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Anisotropic flows of light-flavor and charmed hadrons in Pb+Pb collisions at LHC energy

Yan-ting Feng, Rui-qin Wang, Feng-lan Shao, Jun Song

Abstract

We apply a constituent quark equal-velocity combination (EVC) model to study the elliptic flow ($v_{2}$) and triangular flow ($v_{3}$) of light-flavor and single-charmed hadrons in Pb+Pb collisions at $\sqrt{s_{NN}}=$ 2.76 and 5.02 TeV. $v_{2,3}$ of hadrons in the EVC model can be expressed as a linear superposition of the $v_{2,3}$ of quarks at the same velocity as that of the hadrons. We find that available experimental data for $v_{2}$ and $v_{3}$ of $p$, $Λ$, $Ξ$, and $Ω$ as the function of transverse momentum ($p_{T}$) can be consistently explained by the EVC formula using a $v_{2}$ of up/down quarks and a $v_{2}$ of strange quarks. In comparison with $v_{2}$ data of $φ$ at $\sqrt{s_{NN}}=$2.76 TeV which can be naturally explained by $v_{2}$ of strange quarks, explanation of data of $φ$ mesons at $\sqrt{s_{NN}}=$5.02 TeV requires an additional contribution of two-kaon coalescence, which indicates approximately 20% influence of final-state hadronic rescattering on $v_{2}$ of $φ$ at $\sqrt{s_{NN}}=$5.02 TeV. Using $v_{2}$ and $v_{3}$ of light-flavor quarks obtained in studying light-flavor hadrons and $v_{2}$ and $v_{3}$ of charm quarks determined from $D^{0}$ meson data, we apply the EVC model to predict the anisotropic flows of $D_{s}^{+}$, $Λ_{c}^{+}$, $Ξ_{c}^{0}$, and $Ω_{c}^{0}$ and compare them with the available experimental data. The preliminary data for $v_{2}$ of $D^{0}$, $D_{s}^{+}$, and $Λ_{c}^{+}$ at $\sqrt{s_{NN}}=$ 5.36 TeV are found to be naturally described by the EVC model.

Anisotropic flows of light-flavor and charmed hadrons in Pb+Pb collisions at LHC energy

Abstract

We apply a constituent quark equal-velocity combination (EVC) model to study the elliptic flow () and triangular flow () of light-flavor and single-charmed hadrons in Pb+Pb collisions at 2.76 and 5.02 TeV. of hadrons in the EVC model can be expressed as a linear superposition of the of quarks at the same velocity as that of the hadrons. We find that available experimental data for and of , , , and as the function of transverse momentum () can be consistently explained by the EVC formula using a of up/down quarks and a of strange quarks. In comparison with data of at 2.76 TeV which can be naturally explained by of strange quarks, explanation of data of mesons at 5.02 TeV requires an additional contribution of two-kaon coalescence, which indicates approximately 20% influence of final-state hadronic rescattering on of at 5.02 TeV. Using and of light-flavor quarks obtained in studying light-flavor hadrons and and of charm quarks determined from meson data, we apply the EVC model to predict the anisotropic flows of , , , and and compare them with the available experimental data. The preliminary data for of , , and at 5.36 TeV are found to be naturally described by the EVC model.
Paper Structure (11 sections, 21 equations, 13 figures)

This paper contains 11 sections, 21 equations, 13 figures.

Figures (13)

  • Figure 1: $v_{2}$ of quarks as a function of $p_{T}$ in different centralities in Pb+Pb collisions at $\sqrt{s_{NN}}=$2.76 and 5.02 TeV.
  • Figure 2: The $v_{2}$ of (a) $p$, (b) $\Lambda$, (c) $\Xi$, (d) $\Omega,$ and (e) $\phi$ in different centralities in Pb+Pb collisions at $\sqrt{s_{NN}}=$2.76 TeV. Symbols are the experimental data ALICE:2014wao and lines are model results.
  • Figure 3: The $v_{2}$ of (a) $p$, (b) $\Lambda$, (c) $\Xi$, (d) $\Omega,$ and (e) $\phi$ in different centralities in Pb+Pb collisions at $\sqrt{s_{NN}}=$5.02 TeV. Symbols are the experimental data ALICE:2022zksZhu:2019twz and lines are model results.
  • Figure 4: The $v_{2}$ of $\phi$ mesons as a function of $p_{T}$ in Pb+Pb collisions at $\sqrt{s_{NN}}=$5.02 TeV. Experimental data (symbols) are from Refs. ALICE:2022zksZhu:2019twz. Theoretical results including only the $s\overline{s}$ combination are shown as dashed lines and those incorporating both $s\overline{s}$ combination and two-kaon coalescence are shown as solid lines.
  • Figure 5: $v_{3}$ of quarks as a function of $p_{T}$ in different centralities in Pb+Pb collisions at $\sqrt{s_{NN}}=$ 5.02 TeV.
  • ...and 8 more figures