Observed and expected 95% CL upper limits on the cross section for the resonant production of a new spin-2 particle $\mathrm{X}^{(2)}$ which decays to Higgs boson pairs, $\sigma(\mathrm{pp} \to \mathrm{X}^{(2)} \to \mathrm{HH})$, given for different values of $m_\mathrm{X}$ in the range 260-1000 GeV.

Observed and expected 95% CL upper limits on the cross section for the resonant production of a new scalar particle $\mathrm{X}$ which decays to a SM Higgs boson and a new scalar particle $\mathrm{Y}$ which subsequently decay to a pair of photons and a pair of tau leptons, $\sigma(\mathrm{pp} \to \mathrm{X} \to \mathrm{YH} \to \gamma\gamma\tau\tau)$. The limits are shown for different values of $m_\mathrm{Y}$ in the range 50-800 GeV and at particular values of $m_\mathrm{X}$ in the range 300-1000 GeV.

Observed and expected 95% CL upper limits on the cross section for the resonant production of a new scalar particle $\mathrm{X}$ which decays to a SM Higgs boson and a new scalar particle $\mathrm{Y}$ which subsequently decay to a pair of photons and a pair of tau leptons, $\sigma(\mathrm{pp} \to \mathrm{X} \to \mathrm{YH} \to \gamma\gamma\tau\tau)$. The limits are shown for different values of $m_\mathrm{X}$ in the range 300-1000 GeV and at particular values of $m_\mathrm{Y}$ in the range 50-800 GeV.

Observed and expected 95% CL upper limits on the cross section for the resonant production of a new scalar particle $\mathrm{X}$ which decays to a SM Higgs boson and a new scalar particle $\mathrm{Y}$ which subsequently decay to a pair of photons and a pair of tau leptons, $\sigma(\mathrm{pp} \to \mathrm{X} \to \mathrm{YH} \to \gamma\gamma\tau\tau)$. The limits are shown for different values of $m_\mathrm{X}$ in the range 300-1000 GeV and $m_\mathrm{Y}$ in the range 50-800 GeV.

Observed and expected 95% CL upper limits on the cross section for the resonant production of a new scalar particle $\mathrm{X}$ which decays to a SM Higgs boson and a new scalar particle $\mathrm{Y}$, multiplied by the $\mathrm{Y} \to \gamma\gamma$ branching fraction, $\sigma(\mathrm{pp} \to \mathrm{X} \to \mathrm{YH})B(\mathrm{Y} \to \gamma\gamma)$. The limits are shown for different values of $m_\mathrm{Y}$ in the range 70-125 GeV and at particular values of $m_\mathrm{X}$ in the range 300-1000 GeV.

Observed and expected 95% CL upper limits on the cross section for the resonant production of a new scalar particle $\mathrm{X}$ which decays to a SM Higgs boson and a new scalar particle $\mathrm{Y}$, multiplied by the $\mathrm{Y} \to \gamma\gamma$ branching fraction, $\sigma(\mathrm{pp} \to \mathrm{X} \to \mathrm{YH})B(\mathrm{Y} \to \gamma\gamma)$. The limits are shown for different values of $m_\mathrm{X}$ in the range 300-800 GeV and at particular values of $m_\mathrm{Y}$ in the range 70-125 GeV.

Observed and expected 95% CL upper limits on the cross section for the resonant production of a new scalar particle $\mathrm{X}$ which decays to a SM Higgs boson and a new scalar particle $\mathrm{Y}$, multiplied by the $\mathrm{Y} \to \gamma\gamma$ branching fraction, $\sigma(\mathrm{pp} \to \mathrm{X} \to \mathrm{YH})B(\mathrm{Y} \to \gamma\gamma)$. The limits are shown for different values of $m_\mathrm{X}$ in the range 300-1000 GeV and $m_\mathrm{Y}$ in the range 70-125 GeV.

Observed and expected 95% CL upper limits on the cross section for the resonant production of a new scalar particle $\mathrm{X}$ which decays to a SM Higgs boson and a new scalar particle $\mathrm{Y}$, multiplied by the $\mathrm{Y} \to \gamma\gamma$ branching fraction, $\sigma(\mathrm{pp} \to \mathrm{X} \to \mathrm{YH})B(\mathrm{Y} \to \gamma\gamma)$. The limits are shown for different values of $m_\mathrm{Y}$ in the range 125-800 GeV and at particular values of $m_\mathrm{X}$ in the range 300-1000 GeV.

