{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.105047.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1848990"}},{"@id":"https://doi.org/10.1007/JHEP05(2021)220","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2021","description":"The $p_{\\mathrm{T}}$-differential production cross sections of prompt and non-prompt (produced in beauty-hadron decays) D mesons were measured by the ALICE experiment at midrapidity ($|y|<0.5$) in proton--proton collisions at $\\sqrt{s}=5.02~\\mathrm{TeV}$. The data sample used in the analysis corresponds to an integrated luminosity of $(19.3\\pm0.4)~\\mathrm{nb^{-1}}$. D mesons were reconstructed from their decays $\\mathrm{D^0 \\to K^-\\pi^+}$, $\\mathrm{D^+\\to K^-\\pi^+\\pi^+}$, and $\\mathrm{D_s^+\\to \\phi\\pi^+\\to K^-K^+\\pi^+}$ and their charge conjugates. Compared to previous measurements in the same rapidity region, the cross sections of prompt $\\mathrm{D^+}$ and $\\mathrm{D_s^+}$ mesons have an extended $p_{\\mathrm{T}}$ coverage and total uncertainties reduced by a factor ranging from 1.05 to 1.6, depending on $p_{\\mathrm{T}}$, allowing for a more precise determination of their $p_{\\mathrm{T}}$-integrated cross sections. The results are well described by perturbative QCD calculations. The fragmentation fraction of heavy quarks to strange mesons divided by the one to non-strange mesons, $f_\\mathrm{s}/(f_\\mathrm{u}+f_\\mathrm{d})$, is compatible for charm and beauty quarks and with previous measurements at different centre-of-mass energies and collision systems. The $\\mathrm{b\\overline{b}}$ production cross section per rapidity unit at midrapidity, estimated from non-prompt D-meson measurements, is $\\mathrm{d}\\sigma_\\mathrm{b\\overline{b}}/\\mathrm{d} y|_\\mathrm{|y|<0.5} = 34.5 \\pm 2.4 (\\mathrm{stat}) ^{+4.7}_{-2.9} (\\mathrm{tot.~syst})~\\mathrm{\\mu b}$. It is compatible with previous measurements at the same centre-of-mass energy and with the cross section predicted by perturbative QCD calculations.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.105047.v1/t1","@type":"Dataset","description":"$p_\\mathrm{T}$-differential production cross section of non-prompt $\\mathrm{D^0}$ mesons in pp collision at $\\sqrt{s}=5.02~\\mathrm{TeV}$ in the rapidity interval $|y|<0.5$. Branching ratio...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.105047.v1/t2","@type":"Dataset","description":"$p_\\mathrm{T}$-differential production cross section of non-prompt $\\mathrm{D^+}$ mesons in pp collision at $\\sqrt{s}=5.02~\\mathrm{TeV}$ in the rapidity interval $|y|<0.5$. Branching ratio...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.105047.v1/t3","@type":"Dataset","description":"$p_\\mathrm{T}$-differential production cross section of non-prompt $\\mathrm{D_{s}^{+}}$ mesons in pp collision at $\\sqrt{s}=5.02~\\mathrm{TeV}$ in the rapidity interval $|y|<0.5$. Branching ratio...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.105047.v1/t4","@type":"Dataset","description":"$p_\\mathrm{T}$-differential production cross section of prompt $\\mathrm{D^0}$ mesons in pp collision at $\\sqrt{s}=5.02~\\mathrm{TeV}$ in the rapidity interval $|y|<0.5$. Result already...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.105047.v1/t5","@type":"Dataset","description":"$p_\\mathrm{T}$-differential production cross section of prompt $\\mathrm{D^+}$ mesons in pp collision at $\\sqrt{s}=5.02~\\mathrm{TeV}$ in the rapidity interval $|y|<0.5$. Branching ratio...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.105047.v1/t6","@type":"Dataset","description":"$p_\\mathrm{T}$-differential production cross section of prompt $\\mathrm{D_{s}^{+}}$ mesons in pp collision at $\\sqrt{s}=5.02~\\mathrm{TeV}$ in the rapidity interval $|y|<0.5$. Branching ratio...