{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.88408.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1672798"}},{"@id":"https://doi.org/10.1016/j.physletb.2018.11.067","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2019","description":"CERN-LHC. Inclusive $\\Upsilon$(1S) and $\\Upsilon$(2S) production have been measured in Pb-Pb collisions at the centre-of-mass energy per nucleon-nucleon pair $\\sqrt{s_{_{\\rm NN}}}=5.02$ TeV, using the ALICE detector at the CERN LHC. The $\\Upsilon$ mesons are reconstructed in the centre-of-mass rapidity interval $2.5<y<4$ and in the transverse-momentum range $p_{\\rm T}<15$ GeV/$c$, via their decays to muon pairs. Results on the inclusive $\\Upsilon$(1S) nuclear modification factor $R_{\\rm AA}$ as a function of collision centrality, transverse momentum and rapidity are reported.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.88408.v1/t1","@type":"Dataset","description":"Inclusive $\\Upsilon$(1S) $R_{\\rm AA}$ and Pb-Pb yields for the centrality, transverse-momentum and rapidity ranges 0-90%, $0<p_{\\rm T}<15$ GeV/$c$ and $2.5<y<4$,...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.88408.v1/t2","@type":"Dataset","description":"Inclusive $\\Upsilon$(1S) $R_{\\rm AA}$ and Pb-Pb yields as a function of collision centrality. The transverse-momentum and rapidity ranges are $0<p_{\\rm...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.88408.v1/t3","@type":"Dataset","description":"Inclusive $\\Upsilon$(1S) $R_{\\rm AA}$ and Pb-Pb yields as a function of transverse momentum. The centrality and rapidity ranges are 0-90%...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.88408.v1/t4","@type":"Dataset","description":"Inclusive $\\Upsilon$(1S) $R_{\\rm AA}$ and Pb-Pb yields as a function of rapidity. The centrality and transverse-momentum ranges are 0-90% and...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.88408.v1/t5","@type":"Dataset","description":"Inclusive $\\Upsilon$(2S) $R_{\\rm AA}$ and Pb-Pb yield for the centrality, transverse-momentum and rapidity ranges 0-90%, $0<p_{\\rm T}<15$ GeV/$c$ and $2.5<y<4$,...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.88408.v1/t6","@type":"Dataset","description":"Inclusive $\\Upsilon\\text{(2S)}/\\Upsilon\\text{(1S)}$ Pb-Pb yield ratio and $R_{\\rm AA}$ ratio for the centrality, transverse-momentum and rapidity ranges 0-90%, $0<p_{\\rm T}<15$ GeV/$c$...","name":"Table 6"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1672798?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/88408"}],"inLanguage":"en","name":"$\\Upsilon$ suppression at forward rapidity in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1672798?version=1","version":1}