{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.69529.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1366028"}},{"@id":"https://doi.org/10.1007/JHEP09(2015)148","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2016","description":"CERN-LHC. Prompt D meson and non-prompt JPSI yields are studied as a function of the multiplicity of charged particles produced in inelastic proton-proton collisions at a centre-of-mass energy of SQRT(S) = 7 TeV. The results are reported as a ratio between yields in a given multiplicity interval normalised to the multiplicity-integrated ones (relative yields). They are shown as a function of the multiplicity of charged particles normalised to the average value for inelastic collisions (relative charged-particle multiplicity). D$^{0}$, D$^{+}$ and D*$^{+}$ mesons are measured in five PT intervals from 1 GeV/c to 20 GeV/c and for |YRAP| < 0.5 via their hadronic decays. The D0-meson relative yield is also measured as a function of the relative multiplicity at forward pseudo-rapidity. The non-prompt JPSI i.e. the B hadron, contribution to the inclusive JPSI production is measured in the di-electron decay channel at central rapidity. It is evaluated for PT > 1.3 GeV/c and |YRAP| < 0.9, and extrapolated to PT > 0.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.69529.v1/t1","@type":"Dataset","description":"Average of D$^{0}$, D$^{+}$ and D*$^{+}$ mesons relative yields for the sum of particle and antiparticle in several multiplicity and...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.69529.v1/t2","@type":"Dataset","description":"Average of D$^{0}$, D$^{+}$ and D*$^{+}$ mesons relative yields for the sum of particle and antiparticle in several multiplicity and...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.69529.v1/t3","@type":"Dataset","description":"D$^{0}$-meson relative yields for the sum of particle and antiparticle in several multiplicity and PT intervals for pp collisions at...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.69529.v1/t4","@type":"Dataset","description":"D$^{0}$-meson relative yields for the sum of particle and antiparticle in several multiplicity and PT intervals for pp collisions at...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.69529.v1/t5","@type":"Dataset","description":"Fraction of non-prompt JPSI measured for PT > 1.3 GeV/c, $f_{\\rm B}$(%), and extrapolated down to PT > 0, $f_{\\rm...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.69529.v1/t6","@type":"Dataset","description":"Prompt and non-prompt relative JPSI relative yields for PT > 0 in the in different multiplicity bins. The first and...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.69529.v1/t7","@type":"Dataset","description":"Prompt and non-prompt relative JPSI relative yields for PT > 0 in the in different multiplicity bins. The first and...","name":"Table 7"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1366028?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/69529"}],"inLanguage":"en","name":"Measurement of charm and beauty production at central rapidity versus charged-particle multiplicity in proton-proton collisions at $\\mathbf{\\sqrt{{\\textit s}}}=7$ TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1366028?version=1","version":1}