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Comparison of the second-order azimuthal harmonic v2 obtained from the template fitting procedure in the 13 TeV pp, 5.02 TeV pp, 5.02 TeV p+Pb and 8.16 TeV p+Pb data, as a function of Nchrec. The results are for 0.5 < pTa,b < 5 GeV. The error bars and shaded bands indicate statistical and systematic uncertainties, respectively.
png 102kB, pdf 16kB
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Comparison of the second-order azimuthal harmonic v2 obtained from the template fitting procedure in the 13 TeV pp, 5.02 TeV pp and 5.02 TeV p+Pb, as a function of Nchrec. The results are for 0.5 < pTa,b < 5 GeV. The error bars and shaded bands indicate statistical and systematic uncertainties, respectively.
png 82kB, pdf 16kB
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Compilation of results for the nuclear modification factor RAA vs. number of participating nucleons Npart in different channels from the Run 2 Pb+Pb and pp data. Results are shown for Z bosons (black squares), anti-kt R=0.4 jets (red circles), intermediate-pT charged hadrons (cyan triangles) and prompt J/ψ's (magenta inverted triangles). The statistical uncertainties are shown as vertical bars and the total systematic uncertainties, including pp luminosity and TAA uncertainties, are shown as boxes.
png 77kB, pdf 15kB
This and previous plot versions
Compilation of results for the nuclear modification factor RAA vs. number of participating nucleons Npart in different channels from the Run 2 Pb+Pb and pp data. Results are shown for Z bosons (black squares), anti-kt R=0.4 jets (red circles) and high-pT charged hadrons (blue crosses). Statistical uncertainties are shown as vertical bars and total systematic uncertainties, including pp luminosity and TAA uncertainties, are shown as boxes. The Z and jet data are identical to those in Fig. 1.
png 41kB, pdf 15kB
This and previous plot versions
Compilation of results for the nuclear modification factor RAA vs. number of participating nucleons Npart in different channels from the Run 2 Pb+Pb and pp data. Results are shown for anti-kt R=0.4 jets (red circles) and for high-pT (blue crosses), intermediate-pT (cyan triangles) and low-pT (green diamonds) charged hadrons. Statistical uncertainties are shown as vertical bars and total systematic uncertainties, including pp luminosity and TAA uncertainties, are shown as boxes. The jet, intermediate-pT and high-pT hadron data are identical to those in Figs. 1 and 2.
png 75kB, pdf 15kB
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Compilation of results for the nuclear modification factor RAA vs. pT or mZ in different channels from the Run 2 Pb+Pb and pp data. Results are shown for Z bosons (black squares, plotted at the Z boson mass), anti-kt R=0.4 jets (red circles), intermediate-pT charged hadrons (blue diamonds) and prompt J/ψ's (green crosses). The statistical uncertainties are shown as vertical bars and the total systematic uncertainties, including pp luminosity and TAA uncertainties, are shown as boxes.
png 88kB, pdf 17kB
This and previous plot versions
Compilation of results for the nuclear modification factor RAA vs. pT or mZ in different channels from the Run 2 Pb+Pb and pp data. Results are shown for Z bosons (black squares, plotted at the Z boson mass), anti-kt R=0.4 jets (red circles), intermediate-pT charged hadrons (blue diamonds) and non-prompt J/ψ's (magenta crosses). The statistical uncertainties are shown as vertical bars and the total systematic uncertainties, including pp luminosity and TAA uncertainties, are shown as boxes. The Z, jet and hadron data are identical to those in Fig. 4.
png 88kB, pdf 17kB
This and previous plot versions
ATLAS Collaboration, 2019