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CMS-HIN-21-008 ; CERN-EP-2023-052
Measurements of the azimuthal anisotropy of prompt and nonprompt charmonia in PbPb collisions at sNN= 5.02 TeV
JHEP 10 (2023) 115
Abstract: The second-order (v2) and third-order (v3) Fourier coefficients describing the azimuthal anisotropy of prompt and nonprompt (from b-hadron decays) J/ψ, as well as prompt ψ(2S) mesons are measured in lead-lead collisions at a center-of-mass energy per nucleon pair of sNN= 5.02 TeV. The analysis uses a data set corresponding to an integrated luminosity of 1.61 nb1 recorded with the CMS detector. The J/ψ and ψ(2S) mesons are reconstructed using their dimuon decay channel. The v2 and v3 coefficients are extracted using the scalar product method and studied as functions of meson transverse momentum and collision centrality. The measured v2 values for prompt J/ψ mesons are found to be larger than those for nonprompt J/ψ mesons. The prompt J/ψ v2 values at high pT are found to be underpredicted by a model incorporating only parton energy loss effects in a quark-gluon plasma medium. Prompt and nonprompt J/ψ meson v3 and prompt ψ(2S) v2 and v3 values are also reported for the first time, providing new information about heavy quark interactions in the hot and dense medium created in heavy ion collisions.
Figures & Tables Summary References CMS Publications
Figures

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Figure 1:
Invariant mass (left) and J/ψ (right) distributions for the bin of 3.0 <pT< 4.5 GeV/c and 0.0 <v2< 0.3 in centrality 10-60%. The solid lines represent the total fit, while the dashed and dash-dotted lines represent the prompt and nonprompt components, respectively. The background contributions are shown by the filled blue histograms.

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Figure 1-a:
Invariant mass distribution for the bin of 3.0 <pT< 4.5 GeV/c and 0.0 <v2< 0.3 in centrality 10-60%. The solid line represents the total fit, while the dashed and dash-dotted lines represent the prompt and nonprompt components, respectively. The background contributions are shown by the filled blue histogram.

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Figure 1-b:
J/ψ distribution for the bin of 3.0 <pT< 4.5 GeV/c and 0.0 <v2< 0.3 in centrality 10-60%. The solid line represents the total fit, while the dashed and dash-dotted lines represent the prompt and nonprompt components, respectively. The background contributions are shown by the filled blue histogram.

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Figure 2:
Simultaneous fits of the dimuon invariant mass spectrum and the vSig+Bkg2 (left) and vSig+Bkg3 (right) distributions for ψ(2S) mesons, as defined by Eq. (5), for 6.5 <pT< 10 GeV/c and centrality 10-60%. In the upper panel, the solid black (signal + background) and dashed blue (background only) lines show the result of the mass fit. In the lower panel, the vertical lines of the vSign points represent the statistical uncertainty. The solid (vn signal + background) and the dashed (vn background) lines indicate the corresponding fit to the vn distributions.

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Figure 2-a:
Simultaneous fits of the dimuon invariant mass spectrum and the vSig+Bkg2 distribution for ψ(2S) mesons, as defined by Eq. (5), for 6.5 <pT< 10 GeV/c and centrality 10-60%. In the upper panel, the solid black (signal + background) and dashed blue (background only) lines show the result of the mass fit. In the lower panel, the vertical lines of the vSig2 points represent the statistical uncertainty. The solid (v2 signal + background) and the dashed (v2 background) lines indicate the corresponding fit to the v2 distribution.

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Figure 2-b:
Simultaneous fits of the dimuon invariant mass spectrum and the vSig+Bkg2 distribution for ψ(2S) mesons, as defined by Eq. (5), for 6.5 <pT< 10 GeV/c and centrality 10-60%. In the upper panel, the solid black (signal + background) and dashed blue (background only) lines show the result of the mass fit. In the lower panel, the vertical lines of the vSig3 points represent the statistical uncertainty. The solid (v3 signal + background) and the dashed (v3 background) lines indicate the corresponding fit to the v3 distribution.

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Figure 3:
The v2 (upper) and v3 (lower) values, as functions of pT (left) and Npart (right) for prompt and nonprompt J/ψ mesons. The results for 3 <pT< 6.5 and 6.5 <pT< 50 GeV/c are studied in the rapidity range of 1.6 <|y|< 2.4 and |y|< 2.4, respectively (left). The kinematic range for the right panel is 6.5 <pT< 50 GeV/c and |y|< 2.4. The data points are positioned in the middle of each pT bin. The vertical bars denote the statistical uncertainties and the rectangular bands show the systematic uncertainties.

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Figure 4:
The v2 values of prompt J/ψ mesons (blue circles) as a function of pT in the 10-60% centrality range compared with a model calculation in Ref. [31] (green dashed line). The results for 3 <pT< 6.5 and 6.5 <pT< 50 GeV/c are studied in the rapidity range of 1.6 <|y|< 2.4 and |y|< 2.4, respectively. The vertical bars denote the statistical uncertainties and the rectangular bands show the systematic uncertainties.

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Figure 5:
The v2 (upper) and v3 (lower) values, as functions of pT (left) and Npart (right) for prompt J/ψ (blue circles) and prompt ψ(2S) (green squares) mesons. The results for pT< 6.5 and pT> 6.5 GeV/c are studied in the rapidity range of 1.6 <|y|< 2.4 and |y|< 2.4, respectively (left). The kinematic range for the right panel is 6.5 <pT< 50 GeV/c and |y|< 2.4. The data points are positioned in the middle of each pT bin. The vertical bars denote the statistical uncertainties and the rectangular bands show the systematic uncertainties.
Tables

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Table 1:
Summary of the absolute total systematic uncertainty and its dominant contributions, in units of 103.

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Table 2:
A Summary of the kinematic regions for J/ψ and ψ(2S) in the centrality interval 10-60%.

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Table 3:
The centrality classes and Npart values for PbPb collisions at sNN= 5.02 TeV used in this study.
Summary
The second-order (v2) and third-order (v3) Fourier coefficients of azimuthal distributions for prompt and nonprompt J/ψ, and prompt ψ(2S) mesons are measured in PbPb collisions as functions of transverse momentum (pT) and event centrality. The v2 values for prompt and nonprompt J/ψ mesons both indicate a decreasing trend from mid-central towards central collision events. Within present experimental uncertainties, these v2 values show no clear pT dependence between 3 and 50 GeVc. The prompt J/ψ meson v2 values are found to be larger than those of nonprompt J/ψ mesons throughout the studied kinematic region, suggesting different in-medium effects for charm and bottom quarks. The prompt J/ψ meson v2 values are larger than those from a model calculation which considered the prompt J/ψ production above 10 GeVc from jet fragmentation. This discrepancy indicates additional effects are required to describe the observed sizable v2 at high pT for prompt J/ψ mesons. The v3 values for prompt and nonprompt J/ψ mesons are reported for the first time, and found to be consistent with zero in the measured pT and centrality intervals. The v2 and v3 values are also measured for prompt ψ(2S) mesons and are compatible with, although slightly larger than, those of prompt J/ψ mesons. These J/ψ and ψ(2S) meson measurements provide new information about heavy quark interactions in the hot and dense medium created in heavy ion collisions.
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