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CMS-PAS-HIN-24-015
Exploring the origin of $ \mathrm{D^0} $ meson elliptic flow in PbPb collisions at $ \sqrt{\smash[b]{s_{_{\mathrm{NN}}}}}= $ 5.02 TeV using event shape engineering
Abstract: The effect of the initial collision geometry on the elliptic flow ($ v_2 $) in events with prompt $ \mathrm{D^0} $ mesons produced in PbPb collisions at $ \sqrt{\smash[b]{s_{_{\mathrm{NN}}}}}= $ 5.02 TeV is studied using data from the CMS experiment. Using an event-shape engineering technique, initial-state eccentricities within a given centrality range are systematically varied. The $ v_2 $ of $ \mathrm{D^0} $ mesons is measured in five centrality classes, 0-10, 10-20, 20-30, 30-40 and 40-50$ % $ and further categorized into ten event-shape classes based on the reduced flow vector ($ q_2 $) within each centrality range. The measurement is performed within the kinematic region of $ \mathrm{D^0} $ rapidity, $ \lvert y \rvert < $ 1 and transverse momentum ($ p_{\mathrm{T}} $) of 2-30 GeV/$c$. A clear positive correlation is observed between the $ q_2 $ and the $ \mathrm{D^0} v_2 $, indicating that the initial-state geometry significantly influences the development of charm-hadron flow in heavy-ion collisions. Furthermore, a comparison between the $ v_2 $ of $ \mathrm{D^0} $ mesons and that of low-$ p_{\mathrm{T}} $ (1-3 GeV/$c$) charged particles reveals a linear correlation, strongly suggesting that initial-geometry eccentricity is the primary origin of the charm-hadron elliptic flow, and hints of nonlinearity are observed at $ \mathrm{D^0} p_{\mathrm{T}} > $ 10 GeV/$c$.
Figures & Tables Summary References CMS Publications
Figures

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Figure 1:
Correlation between the normalized $ \mathrm{D^0} v_2 $ and the charged-particle $ v_2 $. The $ v_2 $ value in each $ q_2 $ bin is scaled by the $ q_2 $-inclusive $ v_2 $. The charged-particle $ v_2 $ is measured in the $ p_{\mathrm{T}} $ region 1-3 GeV/$c$. The correlation plots for $ \mathrm{D^0} p_{\mathrm{T}} $ 2-4 (upper left), 4-6 (upper right), 6-10 (lower left) and 10-30 GeV/$c$ (lower right) in the centrality class 20-30%. The red band corresponds to the uncertainty of one standard deviation.

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Figure 1-a:
Correlation between the normalized $ \mathrm{D^0} v_2 $ and the charged-particle $ v_2 $. The $ v_2 $ value in each $ q_2 $ bin is scaled by the $ q_2 $-inclusive $ v_2 $. The charged-particle $ v_2 $ is measured in the $ p_{\mathrm{T}} $ region 1-3 GeV/$c$. The correlation plots for $ \mathrm{D^0} p_{\mathrm{T}} $ 2-4 (upper left), 4-6 (upper right), 6-10 (lower left) and 10-30 GeV/$c$ (lower right) in the centrality class 20-30%. The red band corresponds to the uncertainty of one standard deviation.

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Figure 1-b:
Correlation between the normalized $ \mathrm{D^0} v_2 $ and the charged-particle $ v_2 $. The $ v_2 $ value in each $ q_2 $ bin is scaled by the $ q_2 $-inclusive $ v_2 $. The charged-particle $ v_2 $ is measured in the $ p_{\mathrm{T}} $ region 1-3 GeV/$c$. The correlation plots for $ \mathrm{D^0} p_{\mathrm{T}} $ 2-4 (upper left), 4-6 (upper right), 6-10 (lower left) and 10-30 GeV/$c$ (lower right) in the centrality class 20-30%. The red band corresponds to the uncertainty of one standard deviation.

