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Direct photon production in d+Au collisions at sNN=200 GeV

A. Adare et al. (PHENIX Collaboration)
Phys. Rev. C 87, 054907 – Published 17 May 2013

Abstract

Direct photons have been measured in sNN=200 GeV d+Au collisions at midrapidity. A wide pT range is covered by measurements of nearly real virtual photons (1<pT<6 GeV/c) and real photons (5<pT<16 GeV/c). The invariant yield of the direct photons in d+Au collisions over the scaled p+p cross section is consistent with unity. Theoretical calculations assuming standard cold-nuclear-matter effects describe the data well for the entire pT range. This indicates that the large enhancement of direct photons observed in Au+Au collisions for 1.0<pT<2.5 GeV/c is attributable to a source other than the initial-state nuclear effects.

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  • Received 6 August 2012

DOI:https://doi.org/10.1103/PhysRevC.87.054907

©2013 American Physical Society

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Vol. 87, Iss. 5 — May 2013

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Images

  • Figure 1
    Figure 1

    The direct-photon fractions from the virtual-photon analysis as a function of pT in (a) p+p, (b) d+Au, and (c) Au+Au (MB) [4] collisions. The statistical and systematic uncertainties are shown by the bars and bands, respectively. The curves show expectations from a NLO pQCD calculation [18, 19] with different cutoff mass scales: (solid line) μ=0.5pT, (dashed line) μ=1.0pT, and (dash-dotted line) μ=2.0pT.

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  • Figure 2
    Figure 2

    (a) The invariant cross sections of the direct photon in p+p [6, 7] and d+Au collisions. The p+p fit result with the empirical parameterization described in the text is shown, as well as NLO pQCD calculations, and the scaled p+p fit is compared with the d+Au data. The solid and open symbols show the results from the virtual photon and π0-tagging methods, respectively. The asterisk symbols show the result from the statistical subtraction method for d+Au data, overlapping with the virtual photon result in 3<pT<5 GeV/c. The bars and bands represent the point-to-point and pT-correlated uncertainties, respectively. (b) The p+p data over the fit. The uncertainties of the fit owing to both point-to-point and pT-correlated uncertainties of the data are summed quadratically, and the sum is shown as dotted lines. The NLO pQCD calculations divided by the fit are also shown.

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  • Figure 3
    Figure 3

    Nuclear modification factor for d+Au, RdA, as a function of pT. The solid and open symbols show the results from the virtual- and real-photon measurements, respectively. The bars and bands represent the point-to-point and pT-correlated uncertainties, respectively. The box on the right shows the uncertainty of TdA for d+Au. The curves indicate the theoretical calculations [26] with different combinations of the CNM effects such as the Cronin enhancement, isospin effect, nuclear shadowing, and initial-state energy loss.

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  • Figure 4
    Figure 4

    Nuclear modification factors for Au+Au (MB) and d+Au as a function of pT. The triangle symbols show results from the (solid) virtual [4] and (open) real photon [8] measurements, respectively. The bars, bands, and boxes represent the same uncertainties as in Fig. 3. The + symbols for RdA for pT<5 GeV/c illustrates the difference in magnitude for RAA between Au+Au and d+Au collisions. The curves indicate the theoretical calculations [26, 28] for Au+Au MB considering only the standard CNM effects.

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