{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.83778.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1669805"}},{"@id":"https://doi.org/10.1140/epjc/s10052-018-6034-3","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2018","description":"phi meson measurements provide insight into strangeness production, which is one of \nthe key observables for the hot medium formed in high-energy heavy-ion \ncollisions. ALICE measured phi production through its decay \nin muon pairs in Pb-Pb collisions at SQRT(S_NN) = 2.76 TeV \nin the intermediate transverse momentum range 2 < PT < 5 GeV/c \nand in the rapidity interval 2.5 < y <4. \nThe phi yield was measured as a function of the transverse momentum and collision centrality. \nThe nuclear modification factor was obtained as a\nfunction of the average number of participating nucleons.  \nResults were compared with the ones obtained via the kaon decay channel in the same \nPT range at midrapidity. The values of the nuclear modification factor in the two rapidity \nregions are in agreement within uncertainties.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.83778.v1/t1","@type":"Dataset","description":"phi yield as a function of $p_\\mathrm{T}$ at forward rapidity in pp collisions.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.83778.v1/t2","@type":"Dataset","description":"phi yield as a function of $p_\\mathrm{T}$ at forward rapidity in Pb-Pb collisions for 0-40\\% centrality.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.83778.v1/t3","@type":"Dataset","description":"phi yield as a function of $p_\\mathrm{T}$ at forward rapidity in Pb-Pb collisions for 40-90\\% centrality (scaled by 3 in...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.83778.v1/t4","@type":"Dataset","description":"$(\\mathrm{d}N_{\\phi}/\\mathrm{d}y)/\\left\\langle N_\\mathrm{part}\\right\\rangle$ as a function of $\\left\\langle N_\\mathrm{part}\\right\\rangle$ measured in the muon decay channel at forward rapidity in pp and...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.83778.v1/t5","@type":"Dataset","description":"$R_{\\mathrm{AA}}$ of the $\\phi$ meson as a function of $\\langle N_{\\mathrm{part}} \\rangle$ for $2.5<y<4$ and $2 < p_\\mathrm{T} <5$ GeV/c.","name":"Table 5"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1669805?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/83778"}],"inLanguage":"en","name":"$\\phi$ meson production at forward rapidity in Pb-Pb collisions at $\\sqrt{s_\\mathrm{NN}}=2.76$ TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1669805?version=1","version":1}