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Figure 1-c:
Correlation between the normalized $ \mathrm{D^0} v_2 $ and the charged-particle $ v_2 $. The $ v_2 $ value in each $ q_2 $ bin is scaled by the $ q_2 $-inclusive $ v_2 $. The charged-particle $ v_2 $ is measured in the $ p_{\mathrm{T}} $ region 1-3 GeV/$c$. The correlation plots for $ \mathrm{D^0} p_{\mathrm{T}} $ 2-4 (upper left), 4-6 (upper right), 6-10 (lower left) and 10-30 GeV/$c$ (lower right) in the centrality class 20-30%. The red band corresponds to the uncertainty of one standard deviation.

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Figure 1-d:
Correlation between the normalized $ \mathrm{D^0} v_2 $ and the charged-particle $ v_2 $. The $ v_2 $ value in each $ q_2 $ bin is scaled by the $ q_2 $-inclusive $ v_2 $. The charged-particle $ v_2 $ is measured in the $ p_{\mathrm{T}} $ region 1-3 GeV/$c$. The correlation plots for $ \mathrm{D^0} p_{\mathrm{T}} $ 2-4 (upper left), 4-6 (upper right), 6-10 (lower left) and 10-30 GeV/$c$ (lower right) in the centrality class 20-30%. The red band corresponds to the uncertainty of one standard deviation.

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Figure 2:
Slopes obtained from the correlation plots of the prompt $ \mathrm{D^0} v_2 $ vs the charged-particle $ v_2 $ for each $ p_{\mathrm{T}} $ and centrality class of $ \mathrm{D^0} $. For the correlation plots, the $ v_2 $ in each $ q_2 $ bin is normalized by the $ q_2 $-inclusive $ v_2 $. The vertical lines correspond to the statistical uncertainties and the vertical bands correspond to the systematic uncertainties added in quadrature. The slopes calculated are consistent with unity.

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Figure 3:
Intercepts obtained from the correlation plots of the prompt $ \mathrm{D^0} v_2 $ vs the charged-particle $ v_2 $ for each $ p_{\mathrm{T}} $ and centrality class of $ \mathrm{D^0} $. For the correlation plots, the $ v_2 $ in each $ q_2 $ bin is normalized by the $ q_2 $-inclusive $ v_2 $. The vertical lines correspond to the statistical uncertainties and the vertical bands correspond to the systematic uncertainties added in quadrature. The intercepts calculated are consistent with zero.

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Figure 4:
Correlation between the normalized $ \mathrm{D^0} v_2 $ and the charged-particle $ v_2 $. The $ v_2 $ value in each $ q_2 $ bin is scaled by the $ q_2 $-inclusive $ v_2 $. The charged-particle $ v_2 $ is measured in the $ p_{\mathrm{T}} $ region 1-3 GeV/$c$. The correlation plots for $ \mathrm{D^0} p_{\mathrm{T}} $ 2-4 (upper left), 4-6 (upper right), 6-10 (lower left) and 10-30 GeV/$c$ (lower right) in the centrality class 0-10%. The red band corresponds to the uncertainty of one standard deviation.

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Figure 4-a:
Correlation between the normalized $ \mathrm{D^0} v_2 $ and the charged-particle $ v_2 $. The $ v_2 $ value in each $ q_2 $ bin is scaled by the $ q_2 $-inclusive $ v_2 $. The charged-particle $ v_2 $ is measured in the $ p_{\mathrm{T}} $ region 1-3 GeV/$c$. The correlation plots for $ \mathrm{D^0} p_{\mathrm{T}} $ 2-4 (upper left), 4-6 (upper right), 6-10 (lower left) and 10-30 GeV/$c$ (lower right) in the centrality class 0-10%. The red band corresponds to the uncertainty of one standard deviation.

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Figure 4-b:
Correlation between the normalized $ \mathrm{D^0} v_2 $ and the charged-particle $ v_2 $. The $ v_2 $ value in each $ q_2 $ bin is scaled by the $ q_2 $-inclusive $ v_2 $. The charged-particle $ v_2 $ is measured in the $ p_{\mathrm{T}} $ region 1-3 GeV/$c$. The correlation plots for $ \mathrm{D^0} p_{\mathrm{T}} $ 2-4 (upper left), 4-6 (upper right), 6-10 (lower left) and 10-30 GeV/$c$ (lower right) in the centrality class 0-10%. The red band corresponds to the uncertainty of one standard deviation.