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.105047.v1/t7","@type":"Dataset","description":"Ratio of $p_\\mathrm{{T}}$-differential production cross sections of non-prompt and prompt $\\mathrm{D^0}$ mesons in pp collision at $\\sqrt{s}=5.02~\\mathrm{TeV}$ in the rapidity...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.105047.v1/t8","@type":"Dataset","description":"Ratio of $p_\\mathrm{{T}}$-differential production cross sections of non-prompt and prompt $\\mathrm{D^+}$ mesons in pp collision at $\\sqrt{s}=5.02~\\mathrm{TeV}$ in the rapidity...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.105047.v1/t9","@type":"Dataset","description":"Ratio of $p_\\mathrm{{T}}$-differential production cross sections of non-prompt and prompt $\\mathrm{D_{s}^{+}}$ mesons in pp collision at $\\sqrt{s}=5.02~\\mathrm{TeV}$ in the rapidity...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.105047.v1/t10","@type":"Dataset","description":"Ratio between the $p_\\mathrm{T}$-differential production cross sections of prompt $\\mathrm{D^+}$ and $\\mathrm{D^0}$ mesons in pp collision at $\\sqrt{{s}}=5.02~\\mathrm{{TeV}}$ in the...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.105047.v1/t11","@type":"Dataset","description":"Ratio between the $p_\\mathrm{T}$-differential production cross sections of non-prompt $\\mathrm{D^+}$ and $\\mathrm{D^0}$ mesons in pp collision at $\\sqrt{{s}}=5.02~\\mathrm{{TeV}}$ in the...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.105047.v1/t12","@type":"Dataset","description":"Ratio between the $p_\\mathrm{T}$-differential production cross sections of prompt $\\mathrm{D_{s}^{+}}$ mesons and the sum of $\\mathrm{{D^+}}$ and $\\mathrm{{D^0}}$ mesons in...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.105047.v1/t13","@type":"Dataset","description":"Ratio between the $p_\\mathrm{T}$-differential production cross sections of non-prompt $\\mathrm{D_{s}^{+}}$ mesons and the sum of $\\mathrm{{D^+}}$ and $\\mathrm{{D^0}}$ mesons in...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.105047.v1/t14","@type":"Dataset","description":"Charm-quark fragmentation-fraction ratio $f_\\mathrm{s}/(f_\\mathrm{u}+f_\\mathrm{d})$ in pp collision at $\\sqrt{s}=5.02~\\mathrm{TeV}$. Obtained by fitting the prompt $\\mathrm{D_{s}^{+}} / (\\mathrm{{D^+}}+\\mathrm{{D^0}})$ ratio with a...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.105047.v1/t15","@type":"Dataset","description":"Beauty-quark fragmentation-fraction ratio $f_\\mathrm{s}/(f_\\mathrm{u}+f_\\mathrm{d})$ in pp collision at $\\sqrt{s}=5.02~\\mathrm{TeV}$. Obtained by fitting the non-prompt $\\mathrm{D_{s}^{+}} / (\\mathrm{{D^+}}+\\mathrm{{D^0}})$ ratio with a...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.105047.v1/t16","@type":"Dataset","description":"$\\mathrm{d}\\sigma_\\mathrm{b\\overline{b}}/\\mathrm{d} y$ estimated from non-prompt $\\mathrm{{D^0}}$, $\\mathrm{{D^+}}$ and $\\mathrm{D_{s}^{+}}$ mesons (black circles of Figure 12) measured in pp collision at...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.105047.v1/t17","@type":"Dataset","description":"Production cross sections of prompt and non-prompt $\\mathrm{{D^0}}$, $\\mathrm{{D^+}}$ and $\\mathrm{D_{s}^{+}}$ mesons in pp collision at $\\sqrt{{s}}=5.02~\\mathrm{{TeV}}$ in the rapidity...","name":"Table 17"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1848990?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/105047"}],"inLanguage":"en","name":"Measurement of beauty and charm production in pp collisions at $\\sqrt{s}=5.02$ TeV via non-prompt and prompt D mesons","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1848990?version=1","version":1}