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Figure 2 Fig. Group : Accessing the deuteron source with pion-deuteron femtoscopy in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV PWG : PWG-CF (Flow and Correlations) System: Pb-Pb Energy: 5.02 TeV
Figure 1 Fig. Group : Accessing the deuteron source with pion-deuteron femtoscopy in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV PWG : PWG-CF (Flow and Correlations) System: Pb-Pb Energy: 5.02 TeV
Figure 3b Fig. Group : First observation of ultra-long-range azimuthal correlations in low multiplicity pp and p-Pb collisions at the LHC PWG : PWG-CF (Flow and Correlations) System: p-p, p-Pb Energy: 5.02 TeV, 13 TeV
Figure 3a Fig. Group : First observation of ultra-long-range azimuthal correlations in low multiplicity pp and p-Pb collisions at the LHC PWG : PWG-CF (Flow and Correlations) System: p-p, p-Pb Energy: 5.02 TeV, 13 TeV
Figure 2 Fig. Group : First observation of ultra-long-range azimuthal correlations in low multiplicity pp and p-Pb collisions at the LHC PWG : PWG-CF (Flow and Correlations) System: p-p, p-Pb Energy: 5.02 TeV, 13 TeV
Figure 1 Fig. Group : First observation of ultra-long-range azimuthal correlations in low multiplicity pp and p-Pb collisions at the LHC PWG : PWG-CF (Flow and Correlations) System: p-p, p-Pb Energy: 5.02 TeV, 13 TeV
Figure A.1 Fig. Group : Revealing the microscopic mechanism of deuteron formation at the LHC PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 2b Fig. Group : Revealing the microscopic mechanism of deuteron formation at the LHC PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 2a Fig. Group : Revealing the microscopic mechanism of deuteron formation at the LHC PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 1 Fig. Group : Revealing the microscopic mechanism of deuteron formation at the LHC PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 5 Fig. Group : Centrality dependence of charged-particle pseudorapidity density at midrapidity in Pb-Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.36}$ TeV PWG : PWG-LF (Light Flavour Spectra) System: Pb-Pb Energy: 5.36 TeV
Figure 4 Fig. Group : Centrality dependence of charged-particle pseudorapidity density at midrapidity in Pb-Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.36}$ TeV PWG : PWG-LF (Light Flavour Spectra) System: Pb-Pb Energy: 5.36 TeV
Figure 3 Fig. Group : Centrality dependence of charged-particle pseudorapidity density at midrapidity in Pb-Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.36}$ TeV PWG : PWG-LF (Light Flavour Spectra) System: Pb-Pb Energy: 5.36 TeV
Figure 2 Fig. Group : Centrality dependence of charged-particle pseudorapidity density at midrapidity in Pb-Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.36}$ TeV PWG : PWG-LF (Light Flavour Spectra) System: Pb-Pb Energy: 5.36 TeV
Figure 1 Fig. Group : Centrality dependence of charged-particle pseudorapidity density at midrapidity in Pb-Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.36}$ TeV PWG : PWG-LF (Light Flavour Spectra) System: Pb-Pb Energy: 5.36 TeV
Figure 1a Fig. Group : D$^{0}$-meson-tagged jet axes difference in proton-proton collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV PWG : PWG-HF (Heavy Flavour) System: p-p Energy: 5.02 TeV
Figure 1b Fig. Group : D$^{0}$-meson-tagged jet axes difference in proton-proton collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV PWG : PWG-HF (Heavy Flavour) System: p-p Energy: 5.02 TeV
Figure 2a Fig. Group : D$^{0}$-meson-tagged jet axes difference in proton-proton collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV PWG : PWG-HF (Heavy Flavour) System: p-p Energy: 5.02 TeV
Figure 2b Fig. Group : D$^{0}$-meson-tagged jet axes difference in proton-proton collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV PWG : PWG-HF (Heavy Flavour) System: p-p Energy: 5.02 TeV
Figure 3 Fig. Group : D$^{0}$-meson-tagged jet axes difference in proton-proton collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV PWG : PWG-HF (Heavy Flavour) System: p-p Energy: 5.02 TeV
Figure 4 Fig. Group : D$^{0}$-meson-tagged jet axes difference in proton-proton collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV PWG : PWG-HF (Heavy Flavour) System: p-p Energy: 5.02 TeV
Figure 5 Fig. Group : D$^{0}$-meson-tagged jet axes difference in proton-proton collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV PWG : PWG-HF (Heavy Flavour) System: p-p Energy: 5.02 TeV
Figure 11 Fig. Group : D$^{0}$-meson-tagged jet axes difference in proton-proton collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV PWG : PWG-HF (Heavy Flavour) System: p-p Energy: 5.02 TeV
Figure 10 Fig. Group : D$^{0}$-meson-tagged jet axes difference in proton-proton collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV PWG : PWG-HF (Heavy Flavour) System: p-p Energy: 5.02 TeV
Figure 7 Fig. Group : D$^{0}$-meson-tagged jet axes difference in proton-proton collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV PWG : PWG-HF (Heavy Flavour) System: p-p Energy: 5.02 TeV

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