Observed and expected 95% CL upper limits on the cross section for the resonant production of a new scalar particle $\mathrm{X}$ which decays to a SM Higgs boson and a new scalar particle $\mathrm{Y}$, multiplied by the $\mathrm{Y} \to \gamma\gamma$ branching fraction, $\sigma(\mathrm{pp} \to \mathrm{X} \to \mathrm{YH})B(\mathrm{Y} \to \gamma\gamma)$. The limits are shown for different values of $m_\mathrm{X}$ in the range 300-800 GeV and at particular values of $m_\mathrm{Y}$ in the range 125-800 GeV.

Observed and expected 95% CL upper limits on the cross section for the resonant production of a new scalar particle $\mathrm{X}$ which decays to a SM Higgs boson and a new scalar particle $\mathrm{Y}$, multiplied by the $\mathrm{Y} \to \gamma\gamma$ branching fraction, $\sigma(\mathrm{pp} \to \mathrm{X} \to \mathrm{YH})B(\mathrm{Y} \to \gamma\gamma)$. The limits are shown for different values of $m_\mathrm{X}$ in the range 300-1000 GeV and $m_\mathrm{Y}$ in the range 125-800 GeV.

Figure 8(left) of the article. Differential fiducial cross-section of the Z boson $p_T$ in events with $Z \left( \rightarrow \ell\ell \right) + 1 b$-jet. The thin inner band corresponds to the statistical uncertainty of the data, and the outer band to statistical and systematic uncertainties of the data, added in quadrature.

Figure 8(right) of the article. Differential fiducial cross-section of the leading $b$-jet $p_T$ in events with $Z \left( \rightarrow \ell\ell \right) + 1 b$-jet. The thin inner band corresponds to the statistical uncertainty of the data, and the outer band to statistical and systematic uncertainties of the data, added in quadrature.

Figure 9 of the article. Differential fiducial cross-section of the $\Delta R$ between the $Z$ boson and the leading $b$-jet in events with $Z \left( \rightarrow \ell\ell \right) + 1 b$-jet. The thin inner band corresponds to the statistical uncertainty of the data, and the outer band to statistical and systematic uncertainties of the data, added in quadrature.

Figure 10(left) of the article. Differential fiducial cross-section of the $\Delta \phi$ between the leading and sub-leading $b$-jets in events with $Z \left( \rightarrow \ell\ell \right) + 2 b$-jets. The thin inner band corresponds to the statistical uncertainty of the data, and the outer band to statistical and systematic uncertainties of the data, added in quadrature.

Figure 10(right) of the article. Differential fiducial cross-section of the invariant mass of the leading and sub-leading $b$-jets in events with $Z \left( \rightarrow \ell\ell \right) + 2 b$-jets. The thin inner band corresponds to the statistical uncertainty of the data, and the outer band to statistical and systematic uncertainties of the data, added in quadrature.

Figure 11(left) of the article. Differential fiducial cross-section of the Z boson $p_T$ in events with $Z \left( \rightarrow \ell\ell \right) + 1 c$-jet. The thin inner band corresponds to the statistical uncertainty of the data, and the outer band to statistical and systematic uncertainties of the data, added in quadrature.

Figure 11(right) of the article. Differential fiducial cross-section of the leading $c$-jet $p_T$ in events with $Z \left( \rightarrow \ell\ell ight) + 1 c$-jet. The thin inner band corresponds to the statistical uncertainty of the data, and the outer band to statistical and systematic uncertainties of the data, added in quadrature.

Figure 12 of the article. Differential fiducial cross-section of the leading $c$-jet $x_F$ in events with $Z \left( \rightarrow \ell\ell \right) + 1 c$-jet. The thin inner band corresponds to the statistical uncertainty of the data, and the outer band to statistical and systematic uncertainties of the data, added in quadrature.

