{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.145759.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2697877"}},{"@id":"https://doi.org/10.1007/JHEP12(2023)086","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2023","description":"Measurements of the production cross sections of prompt $\\mathrm{D}^0$, $\\mathrm{D}^+$, $\\mathrm{D}^{*+}$, $\\mathrm{D}^+_\\mathrm{c}$, $\\Lambda^+_\\mathrm{c}$, and $\\Xi^+_\\mathrm{c}$ charm hadrons at  midrapidity in proton$-$proton collisions at $\\sqrt{s}=13$ TeV with the ALICE detector are presented. The D-meson cross sections as a function of transverse momentum ($p_\\mathrm{T}$) are provided with improved precision and granularity. The ratios of $p_\\mathrm{T}$-differential meson production cross sections based on this publication and on measurements at different rapidity and collision energy provide a constraint on gluon parton distribution functions at low values of Bjorken-$x$ ($10^{-5}-10^{-4}$). The measurements of $\\Lambda^+_\\mathrm{c}$ ($\\Xi^+_\\mathrm{c}$) baryon production extend the measured $p_\\mathrm{T}$ intervals down to $p_\\mathrm{T}=0(3)$~GeV$/c$. These measurements are used to determine the charm-quark fragmentation fractions and the $\\mathrm{c}\\bar{\\mathrm{c}}$ production cross section at midrapidity ($|y|<0.5$) based on the sum of the cross sections of the weakly-decaying ground-state charm hadrons $\\mathrm{D}^0$, $\\mathrm{D}^+$, $\\mathrm{D}^+_\\mathrm{c}$, $\\Lambda^+_\\mathrm{c}$, $\\Xi^0_\\mathrm{c}$ and, for the first time, $\\Xi^+_\\mathrm{c}$, and of the strongly-decaying $J/\\psi$ mesons. The first measurements of $\\Xi^+_\\mathrm{c}$ and $\\Sigma_\\mathrm{c}^{0,+,++}$ fragmentation fractions at midrapidity are also reported. A significantly larger fraction of charm quarks hadronising to baryons is found compared to $\\mathrm{e}^+\\mathrm{e}^-$ and ep collisions. The $\\mathrm{c}\\bar{\\mathrm{c}}$ production cross section at midrapidity is found to be at the upper bound of state-of-the-art perturbative QCD calculations.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.145759.v1/t1","@type":"Dataset","description":"$p_{\\mathrm{T}}$-differential $\\mathrm{D}^{0}$ production cross section at midrapidity ($|y|<0.5$) in pp collisions at $\\sqrt{s}$ = 13 TeV Branching ratio of $\\mathrm{D}^{0}\\rightarrow\\mathrm{K}^-\\pi^+$:...","name":"Figure 4 Dzero pp 13 TeV"},{"@id":"https://doi.org/10.17182/hepdata.145759.v1/t2","@type":"Dataset","description":"$p_{\\mathrm{T}}$-differential $\\mathrm{D}^{+}$ production cross section at midrapidity ($|y|<0.5$) in pp collisions at $\\sqrt{s}$ = 13 TeV Branching ratio of $\\mathrm{D}^{+}\\rightarrow\\mathrm{K}^-\\pi^+\\pi^+$:...","name":"Figure 4 Dplus pp 13 TeV"},{"@id":"https://doi.org/10.17182/hepdata.145759.v1/t3","@type":"Dataset","description":"$p_{\\mathrm{T}}$-differential $\\mathrm{D}^{+}$ 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