{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.93880.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1801111"}},{"@id":"https://doi.org/10.1016/j.physletb.2021.136385","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2020","description":"CERN-LHC. The second-order Fourier coefficients ($v_{2}$) characterizing the azimuthal distribution of $\\Upsilon(\\mathrm{1S})$ and $\\Upsilon(\\mathrm{2S})$ mesons arising from PbPb collisions at $ {\\sqrt {\\smash [b]{s_{_{\\mathrm {NN}}}}}} = $ 5.02 TeV are studied. The $\\Upsilon$ mesons are reconstructed in their $\\mathrm{dimuon}$ decay channel, as measured by the CMS detector. The data set was collected in 2018 and corresponds to an integrated luminosity of 1.7$\\smash{\\,\\text{nb}^{-1}}$. The scalar product method is used to extract the $v_{2}$ coefficients of the azimuthal distribution. Results are reported for the rapidity range  $|y|<2.4$, with the transverse momentum $0 < $ ${p_{\\mathrm{T}}}$ $ < 50\\smash{\\,\\text{GeV/c}}$, and in three centrality ranges of 10-30, 30-50 and 50-90%. In contrast to the J/$\\psi$ mesons, no azimuthal anisotropy is observed for the $\\Upsilon$ mesons.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.93880.v1/t1","@type":"Dataset","description":"$v_{2}$ of $\\Upsilon(\\mathrm{1S})$ mesons as a function of collision centrality.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.93880.v1/t2","@type":"Dataset","description":"$v_{2}$ of $\\Upsilon(\\mathrm{1S})$ and $\\Upsilon(\\mathrm{2S})$ mesons integrated for 10-90% centrality range.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.93880.v1/t3","@type":"Dataset","description":"$v_{2}$ of $\\Upsilon(\\mathrm{1S})$ as a function of $p_{\\mathrm{T}}$ in 10-90% centrality range.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.93880.v1/t4","@type":"Dataset","description":"$v_{2}$ of $\\Upsilon(\\mathrm{1S})$ as a function of $p_{\\mathrm{T}}$ in three centrality ranges, 10-30%, 30-50% and 50-90%.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.93880.v1/t5","@type":"Dataset","description":"$v_{2}$ of $\\Upsilon(\\mathrm{1S})$ as a function of $p_{\\mathrm{T}}$ in 5-60% centrality range.","name":"Table 5"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1801111?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/93880"}],"inLanguage":"en","name":"Measurement of the azimuthal anisotropy of $\\Upsilon$(1S) and $\\Upsilon$(2S) mesons in PbPb collisions at $\\sqrt{s_\\mathrm{NN}} =$ 5.02 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1801111?version=1","version":1}