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Figure 12a Fig. Group : Femtoscopic correlations of identical charged pions and kaons in pp collisions at $\sqrt{s}=13$ TeV with event-shape selection PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 12b Fig. Group : Femtoscopic correlations of identical charged pions and kaons in pp collisions at $\sqrt{s}=13$ TeV with event-shape selection PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 8a Fig. Group : Femtoscopic correlations of identical charged pions and kaons in pp collisions at $\sqrt{s}=13$ TeV with event-shape selection PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 19 Fig. Group : Light-flavor particle production in high-multiplicity pp collisions at $\mathbf{\sqrt{\textit{s}} = 13}$ TeV as a function of transverse spherocity PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 18d Fig. Group : Light-flavor particle production in high-multiplicity pp collisions at $\mathbf{\sqrt{\textit{s}} = 13}$ TeV as a function of transverse spherocity PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 18c Fig. Group : Light-flavor particle production in high-multiplicity pp collisions at $\mathbf{\sqrt{\textit{s}} = 13}$ TeV as a function of transverse spherocity PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 18b Fig. Group : Light-flavor particle production in high-multiplicity pp collisions at $\mathbf{\sqrt{\textit{s}} = 13}$ TeV as a function of transverse spherocity PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 18a Fig. Group : Light-flavor particle production in high-multiplicity pp collisions at $\mathbf{\sqrt{\textit{s}} = 13}$ TeV as a function of transverse spherocity PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 14 Fig. Group : Light-flavor particle production in high-multiplicity pp collisions at $\mathbf{\sqrt{\textit{s}} = 13}$ TeV as a function of transverse spherocity PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 8a Fig. Group : Light-flavor particle production in high-multiplicity pp collisions at $\mathbf{\sqrt{\textit{s}} = 13}$ TeV as a function of transverse spherocity PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 8b Fig. Group : Light-flavor particle production in high-multiplicity pp collisions at $\mathbf{\sqrt{\textit{s}} = 13}$ TeV as a function of transverse spherocity PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 9a Fig. Group : Light-flavor particle production in high-multiplicity pp collisions at $\mathbf{\sqrt{\textit{s}} = 13}$ TeV as a function of transverse spherocity PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 9b Fig. Group : Light-flavor particle production in high-multiplicity pp collisions at $\mathbf{\sqrt{\textit{s}} = 13}$ TeV as a function of transverse spherocity PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 10a Fig. Group : Light-flavor particle production in high-multiplicity pp collisions at $\mathbf{\sqrt{\textit{s}} = 13}$ TeV as a function of transverse spherocity PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 10b Fig. Group : Light-flavor particle production in high-multiplicity pp collisions at $\mathbf{\sqrt{\textit{s}} = 13}$ TeV as a function of transverse spherocity PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 11 Fig. Group : Light-flavor particle production in high-multiplicity pp collisions at $\mathbf{\sqrt{\textit{s}} = 13}$ TeV as a function of transverse spherocity PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 12a Fig. Group : Light-flavor particle production in high-multiplicity pp collisions at $\mathbf{\sqrt{\textit{s}} = 13}$ TeV as a function of transverse spherocity PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 13 Fig. Group : Light-flavor particle production in high-multiplicity pp collisions at $\mathbf{\sqrt{\textit{s}} = 13}$ TeV as a function of transverse spherocity PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 12b Fig. Group : Light-flavor particle production in high-multiplicity pp collisions at $\mathbf{\sqrt{\textit{s}} = 13}$ TeV as a function of transverse spherocity PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 17b Fig. Group : Light-flavor particle production in high-multiplicity pp collisions at $\mathbf{\sqrt{\textit{s}} = 13}$ TeV as a function of transverse spherocity PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 17a Fig. Group : Light-flavor particle production in high-multiplicity pp collisions at $\mathbf{\sqrt{\textit{s}} = 13}$ TeV as a function of transverse spherocity PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 16a Fig. Group : Light-flavor particle production in high-multiplicity pp collisions at $\mathbf{\sqrt{\textit{s}} = 13}$ TeV as a function of transverse spherocity PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 16b Fig. Group : Light-flavor particle production in high-multiplicity pp collisions at $\mathbf{\sqrt{\textit{s}} = 13}$ TeV as a function of transverse spherocity PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 15 Fig. Group : Light-flavor particle production in high-multiplicity pp collisions at $\mathbf{\sqrt{\textit{s}} = 13}$ TeV as a function of transverse spherocity PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 2 Fig. Group : Light-flavor particle production in high-multiplicity pp collisions at $\mathbf{\sqrt{\textit{s}} = 13}$ TeV as a function of transverse spherocity PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV

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