{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.95128.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1752509"}},{"@id":"https://doi.org/10.1103/PhysRevLett.124.082301","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2020","description":"CERN-LHC.  The elliptic flow of muons from the decay of charm and bottom hadrons is measured in pp collisions at 13 TeV using a data sample with an integrated luminosity of 150 pb^{-1} recorded by the ATLAS detector at the LHC. The muons from heavy-flavor decay are separated from light-hadron decay muons using momentum imbalance between the tracking and muon spectrometers. The heavy-flavor decay muons are further separated into those from charm decay and those from bottom decay using the distance-of-closest-approach to the collision vertex. The measurement is performed for muons in the transverse momentum range 4 < pT < 7 GeV and pseudorapidity range |\u03b7|<2.4. A significant non-zero elliptic anisotropy coefficient v2 is observed for muons from charm decays, while the v2 value for muons from bottom decays is consistent with zero within uncertainties.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.95128.v1/t1","@type":"Dataset","description":"Summary of results for inclusive muon v2 as a function of multiplicity. Uncertainties are statistical and systematic, respectively.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.95128.v1/t2","@type":"Dataset","description":"Summary of results for inclusive muon v2 as a function of pT. Uncertainties are statistical and systematic, respectively.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.95128.v1/t3","@type":"Dataset","description":"Summary of results for charm and bottom muon v2 as a function of multiplicity. Uncertainties are statistical and systematic, respectively.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.95128.v1/t4","@type":"Dataset","description":"Summary of results for charm and bottom muon v2 as a function of pT. Uncertainties are statistical and systematic, respectively.","name":"Table 4"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1752509?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/95128"}],"inLanguage":"en","name":"Measurement of azimuthal anisotropy of muons from charm and bottom hadrons in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1752509?version=1","version":1}