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Figure 4-c:
Correlation between the normalized $ \mathrm{D^0} v_2 $ and the charged-particle $ v_2 $. The $ v_2 $ value in each $ q_2 $ bin is scaled by the $ q_2 $-inclusive $ v_2 $. The charged-particle $ v_2 $ is measured in the $ p_{\mathrm{T}} $ region 1-3 GeV/$c$. The correlation plots for $ \mathrm{D^0} p_{\mathrm{T}} $ 2-4 (upper left), 4-6 (upper right), 6-10 (lower left) and 10-30 GeV/$c$ (lower right) in the centrality class 0-10%. The red band corresponds to the uncertainty of one standard deviation.

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Figure 4-d:
Correlation between the normalized $ \mathrm{D^0} v_2 $ and the charged-particle $ v_2 $. The $ v_2 $ value in each $ q_2 $ bin is scaled by the $ q_2 $-inclusive $ v_2 $. The charged-particle $ v_2 $ is measured in the $ p_{\mathrm{T}} $ region 1-3 GeV/$c$. The correlation plots for $ \mathrm{D^0} p_{\mathrm{T}} $ 2-4 (upper left), 4-6 (upper right), 6-10 (lower left) and 10-30 GeV/$c$ (lower right) in the centrality class 0-10%. The red band corresponds to the uncertainty of one standard deviation.

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Figure 5:
Correlation between the normalized $ \mathrm{D^0} v_2 $ and the charged-particle $ v_2 $. The $ v_2 $ value in each $ q_2 $ bin is scaled by the $ q_2 $-inclusive $ v_2 $. The charged-particle $ v_2 $ is measured in the $ p_{\mathrm{T}} $ region 1-3 GeV/$c$. The correlation plots for $ \mathrm{D^0} p_{\mathrm{T}} $ 2-4 (upper left), 4-6 (upper right), 6-10 (lower left) and 10-30 GeV/$c$ (lower right) in the centrality class 10-20%. The red band corresponds to the uncertainty of one standard deviation.

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Figure 5-a:
Correlation between the normalized $ \mathrm{D^0} v_2 $ and the charged-particle $ v_2 $. The $ v_2 $ value in each $ q_2 $ bin is scaled by the $ q_2 $-inclusive $ v_2 $. The charged-particle $ v_2 $ is measured in the $ p_{\mathrm{T}} $ region 1-3 GeV/$c$. The correlation plots for $ \mathrm{D^0} p_{\mathrm{T}} $ 2-4 (upper left), 4-6 (upper right), 6-10 (lower left) and 10-30 GeV/$c$ (lower right) in the centrality class 10-20%. The red band corresponds to the uncertainty of one standard deviation.

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Figure 5-b:
Correlation between the normalized $ \mathrm{D^0} v_2 $ and the charged-particle $ v_2 $. The $ v_2 $ value in each $ q_2 $ bin is scaled by the $ q_2 $-inclusive $ v_2 $. The charged-particle $ v_2 $ is measured in the $ p_{\mathrm{T}} $ region 1-3 GeV/$c$. The correlation plots for $ \mathrm{D^0} p_{\mathrm{T}} $ 2-4 (upper left), 4-6 (upper right), 6-10 (lower left) and 10-30 GeV/$c$ (lower right) in the centrality class 10-20%. The red band corresponds to the uncertainty of one standard deviation.

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Figure 5-c:
Correlation between the normalized $ \mathrm{D^0} v_2 $ and the charged-particle $ v_2 $. The $ v_2 $ value in each $ q_2 $ bin is scaled by the $ q_2 $-inclusive $ v_2 $. The charged-particle $ v_2 $ is measured in the $ p_{\mathrm{T}} $ region 1-3 GeV/$c$. The correlation plots for $ \mathrm{D^0} p_{\mathrm{T}} $ 2-4 (upper left), 4-6 (upper right), 6-10 (lower left) and 10-30 GeV/$c$ (lower right) in the centrality class 10-20%. The red band corresponds to the uncertainty of one standard deviation.

