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Title
ID number ALI-PUB-XXX
Figure Caption
Journal reference
Scope: PWG
- Any -
PWG-CF (Flow and Correlations)
PWG-DQ (Dileptons and Quarkonia)
PWG-EM (Electromagnetic probes)
PWG-HF (Heavy Flavour)
PWG-JE (Jets)
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General
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PWG1
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none
Energy
cosmic rays
900 GeV
2.36 TeV
2.76 TeV
5.02 TeV
5.36 TeV
5.44 TeV
5.5 TeV
7 TeV
8 TeV
8.8 TeV
9.61 TeV
13 TeV
13.6 TeV
14 TeV
none
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Figure
Figure 6b
Fig. Group :
Closing in on critical net-baryon fluctuations at LHC energies: cumulants up to third order in Pb$-$Pb collisions
PWG :
PWG-CF (Flow and Correlations)
System:
Pb-Pb
Energy:
2.76 TeV, 5.02 TeV
Figure 6a
Fig. Group :
Closing in on critical net-baryon fluctuations at LHC energies: cumulants up to third order in Pb$-$Pb collisions
PWG :
PWG-CF (Flow and Correlations)
System:
Pb-Pb
Energy:
2.76 TeV, 5.02 TeV
Figure 5b
Fig. Group :
Closing in on critical net-baryon fluctuations at LHC energies: cumulants up to third order in Pb$-$Pb collisions
PWG :
PWG-CF (Flow and Correlations)
System:
Pb-Pb
Energy:
2.76 TeV, 5.02 TeV
Figure 5a
Fig. Group :
Closing in on critical net-baryon fluctuations at LHC energies: cumulants up to third order in Pb$-$Pb collisions
PWG :
PWG-CF (Flow and Correlations)
System:
Pb-Pb
Energy:
2.76 TeV, 5.02 TeV
Figure 4b
Fig. Group :
Closing in on critical net-baryon fluctuations at LHC energies: cumulants up to third order in Pb$-$Pb collisions
PWG :
PWG-CF (Flow and Correlations)
System:
Pb-Pb
Energy:
2.76 TeV, 5.02 TeV
Figure 4a
Fig. Group :
Closing in on critical net-baryon fluctuations at LHC energies: cumulants up to third order in Pb$-$Pb collisions
PWG :
PWG-CF (Flow and Correlations)
System:
Pb-Pb
Energy:
2.76 TeV, 5.02 TeV
Figure 3b
Fig. Group :
Closing in on critical net-baryon fluctuations at LHC energies: cumulants up to third order in Pb$-$Pb collisions
PWG :
PWG-CF (Flow and Correlations)
System:
Pb-Pb
Energy:
2.76 TeV, 5.02 TeV
Figure 3a
Fig. Group :
Closing in on critical net-baryon fluctuations at LHC energies: cumulants up to third order in Pb$-$Pb collisions
PWG :
PWG-CF (Flow and Correlations)
System:
Pb-Pb
Energy:
2.76 TeV, 5.02 TeV
Figure 2b
Fig. Group :
Closing in on critical net-baryon fluctuations at LHC energies: cumulants up to third order in Pb$-$Pb collisions
PWG :
PWG-CF (Flow and Correlations)
System:
Pb-Pb
Energy:
2.76 TeV, 5.02 TeV
Figure 2a
Fig. Group :
Closing in on critical net-baryon fluctuations at LHC energies: cumulants up to third order in Pb$-$Pb collisions
PWG :
PWG-CF (Flow and Correlations)
System:
Pb-Pb
Energy:
2.76 TeV, 5.02 TeV
Figure 1b
Fig. Group :
Closing in on critical net-baryon fluctuations at LHC energies: cumulants up to third order in Pb$-$Pb collisions
PWG :
PWG-CF (Flow and Correlations)
System:
Pb-Pb
Energy:
