en","name":"Centrality dependence of the pseudorapidity density distribution for charged particles in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=5.02$ TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1507090?version=1","version":1}