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Figure 6b Fig. Group : Studying charm hadronisation into baryons with azimuthal correlations of $Λ_{\rm c}^{+}$ with charged particles in pp collisions at $\mathbf{\sqrt{\it s} = 13}$ TeV PWG : PWG-HF (Heavy Flavour) System: p-p Energy: 13 TeV
Figure 6a Fig. Group : Studying charm hadronisation into baryons with azimuthal correlations of $Λ_{\rm c}^{+}$ with charged particles in pp collisions at $\mathbf{\sqrt{\it s} = 13}$ TeV PWG : PWG-HF (Heavy Flavour) System: p-p Energy: 13 TeV
Figure 5 Fig. Group : Studying charm hadronisation into baryons with azimuthal correlations of $Λ_{\rm c}^{+}$ with charged particles in pp collisions at $\mathbf{\sqrt{\it s} = 13}$ TeV PWG : PWG-HF (Heavy Flavour) System: p-p Energy: 13 TeV
Figure 4 Fig. Group : Studying charm hadronisation into baryons with azimuthal correlations of $Λ_{\rm c}^{+}$ with charged particles in pp collisions at $\mathbf{\sqrt{\it s} = 13}$ TeV PWG : PWG-HF (Heavy Flavour) System: p-p Energy: 13 TeV
Figure 3 Fig. Group : Studying charm hadronisation into baryons with azimuthal correlations of $Λ_{\rm c}^{+}$ with charged particles in pp collisions at $\mathbf{\sqrt{\it s} = 13}$ TeV PWG : PWG-HF (Heavy Flavour) System: p-p Energy: 13 TeV
Figure 2 Fig. Group : Studying charm hadronisation into baryons with azimuthal correlations of $Λ_{\rm c}^{+}$ with charged particles in pp collisions at $\mathbf{\sqrt{\it s} = 13}$ TeV PWG : PWG-HF (Heavy Flavour) System: p-p Energy: 13 TeV
Figure 1 Fig. Group : Studying charm hadronisation into baryons with azimuthal correlations of $Λ_{\rm c}^{+}$ with charged particles in pp collisions at $\mathbf{\sqrt{\it s} = 13}$ TeV PWG : PWG-HF (Heavy Flavour) System: p-p Energy: 13 TeV
Figure A.1 Fig. Group : Search for quasi-particle scattering in the quark-gluon plasma with jet splittings in pp and Pb$-$Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.02}$ TeV PWG : PWG-JE (Jets) System: p-p, Pb-Pb Energy: 5.02 TeV
Figure 3 Fig. Group : Search for quasi-particle scattering in the quark-gluon plasma with jet splittings in pp and Pb$-$Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.02}$ TeV PWG : PWG-JE (Jets) System: p-p, Pb-Pb Energy: 5.02 TeV
Figure 2 Fig. Group : Search for quasi-particle scattering in the quark-gluon plasma with jet splittings in pp and Pb$-$Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.02}$ TeV PWG : PWG-JE (Jets) System: p-p, Pb-Pb Energy: 5.02 TeV
Figure 1 Fig. Group : Search for quasi-particle scattering in the quark-gluon plasma with jet splittings in pp and Pb$-$Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.02}$ TeV PWG : PWG-JE (Jets) System: p-p, Pb-Pb Energy: 5.02 TeV
Figure 5 Fig. Group : Multiplicity dependence of K$^(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV PWG :* PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 4 Fig. Group : Multiplicity dependence of K$^(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV PWG :* PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 3 Fig. Group : Multiplicity dependence of K$^(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV PWG :* PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 2 Fig. Group : Multiplicity dependence of K$^(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV PWG :* PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 1 Fig. Group : Multiplicity dependence of K$^(892)^{\pm}$ production in pp collisions at $\sqrt{s}$ = 13 TeV PWG :* PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 1b Fig. Group : Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 1a Fig. Group : Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 2 Fig. Group : Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 3a Fig. Group : Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 3b Fig. Group : Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 4 Fig. Group : Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 6a Fig. Group : Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 7b Fig. Group : Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 5 Fig. Group : Multiplicity dependence of f$_0$(980) production in pp collisions at $\sqrt{s} = 13$ TeV PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV

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