2.76 TeV, 5.02 TeV
Figure 1a
Fig. Group :
Closing in on critical net-baryon fluctuations at LHC energies: cumulants up to third order in Pb$-$Pb collisions
PWG :
PWG-CF (Flow and Correlations)
System:
Pb-Pb
Energy:
2.76 TeV, 5.02 TeV
Figure 6
Fig. Group :
Measurement of the non-prompt D-meson fraction as a function of multiplicity in proton$-$proton collisions at $\sqrt{s} = 13$ TeV
PWG :
PWG-HF (Heavy Flavour)
System:
p-p
Energy:
13 TeV
Figure 1a
Fig. Group :
Measurement of the non-prompt D-meson fraction as a function of multiplicity in proton$-$proton collisions at $\sqrt{s} = 13$ TeV
PWG :
PWG-HF (Heavy Flavour)
System:
p-p
Energy:
13 TeV
Figure 1b
Fig. Group :
Measurement of the non-prompt D-meson fraction as a function of multiplicity in proton$-$proton collisions at $\sqrt{s} = 13$ TeV
PWG :
PWG-HF (Heavy Flavour)
System:
p-p
Energy:
13 TeV
Figure 2a
Fig. Group :
Measurement of the non-prompt D-meson fraction as a function of multiplicity in proton$-$proton collisions at $\sqrt{s} = 13$ TeV
PWG :
PWG-HF (Heavy Flavour)
System:
p-p
Energy:
13 TeV
Figure 2b
Fig. Group :
Measurement of the non-prompt D-meson fraction as a function of multiplicity in proton$-$proton collisions at $\sqrt{s} = 13$ TeV
PWG :
PWG-HF (Heavy Flavour)
System:
p-p
Energy:
13 TeV
Figure 3a
Fig. Group :
Measurement of the non-prompt D-meson fraction as a function of multiplicity in proton$-$proton collisions at $\sqrt{s} = 13$ TeV
PWG :
PWG-HF (Heavy Flavour)
System:
p-p
Energy:
13 TeV
Figure 3b
Fig. Group :
Measurement of the non-prompt D-meson fraction as a function of multiplicity in proton$-$proton collisions at $\sqrt{s} = 13$ TeV
PWG :
PWG-HF (Heavy Flavour)
System:
p-p
Energy:
13 TeV
Figure 3d
Fig. Group :
Measurement of the non-prompt D-meson fraction as a function of multiplicity in proton$-$proton collisions at $\sqrt{s} = 13$ TeV
PWG :
PWG-HF (Heavy Flavour)
System:
p-p
Energy:
13 TeV
Figure 8
Fig. Group :
Measurement of the non-prompt D-meson fraction as a function of multiplicity in proton$-$proton collisions at $\sqrt{s} = 13$ TeV
PWG :
PWG-HF (Heavy Flavour)
System:
p-p
Energy:
13 TeV
Figure 7
Fig. Group :
Measurement of the non-prompt D-meson fraction as a function of multiplicity in proton$-$proton collisions at $\sqrt{s} = 13$ TeV
PWG :
PWG-HF (Heavy Flavour)
System:
p-p
Energy:
13 TeV
Figure 3c
Fig. Group :
Measurement of the non-prompt D-meson fraction as a function of multiplicity in proton$-$proton collisions at $\sqrt{s} = 13$ TeV
PWG :
PWG-HF (Heavy Flavour)
System:
p-p
Energy:
13 TeV
Figure 4
Fig. Group :
Measurement of the non-prompt D-meson fraction as a function of multiplicity in proton$-$proton collisions at $\sqrt{s} = 13$ TeV
PWG :
PWG-HF (Heavy Flavour)
System:
p-p
Energy:
13 TeV
Figure 5
Fig. Group :
Measurement of the non-prompt D-meson fraction as a function of multiplicity in proton$-$proton collisions at $\sqrt{s} = 13$ TeV
PWG :
PWG-HF (Heavy Flavour)
System:
p-p
Energy:
13 TeV
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