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Figure 5-d:
Correlation between the normalized $ \mathrm{D^0} v_2 $ and the charged-particle $ v_2 $. The $ v_2 $ value in each $ q_2 $ bin is scaled by the $ q_2 $-inclusive $ v_2 $. The charged-particle $ v_2 $ is measured in the $ p_{\mathrm{T}} $ region 1-3 GeV/$c$. The correlation plots for $ \mathrm{D^0} p_{\mathrm{T}} $ 2-4 (upper left), 4-6 (upper right), 6-10 (lower left) and 10-30 GeV/$c$ (lower right) in the centrality class 10-20%. The red band corresponds to the uncertainty of one standard deviation.

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Figure 6:
Correlation between the normalized $ \mathrm{D^0} v_2 $ and the charged-particle $ v_2 $. The $ v_2 $ value in each $ q_2 $ bin is scaled by the $ q_2 $-inclusive $ v_2 $. The charged-particle $ v_2 $ is measured in the $ p_{\mathrm{T}} $ region 1-3 GeV/$c$. The correlation plots for $ \mathrm{D^0} p_{\mathrm{T}} $ 2-4 (upper left), 4-6 (upper right), 6-10 (lower left) and 10-30 GeV/$c$ (lower right) in the centrality class 30-40%. The red band corresponds to the uncertainty of one standard deviation.

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Figure 6-a:
Correlation between the normalized $ \mathrm{D^0} v_2 $ and the charged-particle $ v_2 $. The $ v_2 $ value in each $ q_2 $ bin is scaled by the $ q_2 $-inclusive $ v_2 $. The charged-particle $ v_2 $ is measured in the $ p_{\mathrm{T}} $ region 1-3 GeV/$c$. The correlation plots for $ \mathrm{D^0} p_{\mathrm{T}} $ 2-4 (upper left), 4-6 (upper right), 6-10 (lower left) and 10-30 GeV/$c$ (lower right) in the centrality class 30-40%. The red band corresponds to the uncertainty of one standard deviation.

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Figure 6-b:
Correlation between the normalized $ \mathrm{D^0} v_2 $ and the charged-particle $ v_2 $. The $ v_2 $ value in each $ q_2 $ bin is scaled by the $ q_2 $-inclusive $ v_2 $. The charged-particle $ v_2 $ is measured in the $ p_{\mathrm{T}} $ region 1-3 GeV/$c$. The correlation plots for $ \mathrm{D^0} p_{\mathrm{T}} $ 2-4 (upper left), 4-6 (upper right), 6-10 (lower left) and 10-30 GeV/$c$ (lower right) in the centrality class 30-40%. The red band corresponds to the uncertainty of one standard deviation.

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Figure 6-c:
Correlation between the normalized $ \mathrm{D^0} v_2 $ and the charged-particle $ v_2 $. The $ v_2 $ value in each $ q_2 $ bin is scaled by the $ q_2 $-inclusive $ v_2 $. The charged-particle $ v_2 $ is measured in the $ p_{\mathrm{T}} $ region 1-3 GeV/$c$. The correlation plots for $ \mathrm{D^0} p_{\mathrm{T}} $ 2-4 (upper left), 4-6 (upper right), 6-10 (lower left) and 10-30 GeV/$c$ (lower right) in the centrality class 30-40%. The red band corresponds to the uncertainty of one standard deviation.

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Figure 6-d:
Correlation between the normalized $ \mathrm{D^0} v_2 $ and the charged-particle $ v_2 $. The $ v_2 $ value in each $ q_2 $ bin is scaled by the $ q_2 $-inclusive $ v_2 $. The charged-particle $ v_2 $ is measured in the $ p_{\mathrm{T}} $ region 1-3 GeV/$c$. The correlation plots for $ \mathrm{D^0} p_{\mathrm{T}} $ 2-4 (upper left), 4-6 (upper right), 6-10 (lower left) and 10-30 GeV/$c$ (lower right) in the centrality class 30-40%. The red band corresponds to the uncertainty of one standard deviation.

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Figure 7:
Correlation between the normalized $ \mathrm{D^0} v_2 $ and the charged-particle $ v_2 $. The $ v_2 $ value in each $ q_2 $ bin is scaled by the $ q_2 $-inclusive $ v_2 $. The charged-particle $ v_2 $ is measured in the $ p_{\mathrm{T}} $ region 1-3 GeV/$c$. The correlation plots for $ \mathrm{D^0} p_{\mathrm{T}} $ 2-4 (upper left), 4-6 (upper right), 6-10 (lower left) and 10-30 GeV/$c$ (lower right) in the centrality class 40-50%. The red band corresponds to the uncertainty of one standard deviation.

