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Figure 4b Fig. Group : Towards the understanding of the genuine three-body interaction for p$-$p$-$p and p$-$p$-Λ$ PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 4a Fig. Group : Towards the understanding of the genuine three-body interaction for p$-$p$-$p and p$-$p$-Λ$ PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 3b Fig. Group : Towards the understanding of the genuine three-body interaction for p$-$p$-$p and p$-$p$-Λ$ PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 3a Fig. Group : Towards the understanding of the genuine three-body interaction for p$-$p$-$p and p$-$p$-Λ$ PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 2b Fig. Group : Towards the understanding of the genuine three-body interaction for p$-$p$-$p and p$-$p$-Λ$ PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 2a Fig. Group : Towards the understanding of the genuine three-body interaction for p$-$p$-$p and p$-$p$-Λ$ PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 1c Fig. Group : Towards the understanding of the genuine three-body interaction for p$-$p$-$p and p$-$p$-Λ$ PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 1b Fig. Group : Towards the understanding of the genuine three-body interaction for p$-$p$-$p and p$-$p$-Λ$ PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 1a Fig. Group : Towards the understanding of the genuine three-body interaction for p$-$p$-$p and p$-$p$-Λ$ PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 1 Fig. Group : Measurement of inclusive J/$ψ$ pair production cross section in pp collisions at $\sqrt{s} = 13$ TeV PWG : PWG-DQ (Dileptons and Quarkonia) System: p-p Energy: 13 TeV
Figure 6b Fig. Group : Measurement of $ψ$(2S) production as a function of charged-particle pseudorapidity density in pp collisions at $\sqrt{s}$ = 13 TeV and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV with ALICE at the LHC PWG : PWG-DQ (Dileptons and Quarkonia) System: p-p, p-Pb Energy: 8 TeV, 13 TeV
Figure 6a Fig. Group : Measurement of $ψ$(2S) production as a function of charged-particle pseudorapidity density in pp collisions at $\sqrt{s}$ = 13 TeV and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV with ALICE at the LHC PWG : PWG-DQ (Dileptons and Quarkonia) System: p-p, p-Pb Energy: 8 TeV, 13 TeV
Figure 5b Fig. Group : Measurement of $ψ$(2S) production as a function of charged-particle pseudorapidity density in pp collisions at $\sqrt{s}$ = 13 TeV and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV with ALICE at the LHC PWG : PWG-DQ (Dileptons and Quarkonia) System: p-p, p-Pb Energy: 8 TeV, 13 TeV
Figure 5a Fig. Group : Measurement of $ψ$(2S) production as a function of charged-particle pseudorapidity density in pp collisions at $\sqrt{s}$ = 13 TeV and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV with ALICE at the LHC PWG : PWG-DQ (Dileptons and Quarkonia) System: p-p, p-Pb Energy: 8 TeV, 13 TeV
Figure 4b Fig. Group : Measurement of $ψ$(2S) production as a function of charged-particle pseudorapidity density in pp collisions at $\sqrt{s}$ = 13 TeV and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV with ALICE at the LHC PWG : PWG-DQ (Dileptons and Quarkonia) System: p-p, p-Pb Energy: 8 TeV, 13 TeV
Figure 4a Fig. Group : Measurement of $ψ$(2S) production as a function of charged-particle pseudorapidity density in pp collisions at $\sqrt{s}$ = 13 TeV and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV with ALICE at the LHC PWG : PWG-DQ (Dileptons and Quarkonia) System: p-p, p-Pb Energy: 8 TeV, 13 TeV
Figure 3 Fig. Group : Measurement of $ψ$(2S) production as a function of charged-particle pseudorapidity density in pp collisions at $\sqrt{s}$ = 13 TeV and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV with ALICE at the LHC PWG : PWG-DQ (Dileptons and Quarkonia) System: p-p, p-Pb Energy: 8 TeV, 13 TeV
Figure 2 Fig. Group : Measurement of $ψ$(2S) production as a function of charged-particle pseudorapidity density in pp collisions at $\sqrt{s}$ = 13 TeV and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV with ALICE at the LHC PWG : PWG-DQ (Dileptons and Quarkonia) System: p-p, p-Pb Energy: 8 TeV, 13 TeV
Figure 1c Fig. Group : Measurement of $ψ$(2S) production as a function of charged-particle pseudorapidity density in pp collisions at $\sqrt{s}$ = 13 TeV and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV with ALICE at the LHC PWG : PWG-DQ (Dileptons and Quarkonia) System: p-p, p-Pb Energy: 8 TeV, 13 TeV
Figure 1b Fig. Group : Measurement of $ψ$(2S) production as a function of charged-particle pseudorapidity density in pp collisions at $\sqrt{s}$ = 13 TeV and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV with ALICE at the LHC PWG : PWG-DQ (Dileptons and Quarkonia) System: p-p, p-Pb Energy: 8 TeV, 13 TeV
Figure 1a Fig. Group : Measurement of $ψ$(2S) production as a function of charged-particle pseudorapidity density in pp collisions at $\sqrt{s}$ = 13 TeV and p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV with ALICE at the LHC PWG : PWG-DQ (Dileptons and Quarkonia) System: p-p, p-Pb Energy: 8 TeV, 13 TeV
Figure 2 Fig. Group : Measurement of beauty-strange meson production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV via non-prompt $\mathrm{D_s}^{+}$ mesons PWG : PWG-HF (Heavy Flavour) System: Pb-Pb Energy: 5.02 TeV
Figure 1 Fig. Group : Measurement of beauty-strange meson production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV via non-prompt $\mathrm{D_s}^{+}$ mesons PWG : PWG-HF (Heavy Flavour) System: Pb-Pb Energy: 5.02 TeV
Figure 3 Fig. Group : Measurement of beauty-strange meson production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV via non-prompt $\mathrm{D_s}^{+}$ mesons PWG : PWG-HF (Heavy Flavour) System: Pb-Pb Energy: 5.02 TeV
Figure 4 Fig. Group : Measurement of beauty-strange meson production in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV via non-prompt $\mathrm{D_s}^{+}$ mesons PWG : PWG-HF (Heavy Flavour) System: Pb-Pb Energy: 5.02 TeV

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