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Azimuthal anisotropy measurement of (multi)strange hadrons in Au+Au collisions at sNN=54.4 GeV

M. S. Abdallah et al. (STAR Collaboration)
Phys. Rev. C 107, 024912 – Published 22 February 2023

Abstract

Azimuthal anisotropy of produced particles is one of the most important observables used to access the collective properties of the expanding medium created in relativistic heavy-ion collisions. In this paper, we present second (v2) and third (v3) order azimuthal anisotropies of KS0, ϕ, Λ, Ξ, and Ω at midrapidity (|y|<1) in Au+Au collisions at sNN=54.4 GeV measured by the STAR detector. The v2 and v3 are measured as a function of transverse momentum and centrality. Their energy dependence is also studied. v3 is found to be more sensitive to the change in the center-of-mass energy than v2. Scaling by constituent quark number is found to hold for v2 within 10%. This observation could be evidence for the development of partonic collectivity in 54.4 GeV Au+Au collisions. Differences in v2 and v3 between baryons and antibaryons are presented, and ratios of v3/v23/2 are studied and motivated by hydrodynamical calculations. The ratio of v2 of ϕ mesons to that of antiprotons [v2(ϕ)/v2(p¯)] shows centrality dependence at low transverse momentum, presumably resulting from the larger effects from hadronic interactions on antiproton v2.

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  • Received 18 May 2022
  • Accepted 12 October 2022

DOI:https://doi.org/10.1103/PhysRevC.107.024912

©2023 American Physical Society

Physics Subject Headings (PhySH)

Nuclear Physics

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Vol. 107, Iss. 2 — February 2023

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Images

  • Figure 1
    Figure 1

    The uncorrected multiplicity distribution of reconstructed charged particles in Au+Au collisions at sNN=54.4 GeV. Glauber Monte Carlo simulation is shown as the solid red curve.

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  • Figure 2
    Figure 2

    Invariant mass distributions for KS0, ϕ, Λ, Ξ, Ω, and their antiparticles in minimum bias Au+Au collisions at sNN=54.4 GeV. The combinatorial background is shown as gray shaded histograms. No background subtraction was included in any of the eight panels.

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  • Figure 3
    Figure 3

    The upper panel shows v2 as a function of the invariant mass of π+π pairs and the lower panel shows the same for v3. Red lines represent fit functions given in Eq. (5).

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  • Figure 4
    Figure 4

    v2 and v3 as a function of pT at midrapidity (|y|<1) for minimum bias events. The vertical lines represent the statistical error bars and the shaded bands represent the systematic uncertainties. Data points for antiparticles are shifted by 0.1 GeV/c towards right for better visibility.

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  • Figure 5
    Figure 5

    v2 as function of pT for 0–10 %, 10–40 %, and 40–80 % centrality events. The vertical lines represent the statistical error bars and the shaded bands represent the systematic uncertainties.

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  • Figure 6
    Figure 6

    v3 as function of pT for 0–10 %, 10–40 %, and 40–80 % centrality events. The vertical lines represent the statistical error bars and the shaded bands represent the systematic uncertainties. 40–80 % centrality data points are not shown for Ξ and Ω due to less statistics.

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  • Figure 7
    Figure 7

    v2 of KS0, ϕ, Λ¯, Ξ¯+, and Ω as a function of pT in 0-80 % centrality events at sNN=39, 54.4, and 200 GeV. The dotted line represents the fit to the 200 GeV data points. The vertical lines represent the sum of statistical and systematic uncertainties in quadrature. The data points for 39 and 200 GeV are taken from Refs. [18, 20, 42].

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  • Figure 8
    Figure 8

    v3 of KS0, ϕ, and Λ¯ as a function of pT in 0–80 % centrality events at sNN=54.4 and 200 GeV. The vertical lines represent the sum of statistical and systematic uncertainties in quadrature. The data points for 200 GeV are taken from Ref. [43].

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  • Figure 9
    Figure 9

    Three upper panels, (a), (b), and (c) show the ratio of vn of particles to antiparticles for Λ, Ξ, and Ω, respectively, in 10–40 % centrality. The lower panels show the difference between vn of particles to antiparticles. The vertical lines represent the statistical error bars and the shaded bands represent the systematic uncertainties. Data points for v3 are shifted by 0.15 GeV/c towards the left for better visibility. For the Ω, data points for v3 were not shown due to fewer statistics.

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  • Figure 10
    Figure 10

    The difference of vn of particles and antiparticles is plotted as a function of mass. The result is compared with 62.4 GeV. Uncertainties represent the sum of statistical and systematic in quadrature.

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  • Figure 11
    Figure 11

    v3/v23/2 is plotted as a function of pT for KS0, Λ, Ξ, Ω, ϕ, Λ¯, Ξ¯+, and Ω¯+ in 10–40 % central Au+Au collisions at sNN=54.4 GeV.

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  • Figure 12
    Figure 12

    (a) Shows the nq-scaled v2 as a function of nq-scaled transverse kinetic energy for KS0, ϕ, Λ, Ξ, and Ω in 10–40 % centrality class events. (b) Shows the same for KS0, ϕ, Λ¯, Ξ¯+, and Ω¯+. The red line shows the polynomial fit to the KS0 data points. (c) and (d) show the ratio of nq-scaled v2 of all the particles to the fit function.

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  • Figure 13
    Figure 13

    (a) Shows v3/nq3/2 as a function of nq-scaled transverse kinetic energy for KS0, ϕ, Λ, Ξ, and Ω in 10–40 % centrality class events. (b) Shows the same for KS0, ϕ, Λ¯, Ξ¯+, and Ω¯+. The red line shows the polynomial fit to the KS0 data points. (c) and (d) show the ratio of v3/nq3/2 of all the particles to the fit function.

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  • Figure 14
    Figure 14

    (a) Shows the ratio of v2 of ϕ to v2 of p¯ as a function of pT for 10–40 % and 40–80 % centralities at sNN=54.4 GeV. Data points for 10–40 % centrality are shifted by 0.05 GeV/c to the right for better visibility. (b) Shows the comparison of the ratio at sNN=54.4 GeV and 200 GeV in 0–80 % centrality. For 200 GeV [18], the measured ratio is v2(ϕ)/v2(p+p¯). The vertical lines represent the statistical error bars and the shaded bands represent the systematic uncertainties. Data points at 200 GeV are taken from Ref. [18].

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