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Figure 7-a:
Correlation between the normalized $ \mathrm{D^0} v_2 $ and the charged-particle $ v_2 $. The $ v_2 $ value in each $ q_2 $ bin is scaled by the $ q_2 $-inclusive $ v_2 $. The charged-particle $ v_2 $ is measured in the $ p_{\mathrm{T}} $ region 1-3 GeV/$c$. The correlation plots for $ \mathrm{D^0} p_{\mathrm{T}} $ 2-4 (upper left), 4-6 (upper right), 6-10 (lower left) and 10-30 GeV/$c$ (lower right) in the centrality class 40-50%. The red band corresponds to the uncertainty of one standard deviation.

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Figure 7-b:
Correlation between the normalized $ \mathrm{D^0} v_2 $ and the charged-particle $ v_2 $. The $ v_2 $ value in each $ q_2 $ bin is scaled by the $ q_2 $-inclusive $ v_2 $. The charged-particle $ v_2 $ is measured in the $ p_{\mathrm{T}} $ region 1-3 GeV/$c$. The correlation plots for $ \mathrm{D^0} p_{\mathrm{T}} $ 2-4 (upper left), 4-6 (upper right), 6-10 (lower left) and 10-30 GeV/$c$ (lower right) in the centrality class 40-50%. The red band corresponds to the uncertainty of one standard deviation.

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Figure 7-c:
Correlation between the normalized $ \mathrm{D^0} v_2 $ and the charged-particle $ v_2 $. The $ v_2 $ value in each $ q_2 $ bin is scaled by the $ q_2 $-inclusive $ v_2 $. The charged-particle $ v_2 $ is measured in the $ p_{\mathrm{T}} $ region 1-3 GeV/$c$. The correlation plots for $ \mathrm{D^0} p_{\mathrm{T}} $ 2-4 (upper left), 4-6 (upper right), 6-10 (lower left) and 10-30 GeV/$c$ (lower right) in the centrality class 40-50%. The red band corresponds to the uncertainty of one standard deviation.

png pdf
Figure 7-d:
Correlation between the normalized $ \mathrm{D^0} v_2 $ and the charged-particle $ v_2 $. The $ v_2 $ value in each $ q_2 $ bin is scaled by the $ q_2 $-inclusive $ v_2 $. The charged-particle $ v_2 $ is measured in the $ p_{\mathrm{T}} $ region 1-3 GeV/$c$. The correlation plots for $ \mathrm{D^0} p_{\mathrm{T}} $ 2-4 (upper left), 4-6 (upper right), 6-10 (lower left) and 10-30 GeV/$c$ (lower right) in the centrality class 40-50%. The red band corresponds to the uncertainty of one standard deviation.
Tables

