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Figure 4 Fig. Group : First measurement of $Λ_\mathrm{c}^{+}$ production down to $p_\mathrm{T} = 0$ in pp and p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV PWG : PWG-HF (Heavy Flavour) System: p-p, p-Pb Energy: 5.02 TeV
Figure 1a Fig. Group : First measurement of $Λ_\mathrm{c}^{+}$ production down to $p_\mathrm{T} = 0$ in pp and p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV PWG : PWG-HF (Heavy Flavour) System: p-p, p-Pb Energy: 5.02 TeV
Figure 1b Fig. Group : First measurement of $Λ_\mathrm{c}^{+}$ production down to $p_\mathrm{T} = 0$ in pp and p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV PWG : PWG-HF (Heavy Flavour) System: p-p, p-Pb Energy: 5.02 TeV
Figure 2 Fig. Group : First measurement of $Λ_\mathrm{c}^{+}$ production down to $p_\mathrm{T} = 0$ in pp and p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV PWG : PWG-HF (Heavy Flavour) System: p-p, p-Pb Energy: 5.02 TeV
Figure 3 Fig. Group : First measurement of $Λ_\mathrm{c}^{+}$ production down to $p_\mathrm{T} = 0$ in pp and p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV PWG : PWG-HF (Heavy Flavour) System: p-p, p-Pb Energy: 5.02 TeV
Figure 5 Fig. Group : First measurement of $Λ_\mathrm{c}^{+}$ production down to $p_\mathrm{T} = 0$ in pp and p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV PWG : PWG-HF (Heavy Flavour) System: p-p, p-Pb Energy: 5.02 TeV
Figure 6a Fig. Group : First measurement of $Λ_\mathrm{c}^{+}$ production down to $p_\mathrm{T} = 0$ in pp and p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV PWG : PWG-HF (Heavy Flavour) System: p-p, p-Pb Energy: 5.02 TeV
Figure 6b Fig. Group : First measurement of $Λ_\mathrm{c}^{+}$ production down to $p_\mathrm{T} = 0$ in pp and p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV PWG : PWG-HF (Heavy Flavour) System: p-p, p-Pb Energy: 5.02 TeV
Figure 8 Fig. Group : Measurements of the groomed jet radius and momentum splitting fraction with the soft drop and dynamical grooming algorithms in pp collisions at $\sqrt{s}=5.02$ TeV PWG : PWG-JE (Jets) System: p-p Energy: 5.02 TeV
Figure 7 Fig. Group : Measurements of the groomed jet radius and momentum splitting fraction with the soft drop and dynamical grooming algorithms in pp collisions at $\sqrt{s}=5.02$ TeV PWG : PWG-JE (Jets) System: p-p Energy: 5.02 TeV
Figure 6 Fig. Group : Measurements of the groomed jet radius and momentum splitting fraction with the soft drop and dynamical grooming algorithms in pp collisions at $\sqrt{s}=5.02$ TeV PWG : PWG-JE (Jets) System: p-p Energy: 5.02 TeV
Figure 5 Fig. Group : Measurements of the groomed jet radius and momentum splitting fraction with the soft drop and dynamical grooming algorithms in pp collisions at $\sqrt{s}=5.02$ TeV PWG : PWG-JE (Jets) System: p-p Energy: 5.02 TeV
Figure 4 Fig. Group : Measurements of the groomed jet radius and momentum splitting fraction with the soft drop and dynamical grooming algorithms in pp collisions at $\sqrt{s}=5.02$ TeV PWG : PWG-JE (Jets) System: p-p Energy: 5.02 TeV
Figure 3 Fig. Group : Measurements of the groomed jet radius and momentum splitting fraction with the soft drop and dynamical grooming algorithms in pp collisions at $\sqrt{s}=5.02$ TeV PWG : PWG-JE (Jets) System: p-p Energy: 5.02 TeV
Figure 2 Fig. Group : Measurements of the groomed jet radius and momentum splitting fraction with the soft drop and dynamical grooming algorithms in pp collisions at $\sqrt{s}=5.02$ TeV PWG : PWG-JE (Jets) System: p-p Energy: 5.02 TeV
Figure 1 Fig. Group : Measurements of the groomed jet radius and momentum splitting fraction with the soft drop and dynamical grooming algorithms in pp collisions at $\sqrt{s}=5.02$ TeV PWG : PWG-JE (Jets) System: p-p Energy: 5.02 TeV
Figure 7 Fig. Group : Measurement of inclusive and leading subjet fragmentation in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV PWG : PWG-JE (Jets) System: p-p, Pb-Pb Energy: 5.02 TeV
Figure 1 Fig. Group : Measurement of inclusive and leading subjet fragmentation in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV PWG : PWG-JE (Jets) System: p-p, Pb-Pb Energy: 5.02 TeV
Figure 2 Fig. Group : Measurement of inclusive and leading subjet fragmentation in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV PWG : PWG-JE (Jets) System: p-p, Pb-Pb Energy: 5.02 TeV
Figure 3 Fig. Group : Measurement of inclusive and leading subjet fragmentation in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV PWG : PWG-JE (Jets) System: p-p, Pb-Pb Energy: 5.02 TeV
Figure 4a Fig. Group : Measurement of inclusive and leading subjet fragmentation in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV PWG : PWG-JE (Jets) System: p-p, Pb-Pb Energy: 5.02 TeV
Figure 6 Fig. Group : Measurement of inclusive and leading subjet fragmentation in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV PWG : PWG-JE (Jets) System: p-p, Pb-Pb Energy: 5.02 TeV
Figure 4b Fig. Group : Measurement of inclusive and leading subjet fragmentation in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV PWG : PWG-JE (Jets) System: p-p, Pb-Pb Energy: 5.02 TeV
Figure 5 Fig. Group : Measurement of inclusive and leading subjet fragmentation in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV PWG : PWG-JE (Jets) System: p-p, Pb-Pb Energy: 5.02 TeV
Figure 3 Fig. Group : Observation of flow angle and flow magnitude fluctuations in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV at the CERN Large Hadron Collider PWG : PWG-CF (Flow and Correlations) System: Pb-Pb Energy: 5.02 TeV

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