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Figure 2a Fig. Group : Strangeness enhancement at its extremes: multiple (multi-)strange hadron production in pp collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 5.02 TeV
Figure 1 Fig. Group : Strangeness enhancement at its extremes: multiple (multi-)strange hadron production in pp collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 5.02 TeV
Figure 2b Fig. Group : Strangeness enhancement at its extremes: multiple (multi-)strange hadron production in pp collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 5.02 TeV
Figure 3 Fig. Group : Strangeness enhancement at its extremes: multiple (multi-)strange hadron production in pp collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 5.02 TeV
Figure 4 Fig. Group : Strangeness enhancement at its extremes: multiple (multi-)strange hadron production in pp collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 5.02 TeV
Figure 5a Fig. Group : Strangeness enhancement at its extremes: multiple (multi-)strange hadron production in pp collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 5.02 TeV
Figure 5b Fig. Group : Strangeness enhancement at its extremes: multiple (multi-)strange hadron production in pp collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 5.02 TeV
Figure 7 Fig. Group : Strangeness enhancement at its extremes: multiple (multi-)strange hadron production in pp collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 5.02 TeV
Figure 8 Fig. Group : Strangeness enhancement at its extremes: multiple (multi-)strange hadron production in pp collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 5.02 TeV
Figure 9 Fig. Group : Strangeness enhancement at its extremes: multiple (multi-)strange hadron production in pp collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 5.02 TeV
Figure 10 Fig. Group : Strangeness enhancement at its extremes: multiple (multi-)strange hadron production in pp collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 5.02 TeV
Figure 6 Fig. Group : Strangeness enhancement at its extremes: multiple (multi-)strange hadron production in pp collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 5.02 TeV
Figure 11 Fig. Group : Strangeness enhancement at its extremes: multiple (multi-)strange hadron production in pp collisions at $\mathbf{\sqrt{\textit{s}} = 5.02}$ TeV PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 5.02 TeV
Figure 10b Fig. Group : Multiplicity dependence of two-particle angular correlations of identified particles in pp collisions at $\mathbf{\sqrt{s} = 13}$ TeV PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 10a Fig. Group : Multiplicity dependence of two-particle angular correlations of identified particles in pp collisions at $\mathbf{\sqrt{s} = 13}$ TeV PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 10d Fig. Group : Multiplicity dependence of two-particle angular correlations of identified particles in pp collisions at $\mathbf{\sqrt{s} = 13}$ TeV PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 10c Fig. Group : Multiplicity dependence of two-particle angular correlations of identified particles in pp collisions at $\mathbf{\sqrt{s} = 13}$ TeV PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 3d Fig. Group : Multiplicity dependence of two-particle angular correlations of identified particles in pp collisions at $\mathbf{\sqrt{s} = 13}$ TeV PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 4c Fig. Group : Multiplicity dependence of two-particle angular correlations of identified particles in pp collisions at $\mathbf{\sqrt{s} = 13}$ TeV PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 4b Fig. Group : Multiplicity dependence of two-particle angular correlations of identified particles in pp collisions at $\mathbf{\sqrt{s} = 13}$ TeV PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 4a Fig. Group : Multiplicity dependence of two-particle angular correlations of identified particles in pp collisions at $\mathbf{\sqrt{s} = 13}$ TeV PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 3f Fig. Group : Multiplicity dependence of two-particle angular correlations of identified particles in pp collisions at $\mathbf{\sqrt{s} = 13}$ TeV PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 3b Fig. Group : Multiplicity dependence of two-particle angular correlations of identified particles in pp collisions at $\mathbf{\sqrt{s} = 13}$ TeV PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 3a Fig. Group : Multiplicity dependence of two-particle angular correlations of identified particles in pp collisions at $\mathbf{\sqrt{s} = 13}$ TeV PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 3e Fig. Group : Multiplicity dependence of two-particle angular correlations of identified particles in pp collisions at $\mathbf{\sqrt{s} = 13}$ TeV PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV

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