Correction factors from parton level done with flavour dressing algorithms as seen in Ref. [2] of the paper to hadron level with R 0.3 cone labelling (see Tables 18 & 24) for the differential cross-section of the Z boson $p_T$ in events with $Z (\rightarrow ll) \ge 1 $ b-jets. Systematic errors include Sherpa 2.2.11 and MGaMC+Py8 FxFx uncertainties for what concerns the passage from hadron level flavour dressing to hadron level cone labelling, plus statistical uncertainty of Pythia8 simulations used for parton to hadron corrections. See Table 4.

Correction factors from parton level done with flavour dressing algorithms as seen in Ref. [2] of the paper to hadron level with R 0.3 cone labelling (see Tables 19 & 25) for the differential cross-section of the Z boson $p_T$ in events with $Z (\rightarrow ll) \ge 1 $ c-jets. Systematic errors include Sherpa 2.2.11 and MGaMC+Py8 FxFx uncertainties for what concerns the passage from hadron level flavour dressing to hadron level cone labelling, plus statistical uncertainty of Pythia8 simulations used for parton to hadron corrections. See Table 9.

Correction factors from parton level done with flavour dressing algorithms as seen in Ref. [2] of the paper to hadron level with R 0.3 cone labelling (see Tables 20 & 26) for the differential cross-section of the leading $b$-jet $p_T$ in events with $Z (\rightarrow ll) \ge 1 $ b-jets. Systematic errors include Sherpa 2.2.11 and MGaMC+Py8 FxFx uncertainties for what concerns the passage from hadron level flavour dressing to hadron level cone labelling, plus statistical uncertainty of Pythia8 simulations used for parton to hadron corrections. See Table 5.

Correction factors from parton level done with flavour dressing algorithms as seen in Ref. [2] of the paper to hadron level with R 0.3 cone labelling (see Tables 21 & 27) for the differential cross-section of the leading $c$-jet $p_T$ in events with $Z (\rightarrow ll) \ge 1 $ c-jets. Systematic errors include Sherpa 2.2.11 and MGaMC+Py8 FxFx uncertainties for what concerns the passage from hadron level flavour dressing to hadron level cone labelling, plus statistical uncertainty of Pythia8 simulations used for parton to hadron corrections. See Table 10.

Correction factors from parton level done with flavour dressing algorithms as seen in Ref. [2] of the paper to hadron level with R 0.3 cone labelling (see Tables 22 & 28) for the differential cross-section of the leading $c$-jet $x_F$ in events with $Z (\rightarrow ll) \ge 1 $ c-jets. Systematic errors include Sherpa 2.2.11 and MGaMC+Py8 FxFx uncertainties for what concerns the passage from hadron level flavour dressing to hadron level cone labelling, plus statistical uncertainty of Pythia8 simulations used for parton to hadron corrections. See Table 11.

Correction factors from parton level done with flavour dressing algorithms as seen in Ref. [2] of the paper of the paper to hadron level with R 0.3 cone labelling (see Tables 23 & 29) for the differential cross-section of $\Delta R$ between the $Z$ boson and the leading $b$-jet in events with $Z (\rightarrow ll) \ge 1 $ b-jets. Systematic errors include Sherpa 2.2.11 and MGaMC+Py8 FxFx uncertainties for what concerns the passage from hadron level flavour dressing to hadron level cone labelling, plus statistical uncertainty of Pythia8 simulations used for parton to hadron corrections. See Table 6.

Correction factors from hadron level done with flavour dressing algorithms as seen in Ref. [2] of the paper to hadron level R 0.3 cone labelling for the differential cross-section of the Z boson $p_T$ in events with $Z (\rightarrow ll) \ge 1 $ b-jets. Systematic errors include Sherpa 2.2.11 and MGaMC+Py8 FxFx uncertainties. See Table 12.

Correction factors from hadron level done with flavour dressing algorithms as seen in Ref. [2] of the paper to hadron level with R 0.3 cone labelling for the differential cross-section of the Z boson $p_T$ in events with $Z (\rightarrow ll) \ge 1 $ c-jets. Systematic errors include Sherpa 2.2.11 and MGaMC+Py8 FxFx uncertainties. See Table 13.

Correction factors from hadron level done with flavour dressing algorithms as seen in Ref. [2] of the paper to hadron level with R 0.3 cone labelling for the differential cross-section of the leading $b$-jet $p_T$ in events with $Z (\rightarrow ll) \ge 1 $ b-jets. Systematic errors include Sherpa 2.2.11 and MGaMC+Py8 FxFx uncertainties. See Table 14.

