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Figure 4e Fig. Group : Studying strangeness and baryon production mechanisms through angular correlations between charged $Ξ$ baryons and identified hadrons in pp collisions at $\sqrt{s}$ = 13 TeV PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 4f Fig. Group : Studying strangeness and baryon production mechanisms through angular correlations between charged $Ξ$ baryons and identified hadrons in pp collisions at $\sqrt{s}$ = 13 TeV PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 5a Fig. Group : Studying strangeness and baryon production mechanisms through angular correlations between charged $Ξ$ baryons and identified hadrons in pp collisions at $\sqrt{s}$ = 13 TeV PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 5b Fig. Group : Studying strangeness and baryon production mechanisms through angular correlations between charged $Ξ$ baryons and identified hadrons in pp collisions at $\sqrt{s}$ = 13 TeV PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 5c Fig. Group : Studying strangeness and baryon production mechanisms through angular correlations between charged $Ξ$ baryons and identified hadrons in pp collisions at $\sqrt{s}$ = 13 TeV PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 6a Fig. Group : Studying strangeness and baryon production mechanisms through angular correlations between charged $Ξ$ baryons and identified hadrons in pp collisions at $\sqrt{s}$ = 13 TeV PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 6b Fig. Group : Studying strangeness and baryon production mechanisms through angular correlations between charged $Ξ$ baryons and identified hadrons in pp collisions at $\sqrt{s}$ = 13 TeV PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 6c Fig. Group : Studying strangeness and baryon production mechanisms through angular correlations between charged $Ξ$ baryons and identified hadrons in pp collisions at $\sqrt{s}$ = 13 TeV PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 7a Fig. Group : Studying strangeness and baryon production mechanisms through angular correlations between charged $Ξ$ baryons and identified hadrons in pp collisions at $\sqrt{s}$ = 13 TeV PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 7b Fig. Group : Studying strangeness and baryon production mechanisms through angular correlations between charged $Ξ$ baryons and identified hadrons in pp collisions at $\sqrt{s}$ = 13 TeV PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 7c Fig. Group : Studying strangeness and baryon production mechanisms through angular correlations between charged $Ξ$ baryons and identified hadrons in pp collisions at $\sqrt{s}$ = 13 TeV PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 4d Fig. Group : Studying strangeness and baryon production mechanisms through angular correlations between charged $Ξ$ baryons and identified hadrons in pp collisions at $\sqrt{s}$ = 13 TeV PWG : PWG-CF (Flow and Correlations) System: p-p Energy: 13 TeV
Figure 4b Fig. Group : Investigating charm quark energy loss in medium with the nuclear modification factor of D$^0$-tagged jets PWG : PWG-HF (Heavy Flavour) System: Pb-Pb Energy: 5.02 TeV
Figure 1 Fig. Group : Investigating charm quark energy loss in medium with the nuclear modification factor of D$^0$-tagged jets PWG : PWG-HF (Heavy Flavour) System: Pb-Pb Energy: 5.02 TeV
Figure 2 Fig. Group : Investigating charm quark energy loss in medium with the nuclear modification factor of D$^0$-tagged jets PWG : PWG-HF (Heavy Flavour) System: Pb-Pb Energy: 5.02 TeV
Figure 4a Fig. Group : Investigating charm quark energy loss in medium with the nuclear modification factor of D$^0$-tagged jets PWG : PWG-HF (Heavy Flavour) System: Pb-Pb Energy: 5.02 TeV
Figure 3 Fig. Group : Investigating charm quark energy loss in medium with the nuclear modification factor of D$^0$-tagged jets PWG : PWG-HF (Heavy Flavour) System: Pb-Pb Energy: 5.02 TeV
Figure 1 Fig. Group : Addendum: Dielectron production in proton-proton and proton-lead collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV PWG : PWG-EM (Electromagnetic probes) System: p-p, p-Pb Energy: 5.02 TeV
Figure 97 Fig. Group : ALICE upgrades during the LHC Long Shutdown 2 PWG : UPGRADE System: Upgrade Energy: none
Figure 96 Fig. Group : ALICE upgrades during the LHC Long Shutdown 2 PWG : UPGRADE System: Upgrade Energy: none
Figure 95 Fig. Group : ALICE upgrades during the LHC Long Shutdown 2 PWG : UPGRADE System: Upgrade Energy: none
Figure 94 Fig. Group : ALICE upgrades during the LHC Long Shutdown 2 PWG : UPGRADE System: Upgrade Energy: none
Figure 92 Fig. Group : ALICE upgrades during the LHC Long Shutdown 2 PWG : UPGRADE System: Upgrade Energy: none
Figure 89 Fig. Group : ALICE upgrades during the LHC Long Shutdown 2 PWG : UPGRADE System: Upgrade Energy: none

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