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Figure 3b Fig. Group : Measurement of the angle between jet axes in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV PWG : PWG-JE (Jets) System: Pb-Pb Energy: 5.02 TeV
Figure 3a Fig. Group : Measurement of the angle between jet axes in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV PWG : PWG-JE (Jets) System: Pb-Pb Energy: 5.02 TeV
Figure 2b Fig. Group : Measurement of the angle between jet axes in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV PWG : PWG-JE (Jets) System: Pb-Pb Energy: 5.02 TeV
Figure 2a Fig. Group : Measurement of the angle between jet axes in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV PWG : PWG-JE (Jets) System: Pb-Pb Energy: 5.02 TeV
Figure 1 Fig. Group : Measurement of the angle between jet axes in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV PWG : PWG-JE (Jets) System: Pb-Pb Energy: 5.02 TeV
Figure 3 Fig. Group : Investigating charm quark energy loss in medium with the nuclear modification factor of D$^0$-tagged jets PWG : PWG-HF (Heavy Flavour) System: Pb-Pb Energy: 5.02 TeV
Figure 1 Fig. Group : Investigating charm quark energy loss in medium with the nuclear modification factor of D$^0$-tagged jets PWG : PWG-HF (Heavy Flavour) System: Pb-Pb Energy: 5.02 TeV
Figure 2 Fig. Group : Investigating charm quark energy loss in medium with the nuclear modification factor of D$^0$-tagged jets PWG : PWG-HF (Heavy Flavour) System: Pb-Pb Energy: 5.02 TeV
Figure 4b Fig. Group : Investigating charm quark energy loss in medium with the nuclear modification factor of D$^0$-tagged jets PWG : PWG-HF (Heavy Flavour) System: Pb-Pb Energy: 5.02 TeV
Figure 4a Fig. Group : Investigating charm quark energy loss in medium with the nuclear modification factor of D$^0$-tagged jets PWG : PWG-HF (Heavy Flavour) System: Pb-Pb Energy: 5.02 TeV
Figure A.1 Fig. Group : Observation of partonic flow in proton-proton and proton-nucleus collisions PWG : PWG-CF (Flow and Correlations) System: p-p, p-Pb Energy: 5.02 TeV, 13 TeV
Figure 4 Fig. Group : Observation of partonic flow in proton-proton and proton-nucleus collisions PWG : PWG-CF (Flow and Correlations) System: p-p, p-Pb Energy: 5.02 TeV, 13 TeV
Figure 3 Fig. Group : Observation of partonic flow in proton-proton and proton-nucleus collisions PWG : PWG-CF (Flow and Correlations) System: p-p, p-Pb Energy: 5.02 TeV, 13 TeV
Figure 2 Fig. Group : Observation of partonic flow in proton-proton and proton-nucleus collisions PWG : PWG-CF (Flow and Correlations) System: p-p, p-Pb Energy: 5.02 TeV, 13 TeV
Figure 1 Fig. Group : Observation of partonic flow in proton-proton and proton-nucleus collisions PWG : PWG-CF (Flow and Correlations) System: p-p, p-Pb Energy: 5.02 TeV, 13 TeV
Figure 5b Fig. Group : Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb--Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV PWG : PWG-HF (Heavy Flavour) System: Pb-Pb Energy: 5.02 TeV
Figure 1a Fig. Group : Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb--Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV PWG : PWG-HF (Heavy Flavour) System: Pb-Pb Energy: 5.02 TeV
Figure 1b Fig. Group : Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb--Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV PWG : PWG-HF (Heavy Flavour) System: Pb-Pb Energy: 5.02 TeV
Figure 2 Fig. Group : Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb--Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV PWG : PWG-HF (Heavy Flavour) System: Pb-Pb Energy: 5.02 TeV
Figure 3 Fig. Group : Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb--Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV PWG : PWG-HF (Heavy Flavour) System: Pb-Pb Energy: 5.02 TeV
Figure 4a Fig. Group : Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb--Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV PWG : PWG-HF (Heavy Flavour) System: Pb-Pb Energy: 5.02 TeV
Figure 4b Fig. Group : Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb--Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV PWG : PWG-HF (Heavy Flavour) System: Pb-Pb Energy: 5.02 TeV
Figure 5a Fig. Group : Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb--Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV PWG : PWG-HF (Heavy Flavour) System: Pb-Pb Energy: 5.02 TeV
Figure A.2 Fig. Group : Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb--Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV PWG : PWG-HF (Heavy Flavour) System: Pb-Pb Energy: 5.02 TeV
Figure 8b Fig. Group : Medium-induced modification of azimuthal correlations of electrons from heavy-flavor hadron decays with charged particles in Pb--Pb collisions at $\sqrt{s_{\rm{NN}} = 5.02}$ TeV PWG : PWG-HF (Heavy Flavour) System: Pb-Pb Energy: 5.02 TeV

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