Correction factors from hadron level done with flavour dressing algorithms as seen in Ref. [2] of the paper to hadron level with R 0.3 cone labelling for the differential cross-section of the leading $c$-jet $p_T$ in events with $Z (\rightarrow ll) \ge 1 $ c-jets. Systematic errors include Sherpa 2.2.11 and MGaMC+Py8 FxFx uncertainties. See Table 15.

Correction factors from hadron level done with flavour dressing algorithms as seen in Ref. [2] of the paper to hadron level with R 0.3 cone labelling for the differential cross-section of the leading $c$-jet $x_F$ in events with $Z (\rightarrow ll) \ge 1 $ c-jets. Systematic errors include Sherpa 2.2.11 and MGaMC+Py8 FxFx uncertainties. See Table 16.

Correction factors from hadron level done with flavour dressing algorithms as seen in Ref. [2] of the paper of the paper to hadron level with R 0.3 cone labelling for the differential cross-section of $\Delta R$ between the $Z$ boson and the leading $b$-jet in events with $Z (\rightarrow ll) \ge 1 $ b-jets. Systematic errors include Sherpa 2.2.11 and MGaMC+Py8 FxFx uncertainties. See Table 17.

Correction factors from parton level to hadron level for the differential cross-section of the Z boson $p_T$ in events with $Z (\rightarrow ll) \ge 1 $ b-jets. Systematic errors statistical uncertainty of Pythia8 simulations. See Table 12.

Correction factors from parton level to hadron level for the differential cross-section of the Z boson $p_T$ in events with $Z (\rightarrow ll) \ge 1 $ c-jets. Systematic errors include statistical uncertainty of Pythia8 simulations. See Table 13.

Correction factors from parton level to hadron level for the differential cross-section of the leading $b$-jet $p_T$ in events with $Z (\rightarrow ll) \ge 1 $ b-jets. Systematic errors include statistical uncertainty of Pythia8 simulations. See Table 14.

Correction factors from parton level to hadron level for the differential cross-section of the leading $c$-jet $p_T$ in events with $Z (\rightarrow ll) \ge 1 $ c-jets. Systematic errors include statistical uncertainty of Pythia8 simulations. See Table 15.

Correction factors from parton level to hadron level for the differential cross-section of the leading $c$-jet $x_F$ in events with $Z (\rightarrow ll) \ge 1 $ c-jets. Systematic errors include statistical uncertainty of Pythia8 simulations. See Table 16.

Correction factors from parton level to hadron level for the differential cross-section of $\Delta R$ between the $Z$ boson and the leading $b$-jet in events with $Z (\rightarrow ll) \ge 1 $ b-jets. Systematic errors include statistical uncertainty of Pythia8 simulations. See Table 17.

NSC(6,3) vs centrality in Pb-Pb collisions at 5.02 TeV

NSC(5,4) vs centrality in Pb-Pb collisions at 5.02 TeV

Comparison between the values of the near-side associated peak yield for D mesons (average of D$^{0}$, D$^{+}$, and D$^{*+}$) and $\Lambda_\mathrm{c}^{+}$ correlated with charged particles, as a function of the charm-hadron $p_{\rm T}$, for associated particle $ p_{\rm T} > 0.3 $ GeV/$c$. The rapidity range for the charm hadrons is $|y^{\rm D,\Lambda_{c}^{+}}| < 0.5$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D,\Lambda_{c}^{+}}| < 1$.

Comparison between the values of the near-side associated peak yield for D mesons (average of D$^{0}$, D$^{+}$, and D$^{*+}$) and $\Lambda_\mathrm{c}^{+}$ correlated with charged particles, as a function of the charm-hadron $p_{\rm T}$, for associated particle $ 0.3 < p_{\rm T} < 1 $ GeV/$c$. The rapidity range for the charm hadrons is $|y^{\rm D,\Lambda_{c}^{+}}| < 0.5$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D,\Lambda_{c}^{+}}| < 1$.

