| Figure 2
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| Figure 1d
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| Figure 1c
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| Figure 1b
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| Figure 1a
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| Acceptance-times-efficiency for prompt Ds hadrons in different multiplicity intervals (fig. 2b, Supp.)
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| Acceptance-times-efficiency for prompt D0 hadrons in different multiplicity intervals (fig. 2a, Supp.)
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| Acceptance-times-efficiency for prompt Λc → pK0S hadrons in different multiplicity intervals (fig. 2d, Supp.)
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| Acceptance-times-efficiency for prompt Λc → pK−π+ hadrons in different multiplicity intervals (fig. 2c, Supp.)
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| Invariant-mass (M) distributions of Ds candidates in 8<pt<12 GeV/c (fig. 1b, Supp.)
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| Invariant-mass (M) distributions of D0 --> Kpi candidates in 2<pt<4 GeV/c (fig. 1a, Supp.)
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| Invariant-mass (M) distributions of Λc → pK−π+ candidates in 6<pt<8 GeV/c (fig. 1d, Supp.)
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| Invariant-mass (M) distributions of Λc → pK−π+ candidates in 4<pt<6 GeV/c (fig. 1c, Supp.)
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| pT-integrated Ds/D0 yield ratios for pT > 0 and for the 4 < pT < 6 GeV/c (fig. 7b, Supp.)
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| pT-integrated Lc/D0 yield ratios for pT > 0 and for the 4 < pT < 6 GeV/c (fig. 7a, Supp.)
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| Ds/D0 pT-integrated yield ratios in the visible pT vs mult (fig. 6a, Supp.)
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| Λc/D0 pT-integrated yield ratios in the visible pT range vs mult (fig.6b Supp.)
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| pt>0 integrated yields of D0, Ds, Lc vs multiplicity (fig 5b supp)
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| Visible pt integrated yields of D0, Ds, Lc vs multiplicity (fig. 5a, Supp.)
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| Corrected yield of D0, Ds, Lc in different V0M multiplicity classes (fig. 3, Supp.)
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| Corrected yield of Lc->pKpi, pK0S in different V0M multiplicity classes (fig. 4b, Supp.)
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| Corrected yield of Lc->pKpi, pK0S in different Ntrk multiplicity classes (fig. 4a, Supp.)
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| Figure 2
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| Figure 1
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| Figure 2b
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