{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.77057.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1380453"}},{"@id":"https://doi.org/10.1016/j.physletb.2017.01.074","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2017","description":"CERN-LHC. The first measurement of $\\phi$-meson production in p-Pb collisions at a nucleon-nucleon centre-of-mass energy $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV has been performed with the ALICE apparatus at the LHC. $\\phi$-mesons have been identified in the dimuon decay channel in the transverse momentum ($p_{\\rm T}$) range $1 < p_{\\rm T} < 7$ GeV/$c$, both in the p-going ($2.03 < y < 3.53$) and the Pb-going ($-4.46 < y < -2.96$) directions, where $y$ stands for the rapidity in the nucleon-nucleon centre-of-mass. Differential cross sections as a function of transverse momentum and rapidity are presented. The forward-backward asymmetry for phi-meson production is measured for $2.96<|y|<3.53$, showing no significant $p_{\\rm T}$ dependence within the uncertainties. The $p_{\\rm T}$-dependence of the phi nuclear modification factor $R_{\\rm pPb}$ exhibits an enhancement up to a factor 1.6 at $p_{\\rm T}$ = 3-4 GeV/$c$ in the Pb-going direction. The $p_{\\rm T}$-dependence of the $\\phi$-meson cross section in pp collisions at $\\sqrt{s}$ = 2.76 TeV, which is used to determine a reference for the p-Pb results, is also presented here for $1 < p_{\\rm T} < 5$ GeV/$c$ and $2.5 <y < 4$.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.77057.v1/t1","@type":"Dataset","description":"$p_{\\rm T}$-differential production cross section of $\\phi$ in pp at $\\sqrt{s_{\\rm NN}}$=2.76 TeV, in the rapidity range 2.5 < y...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.77057.v1/t2","@type":"Dataset","description":"$p_{\\rm T}$-differential production cross section of $\\phi$ in p-Pb at $\\sqrt{s_{\\rm NN}}$=5.02 TeV, in the rapidity range 4.46 < y...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.77057.v1/t3","@type":"Dataset","description":"$p_{\\rm T}$-differential production cross section of $\\phi$ in p-Pb at $\\sqrt{s_{\\rm NN}}$=5.02 TeV, in the rapidity range 2.03 < y...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.77057.v1/t4","@type":"Dataset","description":"$y$-differential production cross section of $\\phi$ in p-Pb at $\\sqrt{s_{\\rm NN}}$=5.02 TeV, in $p_{\\rm T}$ range 2.03 < $p_{\\rm T}$...","name":"Table 4"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1380453?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/77057"}],"inLanguage":"en","name":"$\\phi$-meson production at forward rapidity in p-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV and in pp collisions at $\\sqrt{s}$ = 2.76 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1380453?version=1","version":1}