{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.134069.v3","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2610522"}},{"@id":"https://doi.org/10.1103/PhysRevLett.131.121901","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2023","description":"The dependence of the ratio between the $\\mathrm{B}_\\mathrm{s}$ and $\\mathrm{B}^{+}$ hadron production fractions, $f_{s}/f_{u}$, on the transverse momentum ($p_T$) and rapidity of the $\\mathrm{B}$ meson is studied using the decay channels $\\mathrm{B}_\\mathrm{s}\\rightarrow\\mathrm{J/\\psi} \\mathrm{\\phi}$ and $\\mathrm{B}^{+}\\rightarrow \\mathrm{J/\\psi} \\mathrm{K}^{+}$. The analysis uses a data sample of proton-proton collisions at a center-of-mass energy of 13TeV, collected by the CMS experiment in 2018 and corresponding to an integrated luminosity of 61.6 $\\mathrm{fb}^{-1}$. The $f_{s}/f_{u}$ ratio is observed to depend on the $\\mathrm{B}$ $p_T$, and to be consistent with becoming asymptotically constant at large $p_T$. No rapidity  dependence is observed. The ratio of the $\\mathrm{B}^{0}$ to $\\mathrm{B}^{+}$ meson production fractions $f_{d}/f_{u}$, is also measured, for the first time at hadron colliders, using the $\\mathrm{B}^{0} \\rightarrow \\mathrm{J/\\psi} \\mathrm{K}^{*0}$ decay channel. The result is found to be within one standard deviation of unity and independent of $p_T$ and rapidity, as expected from isospin invariance.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.134069.v3/t1","@type":"Dataset","description":"The $\\mathrm{J/\\psi \\phi}$, $\\mathrm{J/\\psi K}$, and $\\mathrm{J/\\psi} \\mathrm{K}^{*0}$ invariant mass distributions, for $\\mathrm{B}$ meson candidates with $20 < p_T <...","name":"Figure 1"},{"@id":"https://doi.org/10.17182/hepdata.134069.v3/t2","@type":"Dataset","description":"Left pannel. The vertical bars (boxes) represent the statistical (bin-to-bin systematic) uncertainties, while the horizontal bars give the bin widths....","name":"Figure 2a"},{"@id":"https://doi.org/10.17182/hepdata.134069.v3/t3","@type":"Dataset","description":"Right pannel. The vertical bars (boxes) represent the statistical (bin-to-bin systematic) uncertainties, while the horizontal bars give the bin widths....","name":"Figure 2b"},{"@id":"https://doi.org/10.17182/hepdata.134069.v3/t4","@type":"Dataset","description":"Left panel.The vertical bars (boxes) represent the statistical (bin-to-bin systematic) uncertainties, while the horizontal bars give the bin widths. The...","name":"Figure 3a"},{"@id":"https://doi.org/10.17182/hepdata.134069.v3/t5","@type":"Dataset","description":"Right panel.The vertical bars (boxes) represent the statistical (bin-to-bin systematic) uncertainties, while the horizontal bars give the bin widths. The...","name":"Figure 3b"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2610522?version=3"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/134069"}],"inLanguage":"en","name":"Measurement of the dependence of the hadron production fraction ratio $f_\\mathrm{s} / f_\\mathrm{u}$ and $f_\\mathrm{d} / f_ \\mathrm{u}$ on B meson kinematic variables in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2610522?version=3","version":3}