{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.88290.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1738943"}},{"@id":"https://doi.org/10.1016/j.physletb.2020.135328","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2020","description":"The differential cross sections of $\\Lambda_\\mathrm{c}^+$ baryon production are measured via the exclusive decay channel $\\Lambda_\\mathrm{c}^+ \\to $pK$^-\\pi^+$, as a function of transverse momentum ($p_\\mathrm{T}$) in proton-proton (pp) and lead-lead (PbPb) collisions at a nucleon-nucleon center-of-mass energy of 5.02 TeV with the CMS detector at the LHC. The measurement is performed within the $\\Lambda_\\mathrm{c}^+$ rapidity interval $|y|<$1.0 in the $p_\\mathrm{T}$ range of 5-20 GeV/$c$ in pp and 10-20 GeV/$c$ in PbPb collisions. The observed yields of $\\Lambda_\\mathrm{c}^+$ for $p_\\mathrm{T}$ of 10-20 GeV/$c$ suggest a possible suppression in central PbPb collisions compared to pp collisions. The $\\Lambda_\\mathrm{c}^+/$D$^0$ production ratio in pp collisions is compared to theoretical models. In PbPb collisions, this ratio is consistent with the result from pp collisions in their common $p_\\mathrm{T}$ range.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.88290.v1/t1","@type":"Dataset","description":"The $p_{T}$-differential cross sections for inclusive $\\Lambda_{c}^{+}$ production in pp collisions. The uncertainties associated with the $\\Lambda_{c}^{+} \\to pK^{-}\\pi^{+}$ branching...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.88290.v1/t2","@type":"Dataset","description":"The $T_{AA}$-scaled yields for inclusive $\\Lambda_{c}^{+}$ baryon in three centrality regions of PbPb collisions. The uncertainties associated with the $\\Lambda_{c}^{+}...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.88290.v1/t3","@type":"Dataset","description":"The nuclear modification factor $R_{AA}$ versus $\\langle N_\\text{part} \\rangle$ for inclusive $\\Lambda_{c}^{+}$ production in the centrality range $0-100\\%$, $0-30\\%$ and...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.88290.v1/t4","@type":"Dataset","description":"The ratio of the production cross sections of inclusive $\\Lambda_{c}^{+}$ to prompt $D^{0}$ versus $p_{T}$ from pp collisions. The $20\\%$...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.88290.v1/t5","@type":"Dataset","description":"The ratio of the production cross sections of inclusive $\\Lambda_{c}^{+}$ to prompt $D^{0}$ versus $p_{T}$ from $0-100\\%$ centrality PbPb collisions....","name":"Table 5"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1738943?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/88290"}],"inLanguage":"en","name":"Production of $\\Lambda_\\mathrm{c}^+$ baryons in proton-proton and lead-lead 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/ins1738943?version=1","version":1}