Comparison between the values of the near-side associated peak yield for D mesons (average of D$^{0}$, D$^{+}$, and D$^{*+}$) and $\Lambda_\mathrm{c}^{+}$ correlated with charged particles, as a function of the charm-hadron $p_{\rm T}$, for associated particle $ p_{\rm T} > 1.0 $ GeV/$c$. The rapidity range for the charm hadrons is $|y^{\rm D,\Lambda_{c}^{+}}| < 0.5$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D,\Lambda_{c}^{+}}| < 1$.

Ratio between the values of the near-side associated peak yield of the $\Lambda_\mathrm{c}^{+}$ and D mesons (average of D$^{0}$, D$^{+}$, and D$^{*+}$) azimuthal correlation distribution with charged particles, as a function of the charm-hadron $p_{\rm T}$, for associated particle $ p_{\rm T} > 0.3 $ GeV/$c$. The rapidity range for the charm hadrons is $|y^{\rm D,\Lambda_{c}^{+}}| < 0.5$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D,\Lambda_{c}^{+}}| < 1$.

Ratio between the values of the near-side associated peak yield of the $\Lambda_\mathrm{c}^{+}$ and D mesons (average of D$^{0}$, D$^{+}$, and D$^{*+}$) azimuthal correlation distribution with charged particles, as a function of the charm-hadron $p_{\rm T}$, for associated particle $ 0.3 < p_{\rm T} < 1 $ GeV/$c$. The rapidity range for the charm hadrons is $|y^{\rm D,\Lambda_{c}^{+}}| < 0.5$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D,\Lambda_{c}^{+}}| < 1$.

Ratio between the values of the near-side associated peak yield of the $\Lambda_\mathrm{c}^{+}$ and D mesons (average of D$^{0}$, D$^{+}$, and D$^{*+}$) azimuthal correlation distribution with charged particles, as a function of the charm-hadron $p_{\rm T}$, for associated particle $ p_{\rm T} > 1.0 $ GeV/$c$. The rapidity range for the charm hadrons is $|y^{\rm D,\Lambda_{c}^{+}}| < 0.5$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D,\Lambda_{c}^{+}}| < 1$.

Comparison between the values of the near-side associated peak width for D mesons (average of D$^{0}$, D$^{+}$, and D$^{*+}$) and $\Lambda_\mathrm{c}^{+}$ correlated with charged particles, as a function of the charm-hadron $p_{\rm T}$, for associated particle $ p_{\rm T} > 0.3 $ GeV/$c$. The rapidity range for the charm hadrons is $|y^{\rm D,\Lambda_{c}^{+}}| < 0.5$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D,\Lambda_{c}^{+}}| < 1$.

Comparison between the values of the near-side associated peak width for D mesons (average of D$^{0}$, D$^{+}$, and D$^{*+}$) and $\Lambda_\mathrm{c}^{+}$ correlated with charged particles, as a function of the charm-hadron $p_{\rm T}$, for associated particle $ 0.3 < p_{\rm T} < 1.0 $ GeV/$c$. The rapidity range for the charm hadrons is $|y^{\rm D,\Lambda_{c}^{+}}| < 0.5$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D,\Lambda_{c}^{+}}| < 1$.

Comparison between the values of the near-side associated peak width for D mesons (average of D$^{0}$, D$^{+}$, and D$^{*+}$) and $\Lambda_\mathrm{c}^{+}$ correlated with charged particles, as a function of the charm-hadron $p_{\rm T}$, for associated particle $ p_{\rm T} > 1.0 $ GeV/$c$. The rapidity range for the charm hadrons is $|y^{\rm D,\Lambda_{c}^{+}}| < 0.5$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D,\Lambda_{c}^{+}}| < 1$.

Ratio between the values of the near-side associated peak width of the $\Lambda_\mathrm{c}^{+}$ and D mesons (average of D$^{0}$, D$^{+}$, and D$^{*+}$) azimuthal correlation distribution with charged particles, as a function of the charm-hadron $p_{\rm T}$, for associated particle $ p_{\rm T} > 0.3 $ GeV/$c$. The rapidity range for the charm hadrons is $|y^{\rm D,\Lambda_{c}^{+}}| < 0.5$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D,\Lambda_{c}^{+}}| < 1$.

