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.
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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.
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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.
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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)
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.
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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
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.
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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.
PDF File
Previous Version
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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 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.
PDF File
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