{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.95735.v1/t1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1784454"}},{"@id":"https://doi.org/10.1016/j.physletb.2020.135595","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Dataset","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2020","description":"Summary of results for Inclusive HF muon v2 as a function of pT for different centrality. Uncertainties are statistical and...","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/627465/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/627465/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/627465/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/627465/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/627465/yoda.h5","description":"YODA.H5 file","encodingFormat":"https://yoda.hepforge.org"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1784454?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/95735"}],"inLanguage":"en","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.95735.v1","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins1784454?version=1"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.95735.v1","@type":"Dataset","description":"CERN-LHC.  Azimuthal anisotropies of muons from charm and bottom hadron decays are measured in Pb+Pb collisions at 5.02 TeV. The data were collected with the ATLAS detector at the Large Hadron Collider in 2015 and 2018 with integrated luminosities of 0.5 nb^{-1} and 1.4 nb^{-1}, respectively. The kinematic selection for heavy-flavor muons requires transverse momentum 4 <pT< 30 GeV and pseudorapidity |\u03b7|< 2.0. The dominant sources of muons in this pT range are semi-leptonic decays of charm and bottom hadrons. These heavy-flavor muons are separated from light-hadron decay muons and punch-through hadrons using the momentum imbalance between the tracking and muon spectrometers. Azimuthal anisotropies, quantified by flow coefficients, are measured via the event-plane method for inclusive heavy-flavor muons as a function of the muon pT and in intervals of Pb+Pb collision centrality. Heavy-flavor muons are separated into contributions from charm and bottom hadron decays using the muon transverse impact parameter with respect to the event primary vertex. Non-zero elliptic (v2) and triangular (v3) flow coefficients are extracted for charm and bottom muons, with the charm muon coefficients larger than those for bottom muons for all Pb+Pb collision centralities. The results indicate substantial modification to the charm and bottom quark angular distributions through interactions in the quark-gluon plasma produced in these Pb+Pb collisions, with smaller modifications for the bottom quarks as expected theoretically due to their larger mass.","name":"Measurement of azimuthal anisotropy of muons from charm and bottom hadrons in Pb+Pb collisions at $\\sqrt{s_\\mathrm{NN}} = 5.02$ TeV with the ATLAS detector","url":"https://www.hepdata.net/record/ins1784454?version=1"},"keywords":"P P --> HF muon + X, v2, 5020.0, Inclusive HF muon, v2, Proton-Proton Collision","name":"Table 1","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/95736","version":1}