{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.142463.v2","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2601281"}},{"@id":"https://doi.org/10.1016/j.physletb.2024.138700","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2024","description":"CERN-LHC. ALICE. Multiplicity ($N_{\\mathrm{ch}}$) distributions and transverse momentum ($p_{\\mathrm{T}}$) spectra of inclusive primary charged particles in the kinematic range of $|\\eta| < 0.8$ and $0.15\\ \\mathrm{GeV}/c < p_{\\mathrm{T}} < 10\\ \\mathrm{GeV}/c$ are reported for pp, p-Pb, Xe-Xe and Pb-Pb collisions at centre-of-mass energies per nucleon pair ranging from $\\sqrt{s_\\mathrm{NN}} = 2.76\\ \\mathrm{TeV}$ up to $13\\ \\mathrm{TeV}$. The multiplicity distributions are also shown in their KNO-scaled form. The correlation between the transverse momentum of primary charged particles and the charged-particle multiplicity of the corresponding collision is reported in fine intervals. In addition, the mean $ \\langle p_{\\mathrm{T}} \\rangle $ and standard deviation $ \\sigma(p_{\\mathrm{T}}) $ derived from these multiplicity dependent $p_\\mathrm{T}$ spectra are shown as a function of $N_{\\mathrm{ch}}$. The relative standard deviation $ \\sigma(p_{\\mathrm{T}}) / \\langle p_{\\mathrm{T}} \\rangle $ of the spectra is reported as well. All observables are also presented as a function of the reltaive multiplicity $ N_{\\mathrm{ch}}\\ / \\langle N_{\\mathrm{ch}} \\rangle $. Note that $ \\langle N_{\\mathrm{ch}} \\rangle $ is calculated for the whole multiplicity range extending beyond the $N_{\\mathrm{ch}}$ values reported for the multiplicity-differential observables. Also the transverse momentum spectra integrated over this full range of multiplicities are presented. The mean and standard deviation derived from these multiplicity-integrated $p_\\mathrm{T}$ spectra are used to normalize the corresponding multiplicity-dependent values which are then reported as a function of $ N_{\\mathrm{ch}}\\ / \\langle N_{\\mathrm{ch}} \\rangle $.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.142463.v2/t1","@type":"Dataset","description":"Charged-particle multiplicity distribution for pp collisions at 2.76 TeV.","name":"pp_2TeV_multDist"},{"@id":"https://doi.org/10.17182/hepdata.142463.v2/t2","@type":"Dataset","description":"Koba-Nielsen-Olesen scaled charged-particle multiplicity distribution for pp collisions at 2.76 TeV.","name":"pp_2TeV_multDistKNO"},{"@id":"https://doi.org/10.17182/hepdata.142463.v2/t3","@type":"Dataset","description":"Charged-particle transverse momentum spectra as a function of charged-particle multiplicity for pp collisions at 2.76 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