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Figure 6 Fig. Group : Measurement of isolated-prompt photon$-$hadron correlations in Pb$-$Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.02}$ TeV PWG : PWG-JE (Jets) System: Pb-Pb Energy: 5.02 TeV
Figure 7 Fig. Group : Measurement of isolated-prompt photon$-$hadron correlations in Pb$-$Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.02}$ TeV PWG : PWG-JE (Jets) System: Pb-Pb Energy: 5.02 TeV
Figure 5 Fig. Group : Measurement of isolated-prompt photon$-$hadron correlations in Pb$-$Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.02}$ TeV PWG : PWG-JE (Jets) System: Pb-Pb Energy: 5.02 TeV
Figure A.3 Fig. Group : $\mathbf{\textbf{K}^{0}_{\textbf{S}}}-\mathbf{\textbf{K}^{0}_{\textbf{S}}}$ femtoscopy in Pb$-$Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.02}$ TeV at the LHC PWG : PWG-CF (Flow and Correlations) System: Pb-Pb Energy: 5.02 TeV
Figure A.2 Fig. Group : $\mathbf{\textbf{K}^{0}_{\textbf{S}}}-\mathbf{\textbf{K}^{0}_{\textbf{S}}}$ femtoscopy in Pb$-$Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.02}$ TeV at the LHC PWG : PWG-CF (Flow and Correlations) System: Pb-Pb Energy: 5.02 TeV
Figure A.1 Fig. Group : $\mathbf{\textbf{K}^{0}_{\textbf{S}}}-\mathbf{\textbf{K}^{0}_{\textbf{S}}}$ femtoscopy in Pb$-$Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.02}$ TeV at the LHC PWG : PWG-CF (Flow and Correlations) System: Pb-Pb Energy: 5.02 TeV
Figure 5 Fig. Group : $\mathbf{\textbf{K}^{0}_{\textbf{S}}}-\mathbf{\textbf{K}^{0}_{\textbf{S}}}$ femtoscopy in Pb$-$Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.02}$ TeV at the LHC PWG : PWG-CF (Flow and Correlations) System: Pb-Pb Energy: 5.02 TeV
Figure 4 Fig. Group : $\mathbf{\textbf{K}^{0}_{\textbf{S}}}-\mathbf{\textbf{K}^{0}_{\textbf{S}}}$ femtoscopy in Pb$-$Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.02}$ TeV at the LHC PWG : PWG-CF (Flow and Correlations) System: Pb-Pb Energy: 5.02 TeV
Figure 3 Fig. Group : $\mathbf{\textbf{K}^{0}_{\textbf{S}}}-\mathbf{\textbf{K}^{0}_{\textbf{S}}}$ femtoscopy in Pb$-$Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.02}$ TeV at the LHC PWG : PWG-CF (Flow and Correlations) System: Pb-Pb Energy: 5.02 TeV
Figure 2 Fig. Group : $\mathbf{\textbf{K}^{0}_{\textbf{S}}}-\mathbf{\textbf{K}^{0}_{\textbf{S}}}$ femtoscopy in Pb$-$Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.02}$ TeV at the LHC PWG : PWG-CF (Flow and Correlations) System: Pb-Pb Energy: 5.02 TeV
Figure 1 Fig. Group : $\mathbf{\textbf{K}^{0}_{\textbf{S}}}-\mathbf{\textbf{K}^{0}_{\textbf{S}}}$ femtoscopy in Pb$-$Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.02}$ TeV at the LHC PWG : PWG-CF (Flow and Correlations) System: Pb-Pb Energy: 5.02 TeV
Figure 3 Fig. Group : Wave-Function Femtometry: Hypertriton - The Ultimate Halo Nucleus PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 1 Fig. Group : Wave-Function Femtometry: Hypertriton - The Ultimate Halo Nucleus PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 2 Fig. Group : Wave-Function Femtometry: Hypertriton - The Ultimate Halo Nucleus PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure A.1b Fig. Group : Wave-Function Femtometry: Hypertriton - The Ultimate Halo Nucleus PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure A.2 Fig. Group : Wave-Function Femtometry: Hypertriton - The Ultimate Halo Nucleus PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure A.1a Fig. Group : Wave-Function Femtometry: Hypertriton - The Ultimate Halo Nucleus PWG : PWG-LF (Light Flavour Spectra) System: p-p Energy: 13 TeV
Figure 2 Fig. Group : Dijet invariant mass of charged-particle jets in pp and p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV PWG : PWG-JE (Jets) System: p-p, p-Pb Energy: 5.02 TeV
Figure 1 Fig. Group : Dijet invariant mass of charged-particle jets in pp and p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV PWG : PWG-JE (Jets) System: p-p, p-Pb Energy: 5.02 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 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 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

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