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 $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D,\Lambda_{c}^{+}}| < 1$.

Distributions of the number of hits in the cluster (Nhits) for the DT category in the out-of-time (OOT) region. The last histogram bin contains all overflow events.

Distributions of the number of hits in the cluster (Nhits) for the CSC category in the out-of-time (OOT) region. The last histogram bin contains all overflow events.

The 95% CL observed and expected upper limits on the VLL production cross section as a function of the VLL mass for the pseudoscalar mean proper decay length c$\tau$ = 0.025 m. The pseudoscalar mass is 2 GeV.

The 95% CL observed and expected upper limits on the VLL production cross section as a function of the pseudoscalar mean proper decay length c$\tau$ for VLL Mass of 700 GeV. The pseudoscalar mass is 2 GeV.

The 95% CL observed upper limits on the VLL production cross section as a function of the VLL mass and the pseudoscalar mean proper decay length c$\tau$. The pseudoscalar mass is 2 GeV.

The 95% CL observed exclusion contour on the VLL production cross section as a function of the VLL mass and the pseudoscalar mean proper decay length c$\tau$. The pseudoscalar mass is 2 GeV.

Selection efficiencies in the CSC category signal region (SR) for different signal hypothesis. The pseudoscalar mass is 2 GeV.

Selection efficiencies in the DT category signal region (SR) for different signal hypothesis. The pseudoscalar mass is 2 GeV.

The cluster reconstruction efficiency, including both DT and CSC clusters, as a function of the simulated r and |z| decay positions of the pseudoscalar into photons in events with MET > 200 GeV, for a VLL mass of 300 GeV and a pseudoscalar mass of 2 GeV, and a range of ctau values uniformly distributed between 0.01 and 0.1 m.

The cluster reconstruction efficiency, including both DT and CSC clusters, as a function of the simulated r and |z| decay positions of the pseudoscalar into photons in events with MET > 200 GeV, for a VLL mass of 500 GeV and a pseudoscalar mass of 2 GeV, and a range of ctau values uniformly distributed between 0.01 and 0.1 m.

Source radius $r_0$ as a function of〈$m_\mathrm{T}$〉for the assumption of a purely Gaussian source. The blue crosses result from fitting the p–p correlation function with the strong Argonne v18 potential. The green squared crosses (red triangular crosses) result from fitting the p–Λ correlation functions with the strong χEFT LO (NLO) potential. Statistical (lines) and systematic (boxes) uncertainties are shown separately.

Source radius $r_{core}$ as a function of〈$m_{T}$〉for the assumption of a Gaussian source with added resonances. The blue crosses result from fitting the p–p correlation function with the strong Argonnev18 potential. The green squared crosses (red triangular crosses) result from fitting the p–Λ correlation functions withthe strong χEFT LO (NLO) potential. Statistical (lines) and systematic (boxes) uncertainties are shown separately.

Source radius as a function of $r_\mathrm{core}$ for the assumption of a Gaussian source with added resonances. The blue crosses result from fitting the p–p correlation function with the strong Argonnev18 potential. The green squared crosses (red triangular crosses) result from fitting the p–Λ correlation functions withthe strong χEFT LO (NLO) potential. Statistical (lines) and systematic (boxes) uncertainties are shown separately.

Source radius $r_{core}$ as a function of〈$m_{T}$〉for the assumption of a Gaussian source with added resonances. The blue crosses result from fitting the p–p correlation function with the strong Argonnev18 potential. The green squared crosses (red triangular crosses) result from fitting the p–Λ correlation functions withthe strong χEFT LO (NLO) potential. Statistical (lines) and systematic (boxes) uncertainties are shown separately.

Source radius as a function of $r_\mathrm{core}$ for the assumption of a Gaussian source with added resonances. The blue crosses result from fitting the p–p correlation function with the strong Argonnev18 potential. The green squared crosses (red triangular crosses) result from fitting the p–Λ correlation functions withthe strong χEFT LO (NLO) potential. Statistical (lines) and systematic (boxes) uncertainties are shown separately.

A plot identical to Fig. 5, where the red p–Λ points are obtained by using an Usmani potential tuned to point iv) described in Table 1 in Phys.Lett.B 850 (2024) 138550

The direct-photon fraction r in high-multiplicity pp collisions at $\sqrt{s}$ = 13 TeV as a function of transverse momentum for 1 < $p_{\rm T}$ < 6 GeV/$c$. r is the ratio of direct GAMMA to inclusive GAMMA.

The direct-photon inelastic cross section in pp collisions at $\sqrt{s}$ = 13 TeV as a function of transverse momentum for 1 < $p_{\rm T}$ < 6 GeV/$c$

The direct-photon invariant differential yield in high-multiplicity pp collisions at $\sqrt{s}$ = 13 TeV as a function of transverse momentum for 1 < $p_{\rm T}$ < 6 GeV/$c$

The integrated photon yield in inelastic and high-multiplicity pp collisions at $\sqrt{s}$ = 13 TeV as a function of charged particle multiplicity

The dielectron cross section in inelastic pp collisions at $\sqrt{s}$ = 13 TeV as a function of invariant mass for 1 < $p_{\rm T,ee}$ < 2 GeV/$c$.

The dielectron cross section in high-multiplicity pp collisions at $\sqrt{s}$ = 13 TeV as a function of invariant mass for 1 < $p_{\rm T,ee}$ < 2 GeV/$c$.