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Table 1:
Summary of systematic uncertainties in the absolute differences between the nominal and the alternative analyses for the slope and intercept of the correlation plots.
Summary
In this study, a clear correlation between the initial collision geometry is demonstrated, characterized by the reduced flow vector, and the elliptic flow of prompt $ \mathrm{D^0} $ mesons in PbPb collisions at $ \sqrt{\smash[b]{s_{_{\mathrm{NN}}}}}= $ 5.02 TeV. By employing event-shape engineering to systematically vary initial-state eccentricities, we have shown that the $ \mathrm{D^0} $ meson $ v_2 $ is strongly correlated to the eccentricity ($ \epsilon_2 $) of the initial geometry. This observation, coupled with the observed correlation between $ \mathrm{D^0} v_2 $ and charged-particle $ v_2 $ within the $ p_{\mathrm{T}} $ range 1-3 GeV/$c$, reinforces the conclusion that the initial geometry eccentricity is the dominant source of charm-hadron elliptic flow. This correlation is approximately linear and exists in the centrality region of 0-50% (10% classes) and for both low (2-10 GeV/$c$) and high-$ p_{\mathrm{T}} $ (10-30 GeV/$c$) of $ \mathrm{D^0} $-meson. A nonlinear correlation, specifically for high $ \mathrm{D^0} p_{\mathrm{T}} $ may be an indication of the path-length dependent energy-loss of charm quark in the QGP medium. These findings provide compelling evidence for the significant role of initial-state geometry in shaping the collective flow of heavy quarks within the quark-gluon plasma created in heavy-ion collisions.
References
1 E. V. Shuryak Theory of Hadronic Plasma Sov. Phys. JETP 47 (1978) 212
2 U. Heinz and R. Snellings Collective flow and viscosity in relativistic heavy-ion collisions Ann. Rev. Nucl. Part. Sci. 63 (2013) 123 1301.2826
3 S. Voloshin and Y. Zhang Flow study in relativistic nuclear collisions by fourier expansion of azimuthal particle distributions Z. Phys. C 70 (1996) 665 hep-ph/9407282
4 W. Busza, K. Rajagopal, and W. van der Schee Heavy ion collisions: The big picture, and the big questions Ann. Rev. Nucl. Part. Sci. 68 (2018) 339 1802.04801
5 J. Takahashi et al. Topology studies of hydrodynamics using two particle correlation analysis PRL 103 (2009) 242301 0902.4870
6 B. Alver and G. Roland Collision geometry fluctuations and triangular flow in heavy-ion collisions [Erratum: Phys.Rev.C 82, 039903]
PRC 81 (2010) 054905
1003.0194
7 F. G. Gardim, F. Grassi, M. Luzum, and J.-Y. Ollitrault Mapping the hydrodynamic response to the initial geometry in heavy-ion collisions PRC 85 (2012) 024908 1111.6538
8 H. Niemi, G. S. Denicol, H. Holopainen, and P. Huovinen Event-by-event distributions of azimuthal asymmetries in ultrarelativistic heavy-ion collisions PRC 87 (2013) 054901 1212.1008
9 F. G. Gardim, J. Noronha-Hostler, M. Luzum, and F. Grassi Effects of viscosity on the mapping of initial to final state in heavy ion collisions PRC 91 (2015) 034902 1411.2574
10 PHENIX Collaboration Heavy quark production in $ p+p $ and energy loss and flow of heavy quarks in Au+Au collisions at $ \sqrt {\smash [b]{s_{_{\mathrm {NN}}}}}= $ 200 GeV PRC 84 (2011) 044905 1005.1627
11 STAR Collaboration Elliptic flow of electrons from heavy-flavor hadron decays in Au+Au collisions at $ \sqrt {\smash [b]{s_{_{\mathrm {NN}}}}} = $ 200, 62.4, and 39 GeV PRC 95 (2017) 034907 1405.6348
12 STAR Collaboration Measurement of $ D^0 $ azimuthal anisotropy at midrapidity in Au+Au collisions at $ \sqrt {\smash [b]{s_{_{\mathrm {NN}}}}}= $ 200 GeV PRL 118 (2017) 212301 1701.06060
13 ALICE Collaboration Azimuthal anisotropy of $ D $-meson production in Pb-Pb collisions at $ \sqrt {\smash [b]{s_{_{\mathrm {NN}}}}}= $ 2.76 TeV PRC 90 (2014) 034904 1405.2001
14 ALICE Collaboration $ D $-meson azimuthal anisotropy in midcentral Pb-Pb collisions at $ \sqrt{s_{\rm NN}}= $ 5.02 TeV PRL 120 (2018) 102301 1707.01005
