{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.76790.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1472319"}},{"@id":"https://doi.org/10.1016/j.physletb.2016.12.064","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2017","description":"CERN-LHC. The inclusive J/$\\psi$ production has been studied in Pb-Pb and pp collisions at the centre-of-mass energy per nucleon pair $\\sqrt{s_{\\rm NN}}=5.02$ TeV, using the ALICE detector at the CERN LHC. The J/$\\psi$ meson is reconstructed, in the centre-of-mass rapidity interval $2.5<y<4$ and in the transverse-momentum range $p_{\\rm T}<12$ GeV/$c$, via its decay to a muon pair. In this Letter, we present results on the inclusive J/$\\psi$ cross section in pp collisions at $\\sqrt{s}=5.02$ TeV and on the nuclear modification factor $R_{\\rm AA}$. The latter is presented as a function of the centrality of the collision and, for central collisions, as a function of the transverse momentum $p_{\\rm T}$ of the J/$\\psi$. The measured $R_{\\rm AA}$ values are compared to our previous results obtained in \\pbpb collisions at $\\sqrt{s_{\\rm NN}}=2.76$~TeV. The ratio of the $R_{\\rm AA}$ values at the two energies is also computed and compared to calculations of statistical and dynamical models. The numerical value of the ratio for central events (0--10\\% centrality) is $1.17 \\pm 0.04 {\\rm{(stat.)}}\\pm 0.20 {\\rm{(syst.)}}$. In central events, as a function of $p_{\\rm T}$, a slight increase of $R_{\\rm AA}$ with collision energy is visible in the region $2<p_{\\rm T}<6$ GeV/$c$. Theoretical calculations qualitatively describe the measurements, within uncertainties.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.76790.v1/t1","@type":"Dataset","description":"Differential cross section ${\\rm d}^2\\sigma^{\\rm pp}_{{\\rm J}/\\psi}/{\\rm d}y{\\rm d}p_{\\rm T}$ for inclusive J/$\\psi$ cross section in pp collisions at $\\sqrt{s}=5.02$...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.76790.v1/t2","@type":"Dataset","description":"The nuclear modification factor for inclusive J/$\\psi$ production, as a function of centrality, at $\\sqrt{s_{\\rm NN}}=5.02$ TeV. The widths of...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.76790.v1/t3","@type":"Dataset","description":"Centrality dependence (with 10% width centrality classes) of the inclusive J/$\\psi$ $R_{\\rm AA}$ for $0.3<p_{\\rm T}<8$ GeV/$c$. The first uncertainty...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.76790.v1/t4","@type":"Dataset","description":"Centrality dependence (with 10% width centrality classes) of the ratio of the inclusive J/$\\psi$ $R_{\\rm AA}$ for $0.3<p_{\\rm T}<8$ GeV/$c$...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.76790.v1/t5","@type":"Dataset","description":"Transverse momentum dependence (in 0-20% centrality class) of the inclusive J/$\\psi$ $R_{\\rm AA}$. The first uncertainty is statistical, the second...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.76790.v1/t6","@type":"Dataset","description":"Transverse momentum dependence (in 0-20% centrality class) of the double ratio of the inclusive J/$\\psi$ $R_{\\rm AA}$ at $\\sqrt{s_{NN}}$= 5.02...","name":"Table 6"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1472319?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/76790"}],"inLanguage":"en","name":"J/$\\psi$ suppression at forward rapidity in Pb-Pb collisions at $\\mathbf{\\sqrt{s_{{\\rm NN}}} = 5.02}$ TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1472319?version=1","version":1}