{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.167421.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2954608"}},{"@id":"https://doi.org/10.1140/epjc/s10052-025-15205-7","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2025","description":"The dependence of $\\mathrm{f}_{0}$(980) production on the final-state charged-particle multiplicity is reported for proton--proton (pp) collisions at the centre-of-mass energy, $\\sqrt{s}=$~13~TeV. The production of $\\mathrm{f}_{0}$(980) is measured with the ALICE detector via the $\\mathrm{f}_0 (980) \\rightarrow \\pi^{+}\\pi^{-}$ decay channel in a midrapidity region of $|y|<$~0.5. The evolution of the integrated yields and mean transverse momentum of f$_{0}$(980) as a function of charged-particle multiplicity measured in pp at $\\sqrt{s}=$~13~TeV follows the trends observed in pp at $\\sqrt{s}=$~5.02~TeV and in proton--lead (p--Pb) collisions at $\\sqrt{s_{\\mathrm{NN}}}=$~5.02~TeV. Particle yield ratios of $\\mathrm{f}_{0}$(980) to $\\pi^{\\pm}$ and $\\mathrm{K}^{*}$(892)$^{0}$ are found to decrease with increasing charged-particle multiplicity. These particle ratios are compared with calculations from the canonical statistical thermal model as a function of charged-particle multiplicity. The thermal model calculations provide a better description of the decreasing trend of particle ratios when no strange or antistrange quark composition for f$_{0}$(980) is assumed, which suggests that the tetraquark interpretation of the f$_{0}$(980) is disfavored.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.167421.v1/t1","@type":"Dataset","description":"Transverse momentum spectra in different multiplicity classes. Each spectrum is corrected for the branching ratio of (46 $\\pm$ 6)% based...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.167421.v1/t2","@type":"Dataset","description":"The ratio of transverse momentum spectrum to the INEL > 0 spectrum","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.167421.v1/t3","@type":"Dataset","description":"Transverse momentum integrated f0(980) yield in pp collisions","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.167421.v1/t4","@type":"Dataset","description":"Mean transverse momentum of f0(980) in pp collisions","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.167421.v1/t5","@type":"Dataset","description":"The particle yield ratio of f0((980) to charged pions","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.167421.v1/t6","@type":"Dataset","description":"The particle yield ratio of f0((980) to K*(892)0","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.167421.v1/t7","@type":"Dataset","description":"The double ratio of particle yield of f0(980) to charged pions","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.167421.v1/t8","@type":"Dataset","description":"The double ratio of particle yield of f0((980) to K*(892)0","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.167421.v1/t9","@type":"Dataset","description":"Transverse momentum differential particle yield ratio of f0(980) to charged pions","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.167421.v1/t10","@type":"Dataset","description":"Transverse momentum differential particle yield ratio of f0(980) to K*(892)0","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.167421.v1/t11","@type":"Dataset","description":"Transverse momentum differential double ratio of particle yield of f0(980) to charged pions","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.167421.v1/t12","@type":"Dataset","description":"Transverse momentum differential double ratio of particle yield of f0(980) to K*0","name":"Table 12"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2954608?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/167421"}],"inLanguage":"en","name":"Multiplicity dependence of f$_0$(980) production in pp collisions at $\\sqrt{s} = 13$ TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2954608?version=1","version":1}