Abstract

ATLAS measurements of the production of muons from heavy-flavor decays in $\sqrt{s_{\mathrm{NN}}} = 2.76$ TeV Pb+Pb collisions and $\sqrt{s} = 2.76$ TeV $pp$ collisions at the LHC are presented. Integrated luminosities of 0.14 $\mathrm{nb}^{-1}$ and 570 $\mathrm{nb}^{-1}$ are used for the Pb+Pb and $pp$ measurements, respectively, which are performed over the muon transverse momentum range $4 < p_{\mathrm{T}} < 14$ GeV and for five Pb+Pb centrality intervals. Backgrounds arising from in-flight pion and kaon decays, hadronic showers, and mis-reconstructed muons are statistically removed using a template-fitting procedure. The heavy-flavor muon differential cross-sections and per-event yields are measured in $pp$ and Pb+Pb collisions, respectively. The nuclear modification factor $R_{\mathrm{AA}}$ obtained from these is observed to be independent of $p_{\mathrm{T}}$, within uncertainties, and to be less than unity, which indicates suppressed production of heavy-flavor muons in Pb+Pb collisions. For the 10% most central Pb+Pb events, the measured $R_{\mathrm{AA}}$ is approximately 0.35. The azimuthal modulation of the heavy-flavor muon yields is also measured and the associated Fourier coefficients $v_n$ for $n =$ 2, 3 and 4 are given as a function of $p_{\mathrm{T}}$ and centrality. They vary slowly with $p_{\mathrm{T}}$ and show a systematic variation with centrality which is characteristic of other anisotropy measurements, such as that observed for inclusive hadrons. The measured $R_{\mathrm{AA}}$ and $v_n$ values are also compared with theoretical calculations.

Highlights

  • Heavy quarks, especially bottom quarks, provide an important probe of the properties of the quark-gluon plasma created in high-energy nuclear (A+A) collisions [1,2,3,4,5,6,7,8]

  • For the results presented in this paper, the minimum-bias ETFCal distribution is divided into centrality intervals according to the following percentiles of the ETFCal distribution ordered from the most central to the most peripheral col

  • The measured cross sections are compared with fixed-order plus next-to-leadinglogarithm (FONLL) [75,76,77,78] calculations using CTEQ 6.6 PDFs [79]

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Summary

INTRODUCTION

Especially bottom quarks, provide an important probe of the properties of the quark-gluon plasma created in high-energy nuclear (A+A) collisions [1,2,3,4,5,6,7,8]. Separate measurements of the production of forward heavy-flavor electrons [47] and muons [20] that are predominantly produced in semileptonic B- and D-meson decays give RAA values that are significantly larger than those observed for inclusive hadrons. Measurements of inclusive [49,50,51,52,53] and identified hadron [54,55] vn values in A+A collisions at the LHC and at RHIC show the presence of significant azimuthal anisotropies, which are well reproduced by hydrodynamic calculations These results provide the basis for the interpretation that the medium created in heavy-ion collisions is strongly coupled.

ATLAS DETECTOR
Event selection
Muon reconstruction
Heavy-flavor-suppression measurement
Background
Necvetnt
Azimuthal anisotropy measurement
Jet bias in the vn measurement
SYSTEMATIC UNCERTAINTIES
Systematic uncertainties in vn
Heavy-flavor muon RAA
Comparison with theoretical models
CONCLUSION
Methods
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