{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.77600.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1512297"}},{"@id":"https://doi.org/10.1016/j.physletb.2017.03.049","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2017","description":"CERN-LHC. The production of muons from heavy-flavour hadron decays in p--Pb collisions at $\\sqrt{s_{\\rm NN}}=5.02$~TeV was studied for $2<p_{\\rm T}<16$~GeV/$c$ with the ALICE detector at the CERN LHC. The measurement was performed at forward (p-going direction) and backward (Pb-going direction) rapidity, in the ranges of rapidity in the center-of-mass system (cms) $2.03<y_{\\rm cms}<3.53$ and $\u22124.46<y_{\\rm cms}<-2.96$, respectively. The production cross sections and nuclear modification factors are presented as a function of transverse momentum ($p_{\\rm T}$). At forward rapidity, the nuclear modification factor is compatible with unity while at backward rapidity, in the interval $2.5<p_{\\rm T}<3.5$~GeV/$c$, it is above unity by more than $2\\sigma$. The ratio of the forward-to-backward production cross sections is also measured in the overlapping interval $2.96<|y_{\\rm cms}|<3.53$ and is smaller than unity by $3.7\\sigma$ in $2.5<p_{\\rm T}<3.5$~GeV/$c$. The data are described by model calculations including cold nuclear matter effects.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.77600.v1/t1","@type":"Dataset","description":"pT-differential production cross section of heavy-flavour decay muons at forward rapidity (proton-going side) and backward rapidity (Pb-going side)","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.77600.v1/t2","@type":"Dataset","description":"pT-differential nuclear modification factor of heavy-flavour decay muons at forward rapidity (proton-going side)","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.77600.v1/t3","@type":"Dataset","description":"pT-differential nuclear modification factor of heavy-flavour decay muons at backward rapidity (Pb-going side)","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.77600.v1/t4","@type":"Dataset","description":"pT-differential nuclear modification factor of heavy-flavour decay muons at forward rapidity (proton-going side)","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.77600.v1/t5","@type":"Dataset","description":"pT-differential nuclear modification factor of heavy-flavour decay muons at backward rapidity (Pb-going side)","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.77600.v1/t6","@type":"Dataset","description":"pT-differential forward-to-backward ratio of heavy-flavour decay muons","name":"Table 6"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1512297?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/77600"}],"inLanguage":"en","name":"Production of muons from heavy-flavour hadron decays in p-Pb collisions at $\\mathbf{\\sqrt{{\\textit s}_{NN}} = 5.02}$ TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1512297?version=1","version":1}