Measurement of azimuthal anisotropy of muons from charm and bottom hadrons in Pb+Pb collisions at √sNN=5.02 TeV with the ATLAS detector
Aad, Georges; Abbott, Brad; Abbott, Dale C.; Abed Abud, Adam; Abeling, Kira; Abhayasinghe, Deshan Kavishka; Abidi, Syed Haider; AbouZeid, Hass; Abraham, Nadine L.; Abramowicz, Halina; Bjørke, Kristian; Bugge, Magnar Kopangen; Cameron, David Gordon; Catmore, James Richard; Garonne, Vincent; Gramstad, Eirik; Hellesund, Simen; Morisbak, Vanja; Oppen, Henrik; Ould-Saada, Farid; Pedersen, Maiken; Read, Alexander Lincoln; Rye, Eli Bæverfjord; Røhne, Ole Myren; Sandaker, Heidi; Vadla, Knut Oddvar Høie; Buanes, Trygve; Djuvsland, Julia Isabell; Eigen, Gerald; Fomin, Nikolai; Lee, Graham Richard; Lipniacka, Anna; Martin dit Latour, Bertrand; Stugu, Bjarne; Træet, Are Sivertsen; Abreu, Henso; Abulaiti, Yiming; Acharya, Bobby S.; Achkar, Baida; Adachi, Shunsuke; Adam, Lennart; Adam-Bourdarios, Claire; Adamczyk, Leszek; Adamek, Lukas; Adelman, Jareed; Adersberger, Michael; Adigüzel, Aytül; Adorni, Sofia; Adye, Tim; Affolder, Anthony Allen; ATLAS, Collaboration
Journal article, Peer reviewed
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Date
2020-08-10Metadata
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Abstract
Azimuthal anisotropies of muons from charm and bottom hadron decays are measured in Pb+Pb collisions
at √sNN = 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
|η| < 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 measurements in the tracking detector and in the
muon spectrometers. Azimuthal anisotropies, quantified by flow coefficients, are measured via the eventplane 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.