{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.138404.v2","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1990765"}},{"@id":"https://doi.org/10.1016/j.physletb.2023.137796","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2023","description":"The production of prompt\u00a0$\\rm \\Lambda_{\\rm c}^{+}$\u00a0baryons at midrapidity ($|y|<0.5$) was measured in central (0--10\\%) and mid-central (30--50\\%) Pb--Pb collisions at the center-of-mass energy per nucleon--nucleon pair $\\sqrt{s_{\\mathrm{NN}}}=5.02$ TeV with the ALICE detector. The\u00a0$\\rm \\Lambda_{\\rm c}^{+}$ production yield, the\u00a0$\\rm \\Lambda_{\\rm c}^{+} / D^0$ production ratio, and the\u00a0$\\rm \\Lambda_{\\rm c}^{+}$ nuclear modification factor $R_{\\rm AA}$ are reported. The results are more precise and more differential in transverse momentum ($p_{\\rm T}$) and centrality with respect to previous measurements. The\u00a0$\\rm \\Lambda_{\\rm c}^{+} / D^0$ ratio, which is enhanced with respect to the pp measurement for $4<p_{\\rm T}<8$ GeV/$c$, is described by theoretical calculations that model the charm-quark transport in the quark--gluon plasma and include hadronization via both coalescence and fragmentation mechanisms.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.138404.v2/t1","@type":"Dataset","description":"Transverse-momentum-differential production yields of prompt $\\mathrm{\\Lambda_c^+}$ in central (0--10\\%) and mid-central (30--50\\%) Pb--Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}=5.02$ TeV.","name":"Table 1a"},{"@id":"https://doi.org/10.17182/hepdata.138404.v2/t2","@type":"Dataset","description":"The $\\mathrm{\\Lambda_c^+ / D^0}$ production yield ratio in central (0--10\\%) and mid-central (30--50\\%) Pb--Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}=5.02$ TeV.","name":"Table 1b"},{"@id":"https://doi.org/10.17182/hepdata.138404.v2/t3","@type":"Dataset","description":"The nuclear modification factor of prompt $\\mathrm{\\Lambda_c^+}$ as a function transverse momentum in central (0--10\\%) and mid-central (30--50\\%) Pb--Pb collisions...","name":"Table 2"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1990765?version=2"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/138404"}],"inLanguage":"en","name":"Constraining hadronization mechanisms with $\\rm \\Lambda_{\\rm c}^{+}$/D$^0$ production ratios 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/ins1990765?version=2","version":2}