{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.152619.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2805671"}},{"@id":"https://doi.org/10.1103/PhysRevLett.134.111903","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2024","description":"Nuclear medium effects on $\\text{B}^+$ meson production are studied using the binary-collision scaled cross section ratio between events of different charged-particle multiplicities from proton-lead collisions.  Data, collected by the CMS experiment in 2016 at a nucleon-nucleon center-of-mass energy of $\\sqrt{s_{NN}} = 8.16\\,$TeV, corresponding to an integrated luminosity of 175\\nbinv, were used. The scaling factors in the ratio are determined using a novel approach based on the Z$\\,\\to\\mu^{-}\\mu^{+}$ cross sections measured in the same events. The scaled ratio for $\\text{B}^+$ is consistent with unity for all event multiplicities, putting stringent constraints on nuclear modification for heavy flavor.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.152619.v1/t1","@type":"Dataset","description":"$\\mathrm{B}^+$ differential cross section and FONLL calculations, scaled by the number of binary collisions, vs $p_{\\mathrm{T}}$. Global uncertainty (not included...","name":"B+ diff. cross section and FONLL calculations vs pT"},{"@id":"https://doi.org/10.17182/hepdata.152619.v1/t2","@type":"Dataset","description":"$\\mathrm{B}^+$ differential cross section in $p_{\\mathrm{T}}$ bins divided into classes of multiplicity. For better visibility, data points are scaled by...","name":"B+ diff. cross section in pT bins for different multiplicities"},{"@id":"https://doi.org/10.17182/hepdata.152619.v1/t3","@type":"Dataset","description":"The $R_{\\mathrm{HL}}$ for $\\mathrm{B}^+$ in $p_{\\mathrm{T}}$ bins for the highest and lowest multiplicity classes. The error bars correspond to the...","name":"The observable $R_{\\mathrm{HL}}$ for  B+ in pT bins"},{"@id":"https://doi.org/10.17182/hepdata.152619.v1/t4","@type":"Dataset","description":"The $R_{\\mathrm{HL}}$ for $\\mathrm{B}^+$ in the full $p_{\\mathrm{T}}$ range and as a function of the multiplicity density. The three different...","name":"The observable $R_{\\mathrm{HL}}$  for  B+ vs Nch"},{"@id":"https://doi.org/10.17182/hepdata.152619.v1/t5","@type":"Dataset","description":"Z differential cross section in $p_{\\mathrm{T}}$ bins divided into classes of multiplicity. Vertical bars represent total uncertainties.","name":"Z diff. cross section in pT bins for different multiplicities"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2805671?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/152619"}],"inLanguage":"en","name":"Search for nuclear modifications of B$^+$ meson production in pPb collisions at $\\sqrt{s_\\mathrm{NN}}$ = 8.16 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2805671?version=1","version":1}