15 CMS Collaboration Probing charm quark dynamics via multiparticle correlations in Pb-Pb collisions at $ \sqrt {\smash [b]{s_{_{\mathrm {NN}}}}} $ = 5.02 TeV PRL 129 (2022) 022001 CMS-HIN-20-001
2112.12236
16 CMS Collaboration Measurement of prompt $ D^0 $ meson azimuthal anisotropy in Pb-Pb collisions at $ \sqrt {\smash [b]{s_{_{\mathrm {NN}}}}} $ = 5.02 TeV PRL 120 (2018) 202301 CMS-HIN-16-007
1708.03497
17 CMS Collaboration Measurement of prompt $ \mathrm{D^0} $ and $ \mathrm{\overline{D}}^{0} $ meson azimuthal anisotropy and search for strong electric fields in PbPb collisions at $ \sqrt {\smash [b]{s_{_{\mathrm {NN}}}}} = $ 5.02 TeV PLB 816 (2021) 136253 CMS-HIN-19-008
2009.12628
18 ALICE Collaboration Event-shape engineering for the D-meson elliptic flow in mid-central Pb-Pb collisions at $ \sqrt{s_{\rm NN}} = $ 5.02 TeV JHEP 02 (2019) 150 1809.09371
19 ALICE Collaboration Transverse-momentum and event-shape dependence of D-meson flow harmonics in Pb-Pb collisions at $ \sqrt{s_{\rm NN}} $ = 5.02 TeV PLB 813 (2021) 136054 2005.11131
20 J. Schukraft, A. Timmins, and S. A. Voloshin Ultra-relativistic nuclear collisions: Event shape engineering PLB 719 (2013) 394 1208.4563
21 CMS Collaboration Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in $ p\mathrm{Pb} $ and PbPb collisions at the CERN Large Hadron Collider PRC 97 (2018) 044912 CMS-HIN-17-001
1708.01602
22 CMS Collaboration Description and performance of track and primary-vertex reconstruction with the CMS tracker JINST 9 (2014) P10009 CMS-TRK-11-001
1405.6569
23 CMS Collaboration The CMS experiment at the CERN LHC JINST 3 (2008) S08004
24 CMS Collaboration Precision luminosity measurement in proton-proton collisions at $ \sqrt{s}= $ 13 TeV in 2015 and 2016 at CMS EPJC 81 (2021) 800 CMS-LUM-17-003
2104.01927
25 CMS Collaboration CMS luminosity measurement using nucleus-nucleus collisions at $ \sqrt{{s}_{\mathrm{NN}}}=5.02\text{ }\text{ }\mathrm{TeV} $ in 2018 CMS Physics Analysis Summary, 2022
CMS-PAS-LUM-18-001
CMS-PAS-LUM-18-001
26 CMS Collaboration The CMS trigger system JINST 12 (2017) P01020 CMS-TRG-12-001
1609.02366
27 CMS Collaboration Charged-particle nuclear modification factors in PbPb and pPb collisions at $ \sqrt{s_{\mathrm{NN}}}= $ 5.02 TeV JHEP 04 (2017) 039 CMS-HIN-15-015
1611.01664
28 T. Sjöstrand et al. An introduction to PYTHIA 8.2 Comput. Phys. Commun. 191 (2015) 159 1410.3012
29 CMS Collaboration Event generator tunes obtained from underlying event and multiparton scattering measurements EPJC 76 (2016) 155 CMS-GEN-14-001
1512.00815
30 D. J. Lange The EvtGen particle decay simulation package NIM A 462 (2001) 152
31 GEANT4 Collaboration GEANT 4---a simulation toolkit NIM A 506 (2003) 250
32 Particle Data Group Collaboration Review of particle physics PRD 110 (2024) 030001
33 A. Hoecker et al. TMVA, the Toolkit for Multivariate Data Analysis with ROOT PoS ACAT 04 (2009) 0 physics/0703039
34 STAR Collaboration Elliptic flow from two- and four-particle correlations in Au+Au collisions at $ \sqrt{s_{\mathrm{NN}}}= $ 130 GeV PRC 66 (2002) 034904 nucl-ex/0206001
35 M. Luzum and J.-Y. Ollitrault Eliminating experimental bias in anisotropic-flow measurements of high-energy nuclear collisions PRC 87 (2013) 044907 1209.2323
36 A. M. Poskanzer and S. A. Voloshin Methods for analyzing anisotropic flow in relativistic nuclear collisions PRC 58 (1998) 1671 nucl-ex/9805001
37 NA49 Collaboration Directed and elliptic flow of charged pions and protons in $ \mathrm{Pb}+\mathrm{Pb} $ collisions at 40 $ A $ and 158 $ A\mathrm{GeV} $ PRC 68 (2003) 034903 nucl-ex/0303001
38 CMS Collaboration Measurements of azimuthal anisotropy of nonprompt $ D^0 $ mesons in PbPb collisions at $ \sqrt{{s}_{\mathrm{NN}}}= $ 5.02 TeV Physics Letters B 850 (2024) 138389 CMS-HIN-21-003
2212.01636
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