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Figure 4 Fig. Group : Measurement of $Ω^0_{\rm c}$ baryon production and branching-fraction ratio ${\rm BR(Ω^0_c \rightarrow Ω^- e^+ν_e)} / {\rm BR(Ω^0_c \rightarrow Ω^- π^+)}$ in pp collisions at $\sqrt{s}$ = 13 TeV PWG : PWG-HF (Heavy Flavour) System: p-p Energy: 13 TeV
Figure 3 Fig. Group : Measurement of $Ω^0_{\rm c}$ baryon production and branching-fraction ratio ${\rm BR(Ω^0_c \rightarrow Ω^- e^+ν_e)} / {\rm BR(Ω^0_c \rightarrow Ω^- π^+)}$ in pp collisions at $\sqrt{s}$ = 13 TeV PWG : PWG-HF (Heavy Flavour) System: p-p Energy: 13 TeV
Figure 2b Fig. Group : Measurement of $Ω^0_{\rm c}$ baryon production and branching-fraction ratio ${\rm BR(Ω^0_c \rightarrow Ω^- e^+ν_e)} / {\rm BR(Ω^0_c \rightarrow Ω^- π^+)}$ in pp collisions at $\sqrt{s}$ = 13 TeV PWG : PWG-HF (Heavy Flavour) System: p-p Energy: 13 TeV
Figure 2a Fig. Group : Measurement of $Ω^0_{\rm c}$ baryon production and branching-fraction ratio ${\rm BR(Ω^0_c \rightarrow Ω^- e^+ν_e)} / {\rm BR(Ω^0_c \rightarrow Ω^- π^+)}$ in pp collisions at $\sqrt{s}$ = 13 TeV PWG : PWG-HF (Heavy Flavour) System: p-p Energy: 13 TeV
Figure 1b Fig. Group : Measurement of $Ω^0_{\rm c}$ baryon production and branching-fraction ratio ${\rm BR(Ω^0_c \rightarrow Ω^- e^+ν_e)} / {\rm BR(Ω^0_c \rightarrow Ω^- π^+)}$ in pp collisions at $\sqrt{s}$ = 13 TeV PWG : PWG-HF (Heavy Flavour) System: p-p Energy: 13 TeV
Figure 1a Fig. Group : Measurement of $Ω^0_{\rm c}$ baryon production and branching-fraction ratio ${\rm BR(Ω^0_c \rightarrow Ω^- e^+ν_e)} / {\rm BR(Ω^0_c \rightarrow Ω^- π^+)}$ in pp collisions at $\sqrt{s}$ = 13 TeV PWG : PWG-HF (Heavy Flavour) System: p-p Energy: 13 TeV
Figure 3b Fig. Group : ALICE luminosity determination for Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV PWG : PWG-MM (Monte Carlo generators and Minimum Bias) System: Pb-Pb Energy: 5.02 TeV
Figure 1a Fig. Group : ALICE luminosity determination for Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV PWG : PWG-MM (Monte Carlo generators and Minimum Bias) System: Pb-Pb Energy: 5.02 TeV
Figure 1b Fig. Group : ALICE luminosity determination for Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV PWG : PWG-MM (Monte Carlo generators and Minimum Bias) System: Pb-Pb Energy: 5.02 TeV
Figure 2a Fig. Group : ALICE luminosity determination for Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV PWG : PWG-MM (Monte Carlo generators and Minimum Bias) System: Pb-Pb Energy: 5.02 TeV
Figure 2b Fig. Group : ALICE luminosity determination for Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV PWG : PWG-MM (Monte Carlo generators and Minimum Bias) System: Pb-Pb Energy: 5.02 TeV
Figure 2c Fig. Group : ALICE luminosity determination for Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV PWG : PWG-MM (Monte Carlo generators and Minimum Bias) System: Pb-Pb Energy: 5.02 TeV
Figure 2d Fig. Group : ALICE luminosity determination for Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV PWG : PWG-MM (Monte Carlo generators and Minimum Bias) System: Pb-Pb Energy: 5.02 TeV
Figure 3a Fig. Group : ALICE luminosity determination for Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV PWG : PWG-MM (Monte Carlo generators and Minimum Bias) System: Pb-Pb Energy: 5.02 TeV
Figure 4a Fig. Group : ALICE luminosity determination for Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV PWG : PWG-MM (Monte Carlo generators and Minimum Bias) System: Pb-Pb Energy: 5.02 TeV
Figure 6b Fig. Group : ALICE luminosity determination for Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV PWG : PWG-MM (Monte Carlo generators and Minimum Bias) System: Pb-Pb Energy: 5.02 TeV
Figure 6a Fig. Group : ALICE luminosity determination for Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV PWG : PWG-MM (Monte Carlo generators and Minimum Bias) System: Pb-Pb Energy: 5.02 TeV
Figure 5 Fig. Group : ALICE luminosity determination for Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV PWG : PWG-MM (Monte Carlo generators and Minimum Bias) System: Pb-Pb Energy: 5.02 TeV
Figure 4c Fig. Group : ALICE luminosity determination for Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV PWG : PWG-MM (Monte Carlo generators and Minimum Bias) System: Pb-Pb Energy: 5.02 TeV
Figure 4b Fig. Group : ALICE luminosity determination for Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV PWG : PWG-MM (Monte Carlo generators and Minimum Bias) System: Pb-Pb Energy: 5.02 TeV
Figure 4d Fig. Group : ALICE luminosity determination for Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV PWG : PWG-MM (Monte Carlo generators and Minimum Bias) System: Pb-Pb Energy: 5.02 TeV
Figure 1a Fig. Group : Measurement of the fraction of jet longitudinal momentum carried by $Λ_{\rm c}^+$ baryons in pp collisions PWG : PWG-HF (Heavy Flavour) System: p-p Energy: 13 TeV
Figure 1b Fig. Group : Measurement of the fraction of jet longitudinal momentum carried by $Λ_{\rm c}^+$ baryons in pp collisions PWG : PWG-HF (Heavy Flavour) System: p-p Energy: 13 TeV
Figure 4 Fig. Group : Pseudorapidity dependence of anisotropic flow and its decorrelations using long-range multiparticle correlations in Pb-Pb and Xe-Xe collisions PWG : PWG-CF (Flow and Correlations) System: Pb-Pb , System: Xe-Xe Energy: 5.02 TeV , Energy: 5.44 TeV
Figure 2 Fig. Group : Pseudorapidity dependence of anisotropic flow and its decorrelations using long-range multiparticle correlations in Pb-Pb and Xe-Xe collisions PWG : PWG-CF (Flow and Correlations) System: Pb-Pb , System: Xe-Xe Energy: 5.02 TeV , Energy: 5.44 TeV

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