Data compared to the SM prediction in each region of the positive \lam{} analysis, after the fit to data. The shaded bands represent the total post-fit uncertainty on the prediction.

Fit results in the ($\kappa_{Z}$, $\kappa_{W}$) plane, using the negative-$\lambda_{WZ}$ analysis. The results are overlaid with the confidence regions (shown in blue) from a separate fit using a combination of the Higgs boson measurements collected in Nature 607 (2022) 52. This fit assumes that all Higgs boson couplings besides the ones represented are positive, and that only SM particles contribute to loop processes. Confidence regions are constructed from the log-likelihood ratio $\Lambda_{LR}=-2\ln(L/L_{max})$, where $L_{\max}$ is the likelihood for the best-fit point, which is shown as a black dot for the VBF $WH$ analysis or a blue dot for the Higgs combination. The $1\sigma$, $2\sigma$, and $5\sigma$ regions are defined by $\Lambda_{LR}$ values smaller than 2.30, 6.18, and 28.7, respectively. The SM value is marked with a star, while green triangles mark the points with $\kappa_{Z} = \pm1$, $\kappa_{W} = \mp1$.

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/$c$.

Example description

Differential fiducial cross sections for the number of jets

Example description

Differential fiducial cross sections for the leading jet pT

Example description

Normalized transverse momentum correlator, $\sqrt{ \langle\langle \Delta p_{{\rm T}1}\Delta p_{{\rm T}2} \rangle\rangle }/\langle\langle p_{\rm T} \rangle\rangle $, as a function of the average number of participant nucleons, $\langle{ N_{\rm part}}\rangle$, in Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV

Normalized transverse momentum correlator, $\sqrt{ \langle\langle \Delta p_{{\rm T}1}\Delta p_{{\rm T}2} \rangle\rangle }/\langle\langle p_{\rm T} \rangle\rangle $, as a function of the average number of participant nucleons, $\langle{ N_{\rm part}}\rangle$, in Xe--Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV

Normalized transverse momentum correlator, $\sqrt{ \langle\langle \Delta p_{{\rm T}1}\Delta p_{{\rm T}2} \rangle\rangle }/\langle\langle p_{\rm T} \rangle\rangle $, as a function of the average number of participant nucleons, $\langle{ N_{\rm part}}\rangle$, in Pb--Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV

Normalized transverse momentum correlator, $\sqrt{ \langle\langle \Delta p_{{\rm T}1}\Delta p_{{\rm T}2} \rangle\rangle }/\langle\langle p_{\rm T} \rangle\rangle $ as a function of the charged-particle multiplicity density for spherocity-integrated events in pp collisions at $\sqrt{s}=5.02$ TeV

Normalized transverse momentum correlator, $\sqrt{ \langle\langle \Delta p_{{\rm T}1}\Delta p_{{\rm T}2} \rangle\rangle }/\langle\langle p_{\rm T} \rangle\rangle $ as a function of the charged-particle multiplicity density for jetty events in pp collisions at $\sqrt{s}=5.02$ TeV

Normalized transverse momentum correlator, $\sqrt{ \langle\langle \Delta p_{{\rm T}1}\Delta p_{{\rm T}2} \rangle\rangle }/\langle\langle p_{\rm T} \rangle\rangle $ as a function of the charged-particle multiplicity density for isotropic events in pp collisions at $\sqrt{s}=5.02$ TeV

Normalized transverse momentum correlator, $\sqrt{ \langle\langle \Delta p_{{\rm T}1}\Delta p_{{\rm T}2} \rangle\rangle }/\langle\langle p_{\rm T} \rangle\rangle $ as a function of the charged-particle multiplicity density for spherocity-integrated events in pp collisions at $\sqrt{s}=13$ TeV

Normalized transverse momentum correlator, $\sqrt{ \langle\langle \Delta p_{{\rm T}1}\Delta p_{{\rm T}2} \rangle\rangle }/\langle\langle p_{\rm T} \rangle\rangle $ as a function of the charged-particle multiplicity density for jetty events in pp collisions at $\sqrt{s}=13$ TeV

Normalized transverse momentum correlator, $\sqrt{ \langle\langle \Delta p_{{\rm T}1}\Delta p_{{\rm T}2} \rangle\rangle }/\langle\langle p_{\rm T} \rangle\rangle $ as a function of the charged-particle multiplicity density for isotropic events in pp collisions at $\sqrt{s}=13$ TeV

Systematic covariance matrix for the differential cross-section distribution.