The dielectron cross section in inelastic pp collisions at $\sqrt{s}$ = 13 TeV as a function of invariant mass for 3 < $p_{\rm T,ee}$ < 6 GeV/$c$.

The dielectron cross section in high-multiplicity pp collisions at $\sqrt{s}$ = 13 TeV as a function of invariant mass for 3 < $p_{\rm T,ee}$ < 6 GeV/$c$.

$\rm \Xi_c^+/D^0$ ratio as a function of $p_{\rm T}$ in pp collisions at $\sqrt{s}=13$ TeV for $|y|<0.5$.

$\rm \Xi_c^0/\Lambda_c^+$ ratio as a function of $p_{\rm T}$ in pp collisions at $\sqrt{s}=13$ TeV for $|y|<0.5$.

$\rm \Xi_c^{0,+}/\Sigma_c^{0,+,++}$ ratio as a function of $p_{\rm T}$ in pp collisions at $\sqrt{s}=13$ TeV for $|y|<0.5$.

The $p_{\rm T}-$ integrated cross section of prompt $\Xi^{0}_{\rm c}-$baryon production in pp collisions at 13 TeV for $|y| < 0.5$.

The $p_{\rm T}-$ integrated cross section of prompt $\Xi^{0}_{\rm c}-$baryon production in pp collisions at 13 TeV for $|y| < 0.5$.

The $p_{\rm T}-$ integrated cross section of prompt $\Xi^{+}_{\rm c}-$baryon production in pp collisions at 13 TeV for $|y| < 0.5$.

The branching-fraction ratio $\rm {\rm BR}(\Xi_c^0\rightarrow \Xi^-e^+\nu_e)/\rm {\rm BR}(\Xi_c^0\rightarrow \Xi^{-}\pi^+)$ in pp collisions at 13 TeV for $|y| < 0.5$.

The unfolded charged particle thrust distribution of inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to 1.

The unfolded charged particle broadening distribution of inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to 1.

The unfolded charged particle isotropy distribution of inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to 1.

The unfolded charged particle transverse thrust distribution of inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to 1.

The unfolded charged particle transverse spherocity distribution of inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to 1.

The correlations of the uncertainties in the normalised charged particle multiplicity distribution of inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4.

The correlations of the uncertainties in the normalised charged particle invariant mass distribution of inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4.

The correlations of the uncertainties in the normalised charged particle sphericity distribution of inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4.

The correlations of the uncertainties in the normalised charged particle thrust distribution of inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4.

The correlations of the uncertainties in the normalised charged particle broadening distribution of inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4.

The correlations of the uncertainties in the normalised charged particle isotropy distribution of inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4.

The correlations of the uncertainties in the normalised charged particle transverse thrust distribution of inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4.

The correlations of the uncertainties in the normalised charged particle transverse spherocity distribution of inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4.

The unfolded charged particle invariant mass distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle invariant mass distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle invariant mass distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle invariant mass distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle invariant mass distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle sphericity distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle sphericity distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle sphericity distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle sphericity distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle sphericity distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle thrust distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle thrust distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle thrust distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle thrust distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle thrust distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle broadening distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle broadening distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle broadening distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle broadening distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle broadening distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle isotropy distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle isotropy distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle isotropy distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle isotropy distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle isotropy distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle transverse thrust distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle transverse thrust distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle transverse thrust distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle transverse thrust distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle transverse thrust distribution in a slice of multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle transverse spherocity distribution in a slice from multiplicity of inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle transverse spherocity distribution in a slice from multiplicity of inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle transverse spherocity distribution in a slice from multiplicity of inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle transverse spherocity distribution in a slice from multiplicity of inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded charged particle transverse spherocity distribution in a slice from multiplicity of inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to the fraction of events in this panel among all the panels.

The unfolded joint normalised distribution of charged particle invariant mass and multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to 1.

The unfolded joint normalised distribution of charged particle sphericity and multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to 1.

The unfolded joint normalised distribution of charged particle thrust and multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to 1.

The unfolded joint normalised distribution of charged particle broadening and multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to 1.

The unfolded joint normalised distribution of charged particle isotropy and multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to 1.

The unfolded joint normalised distribution of charged particle transverse thrust and multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to 1.

The unfolded joint normalised distribution of charged particle transverse spherocity and multiplicity of inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4. The total area of the histogram is normalised to 1.

The correlations of the uncertainties in the joint normalised distribution of charged particle invariant mass and multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4.

The correlations of the uncertainties in the joint normalised distribution of charged particle sphericity and multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4.

The correlations of the uncertainties in the joint normalised distribution of charged particle thrust and multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4.

The correlations of the uncertainties in the joint normalised distribution of charged particle broadening and multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4.

The correlations of the uncertainties in the joint normalised distribution of charged particle isotropy and multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4.

The correlations of the uncertainties in the joint normalised distribution of charged particle transverse thrust and multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4.

The correlations of the uncertainties in the joint normalised distribution of charged particle transverse spherocity and multiplicity from inelastic proton-proton collisions with at least three charged particles with transverse momentum higher than 0.5 GeV and pseudorapidity between -2.4 and 2.4.