{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.89326.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1716440"}},{"@id":"https://doi.org/10.1140/epjc/s10052-019-6873-6","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2019","description":"CERN-LHC. The measurements of the production of prompt $\\rm{D}^{0}$, $\\rm{D}^{+}$, $\\rm D^{*+}$ and $\\rm D_{s}$ mesons in proton-proton (pp) collisions at $\\sqrt{s_{\\rm{NN}}}$=5.02 TeV with the ALICE detector at the Large Hadron Collider (LHC) are reported. D mesons were reconstructed at mid-rapidity ($|y|<0.5$) via their hadronic decay channels $\\rm{D^{0}}\\rightarrow K\\pi$, $\\rm{D^{+}}\\rightarrow K\\pi\\pi$, $\\rm{D}^{*+}\\rightarrow \\rm{D}^{0}\\pi\\rightarrow K\\pi\\pi$, $\\rm{D_{s}}\\rightarrow\\phi\\pi\\rightarrow K K \\pi$, and their charge conjugates. The production cross sections were measured in the transverse momentum interval 0<$p_{\\rm T}$<36 GeV/$c$ for $\\rm{D}^{0}$, 1<$p_{\\rm T}$<36 GeV/$c$ for $\\rm{D}^{+}$ and $\\rm D^{*+}$, and in 2<$p_{\\rm T}$<24 GeV/$c$ for $\\rm D_{s}$ mesons. Thanks to the higher integrated luminosity, an analysis in finer $p_{\\rm T}$ bins with respect to the previous measurements at $\\sqrt{s}$=7 Tev was performed, allowing for a more detailed description of the cross-section $p_{\\rm T}$ shape. The measured $p_{\\rm T}$-differential production cross sections are compared to the results at $\\sqrt{s}$=7 TeV and to four different perturbative QCD calculations. Its rapidity dependence is also tested combining the ALICE and LHCb measurements in pp collisions at $\\sqrt{s}$=5.02 TeV. This measurement will allow for a more accurate determination of the nuclear modification factor in p-Pb and Pb-Pb collisions performed at the same nucleon-nucleon centre-of-mass energy.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.89326.v1/t1","@type":"Dataset","description":"$p_{\\rm T}$-differential cross section of prompt $\\rm{D}^{0}$ mesons in pp collisions at $\\sqrt{\\rm{s_{NN}}}$=5.02 TeV in the rapidity interval $|y|$<0.5. Branching...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.89326.v1/t2","@type":"Dataset","description":"$p_{\\rm T}$-differential cross section of prompt $\\rm{D^{+}}$ mesons in pp collisions at $\\sqrt{\\rm{s_{NN}}}$=5.02 TeV in the rapidity interval $|y|$<0.5. Branching...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.89326.v1/t3","@type":"Dataset","description":"$p_{\\rm T}$-differential cross section of prompt $\\rm D^{*}$ mesons in pp collisions at $\\sqrt{\\rm{s_{NN}}}$=5.02 TeV in the rapidity interval $|y|$<0.5....","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.89326.v1/t4","@type":"Dataset","description":"$p_{\\rm T}$-differential cross section of prompt $\\rm{D_{s}}$ mesons in pp collisions at $\\sqrt{\\rm{s_{NN}}}$=5.02 TeV in the rapidity interval $|y|$<0.5. Branching...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.89326.v1/t5","@type":"Dataset","description":"$p_{\\rm T}$-differential cross section of inclusive $\\rm{D}^{0}$ mesons (including also $\\rm{D}^{0}$ mesons from beauty-hadron decays) in pp collisions at $\\sqrt{\\rm{s_{NN}}}$=5.02...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.89326.v1/t6","@type":"Dataset","description":"Ratio of $\\rm {D}^{+}$ to $\\rm{D}^{0}$ meson yield in pp collisions at $\\sqrt{\\rm{s_{NN}}}$=5.02 TeV in |y|<0.5 as a function of...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.89326.v1/t7","@type":"Dataset","description":"Ratio of $\\rm {D}^{*+}$ to $\\rm{D}^{0}$ meson yield in pp collisions at $\\sqrt{\\rm{s_{NN}}}$=5.02 TeV in |y|<0.5 as a function of...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.89326.v1/t8","@type":"Dataset","description":"Ratio of $\\rm {D}_{s}$ to $\\rm{D}^{0}$ meson yield in pp collisions at $\\sqrt{\\rm{s_{NN}}}$=5.02 TeV in |y|<0.5 as a function of...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.89326.v1/t9","@type":"Dataset","description":"Ratio of $\\rm {D}_{s}$ to $\\rm {D}^{+}$ meson yield in pp collisions at $\\sqrt{\\rm{s_{NN}}}$=5.02 TeV in |y|<0.5 as a function...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.89326.v1/t10","@type":"Dataset","description":"Ratio of $\\rm {D}^{+}$ to $\\rm{D}^{0}$ meson yield in pp collisions at $\\sqrt{\\rm{s_{NN}}}$=7 TeV in |y|<0.5 as a function of...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.89326.v1/t11","@type":"Dataset","description":"Ratio of $\\rm {D}^{*+}$ to $\\rm{D}^{0}$ meson yield in pp collisions at $\\sqrt{\\rm{s_{NN}}}$=7 TeV in |y|<0.5 as a function of...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.89326.v1/t12","@type":"Dataset","description":"Ratio of $\\rm {D}_{s}$ to $\\rm{D}^{0}$ meson yield in pp collisions at $\\sqrt{\\rm{s_{NN}}}$=7 TeV in |y|<0.5 as a function of...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.89326.v1/t13","@type":"Dataset","description":"Ratio of $\\rm {D}_{s}$ to $\\rm {D}^{+}$ meson yield in pp collisions at $\\sqrt{\\rm{s_{NN}}}$=7 TeV in |y|<0.5 as a function...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.89326.v1/t14","@type":"Dataset","description":"Ratios of $\\rm {D}^{0}$-mesons production cross sections in pp collisions at $\\sqrt{\\rm{s_{NN}}}$=7 TeV and $\\sqrt{\\rm{s_{NN}}}$=5.02 TeV as a function of...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.89326.v1/t15","@type":"Dataset","description":"Ratios of $\\rm {D}^{+}$-mesons production cross sections in pp collisions at $\\sqrt{\\rm{s_{NN}}}$=7 TeV and $\\sqrt{\\rm{s_{NN}}}$=5.02 TeV as a function of...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.89326.v1/t16","@type":"Dataset","description":"Ratios of $\\rm {D}^{*+}$-mesons production cross sections in pp collisions at $\\sqrt{\\rm{s_{NN}}}$=7 TeV and $\\sqrt{\\rm{s_{NN}}}$=5.02 TeV as a function of...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.89326.v1/t17","@type":"Dataset","description":"Ratios of $\\rm{D_{s}}$-mesons production cross sections in pp collisions at $\\sqrt{\\rm{s_{NN}}}$=7 TeV and $\\sqrt{\\rm{s_{NN}}}$=5.02 TeV as a function of $p_{\\rm...","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.89326.v1/t18","@type":"Dataset","description":"First Column: Production cross sections for prompt D mesons (D0, D+, D*+ and D_s) at mid-rapidity in |y|<0.5 and full...","name":"Table 18"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1716440?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/89326"}],"inLanguage":"en","name":"Measurement of ${\\rm D^0}$, ${\\rm D^+}$, ${\\rm D^{*+}}$ and ${{\\rm D^+_s}}$ production in pp collisions at $\\mathbf{\\sqrt{{\\textit s}}~=~5.02~TeV}$ with ALICE","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1716440?version=1","version":1}