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  • Open Access

Production of π0 and η mesons in Cu+Au collisions at sNN=200GeV

C. Aidala et al. (PHENIX Collaboration)
Phys. Rev. C 98, 054903 – Published 19 November 2018

Abstract

Production of π0 and η mesons has been measured at midrapidity in Cu+Au collisions at sNN=200GeV. Measurements were performed in π0(η)γγ decay channel in the 1(2)20GeV/c transverse momentum range. A strong suppression is observed for π0 and η meson production at high transverse momentum in central Cu+Au collisions relative to the p+p results scaled by the number of nucleon-nucleon collisions. In central collisions the suppression is similar to Au+Au with comparable nuclear overlap. The η/π0 ratio measured as a function of transverse momentum is consistent with mT-scaling parametrization down to pT=2GeV/c, its asymptotic value is constant and consistent with Au+Au and p+p and does not show any significant dependence on collision centrality. Similar results were obtained in hadron-hadron, hadron-nucleus, and nucleus-nucleus collisions as well as in e+e collisions in a range of collision energies sNN=31800 GeV. This suggests that the quark-gluon-plasma medium produced in Cu+Cu collisions either does not affect the jet fragmentation into light mesons or it affects the π0 and η the same way.

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  • Received 4 June 2018

DOI:https://doi.org/10.1103/PhysRevC.98.054903

Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article's title, journal citation, and DOI. Funded by SCOAP3.

Published by the American Physical Society

Physics Subject Headings (PhySH)

Nuclear Physics

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Vol. 98, Iss. 5 — November 2018

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Images

  • Figure 1
    Figure 1

    Drawing showing Au+Au and Cu+Au collisions with comparable Npart. On panel (b) the overlap area is asymmetric, and part of the dilute surfaces of Au and Cu (corona) overlap.

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  • Figure 2
    Figure 2

    Example of an invariant mass plot (4.5<pT<5.0 GeV/c). (a) The foreground (photon pairs from the same event) is shown as points, the shaded area is the scaled mixed event background. Insert (b) shows the π0 peak area after mixed event subtraction; the Gaussian fit to the peak and the first-order polynomial fit to the residual background are also shown. Insert (c) shows the η peak area with the Gaussian fit and second-order polynomial for the residual background.

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  • Figure 3
    Figure 3

    Left: (a) π0 and (b) η invariant pT spectra measured in different centrality intervals of Cu+Au collisions at sNN=200GeV. The dashed curves are a fit with two Hagedorn-type functions with an asymptotic power-law (pTn) behavior. Right: ratios of (b)–(d) π0 and (f)–(h) η yields measured in PbSc or PbGl subsystem to the averaged ones. Error bars represent a quadratic sum of statistical and type-A systematic uncertainties. Error boxes in the right panel correspond to the quadratic sum of systematic uncertainties, which are uncorrelated between PbSc and PbGl.

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  • Figure 4
    Figure 4

    Ratios of η and π0 yields measured as a function of pT in different centrality intervals of Cu+Au collisions at sNN=200GeV. Dashed curve shows the mT scaling curve normalized to 0.5 at high momentum (see text). Error bars represent a quadratic sum of statistical and type-A systematic uncertainties for π0 and η yields. Error boxes represent a quadratic sum of type-B systematic uncertainties for π0 and η yields.

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  • Figure 5
    Figure 5

    RAB of π0 and η mesons measured as a function of pT in different centrality intervals of Cu+Au collisions at sNN=200GeV. Error bars represent a quadratic sum of statistical and type-A systematic uncertainties from Cu+Au and p+p measurements, respectively. Error boxes represent type-B systematic uncertainties from Cu+Au and p+p measurements. Solid and open boxes at unity represent type-C systematic uncertainties from Cu+Au (including uncertainties from the TAB values) and p+p, respectively. The reference p+p measurements are published in Ref. [12] for π0 and in Refs. [30, 38] for η (see details in the text).

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  • Figure 6
    Figure 6

    Comparison of π0RAB measured in Cu+Au, Au+Au and Cu+Cu collisions at sNN=200GeV and comparable Npart. Error bars represent a quadratic sum of statistical and type-A systematic uncertainties from Cu+Au and p+p measurements. Open boxes are type-B systematic uncertainties for Cu+Au and p+p collisions. The three boxes at unity are type-C systematic uncertainties from p+p and heavy-ion collisions. The boxes from left to right correspond to Cu+Au, Au+Au and Cu+Cu measurements, respectively.

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  • Figure 7
    Figure 7

    Comparison of integrated RAB for π0 measured as a function of Npart in Cu+Au and Au+Au collisions at sNN=200GeV. Uncertainties are the same as in the Fig. 6. The lower limit of integration is pT =5 GeV/c on (a), pT =10 GeV/c on (b).

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