Ratio between the values of the near-side associated peak width of the $\Lambda_\mathrm{c}^{+}$ and D mesons (average of D$^{0}$, D$^{+}$, and D$^{*+}$) azimuthal correlation distribution with charged particles, as a function of the charm-hadron $p_{\rm T}$, for associated particle $ 0.3 < p_{\rm T} < 1.0 $ GeV/$c$. The rapidity range for the charm hadrons is $|y^{\rm D,\Lambda_{c}^{+}}| < 0.5$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D,\Lambda_{c}^{+}}| < 1$.

Ratio between the values of the near-side associated peak width of the $\Lambda_\mathrm{c}^{+}$ and D mesons (average of D$^{0}$, D$^{+}$, and D$^{*+}$) azimuthal correlation distribution with charged particles, as a function of the charm-hadron $p_{\rm T}$, for associated particle $ p_{\rm T} > 1.0 $ GeV/$c$. The rapidity range for the charm hadrons is $|y^{\rm D,\Lambda_{c}^{+}}| < 0.5$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D,\Lambda_{c}^{+}}| < 1$.

Comparison between the values of the away-side associated peak yield for D mesons (average of D$^{0}$, D$^{+}$, and D$^{*+}$) and $\Lambda_\mathrm{c}^{+}$ correlated with charged particles, as a function of the charm-hadron $p_{\rm T}$, for associated particle $ p_{\rm T} > 0.3 $ GeV/$c$. The rapidity range for the charm hadrons is $|y^{\rm D,\Lambda_{c}^{+}}| < 0.5$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D,\Lambda_{c}^{+}}| < 1$.

Comparison between the values of the away-side associated peak yield for D mesons (average of D$^{0}$, D$^{+}$, and D$^{*+}$) and $\Lambda_\mathrm{c}^{+}$ correlated with charged particles, as a function of the charm-hadron $p_{\rm T}$, for associated particle $ 0.3 < p_{\rm T} < 1 $ GeV/$c$. The rapidity range for the charm hadrons is $|y^{\rm D,\Lambda_{c}^{+}}| < 0.5$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D,\Lambda_{c}^{+}}| < 1$.

Comparison between the values of the away-side associated peak yield for D mesons (average of D$^{0}$, D$^{+}$, and D$^{*+}$) and $\Lambda_\mathrm{c}^{+}$ correlated with charged particles, as a function of the charm-hadron $p_{\rm T}$, for associated particle $ p_{\rm T} > 1.0 $ GeV/$c$. The rapidity range for the charm hadrons is $|y^{\rm D,\Lambda_{c}^{+}}| < 0.5$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D,\Lambda_{c}^{+}}| < 1$.

Ratio between the values of the away-side associated peak yield of the $\Lambda_\mathrm{c}^{+}$ and D mesons (average of D$^{0}$, D$^{+}$, and D$^{*+}$) azimuthal correlation distribution with charged particles, as a function of the charm-hadron $p_{\rm T}$, for associated particle $ p_{\rm T} > 0.3 $ GeV/$c$. The rapidity range for the charm hadrons is $|y^{\rm D,\Lambda_{c}^{+}}| < 0.5$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D,\Lambda_{c}^{+}}| < 1$.

Ratio between the values of the away-side associated peak yield of the $\Lambda_\mathrm{c}^{+}$ and D mesons (average of D$^{0}$, D$^{+}$, and D$^{*+}$) azimuthal correlation distribution with charged particles, as a function of the charm-hadron $p_{\rm T}$, for associated particle $ 0.3 < p_{\rm T} < 1 $ GeV/$c$. The rapidity range for the charm hadrons is $|y^{\rm D,\Lambda_{c}^{+}}| < 0.5$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D,\Lambda_{c}^{+}}| < 1$.

Ratio between the values of the away-side associated peak yield of the $\Lambda_\mathrm{c}^{+}$ and D mesons (average of D$^{0}$, D$^{+}$, and D$^{*+}$) azimuthal correlation distribution with charged particles, as a function of the charm-hadron $p_{\rm T}$, for associated particle $ p_{\rm T} > 1.0 $ GeV/$c$. The rapidity range for the charm hadrons is $|y^{\rm D,\Lambda_{c}^{+}}| < 0.5$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D,\Lambda_{c}^{+}}| < 1$.