Intensive skewness of $\langle p_\mathrm{T}\rangle$ as a function of $\langle\mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle^{1/3}_{|\eta|<0.5}$ in pp collisions at $\sqrt{s}$ = 5.02 TeV.

Intensive skewness of $\langle p_\mathrm{T}\rangle$ as a function of $\langle\mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle^{1/3}_{|\eta|<0.5}$ in Xe$-$Xe collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV.

Intensive skewness of $\langle p_\mathrm{T}\rangle$ as a function of $\langle\mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle^{1/3}_{|\eta|<0.5}$ in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV.

Kurtosis of $\langle p_\mathrm{T}\rangle$ as a function of $\langle\mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle^{1/3}_{|\eta|<0.5}$ in pp collisions at $\sqrt{s}$ = 5.02 TeV.

Kurtosis of $\langle p_\mathrm{T}\rangle$ as a function of $\langle\mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle^{1/3}_{|\eta|<0.5}$ in Xe$-$Xe collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV.

Kurtosis of $\langle p_\mathrm{T}\rangle$ as a function of $\langle\mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle^{1/3}_{|\eta|<0.5}$ in Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV.

Corrected $\Delta_\mathrm{recoil} (\Delta\varphi)$ distributions measured for $R=$ 0.2 in pp collisions at $\sqrt{s}=5.02$ TeV, in $p_\mathrm{T,ch jet}$ bins [10,20], [20,30], [30,50] and [50,100] GeV/$c$.

Corrected $\Delta_\mathrm{recoil} (\Delta\varphi)$ distributions measured for $R=$ 0.4 in pp collisions at $\sqrt{s}=5.02$ TeV, in $p_\mathrm{T,ch jet}$ bins [10,20], [20,30], [30,50] and [50,100] GeV/$c$.

Corrected $\Delta_\mathrm{recoil} (\Delta\varphi)$ distributions measured for $R=$ 0.5 in pp collisions at $\sqrt{s}=5.02$ TeV, in $p_\mathrm{T,ch jet}$ bins [10,20], [20,30], [30,50] and [50,100] GeV/$c$.

Corrected $\Delta_\mathrm{recoil} (\Delta\varphi)$ distributions measured for $R=$ 0.2 in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV, in $p_\mathrm{T,ch jet}$ bins [10,20], [20,30], [30,50] and [50,100] GeV/$c$.

Corrected $\Delta_\mathrm{recoil} (\Delta\varphi)$ distributions measured for $R=$ 0.4 in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV, in $p_\mathrm{T,ch jet}$ bins [10,20], [20,30], [30,50] and [50,100] GeV/$c$.

Corrected $\Delta_\mathrm{recoil} (\Delta\varphi)$ distributions measured for $R=$ 0.5 in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV, in $p_\mathrm{T,ch jet}$ bins [10,20], [20,30], [30,50] and [50,100] GeV/$c$.

$I_\mathrm{AA} (\Delta\varphi)$ distributions measured for $R=$ 0.2 in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV, in $p_\mathrm{T,ch jet}$ bins [10,20], [20,30], [30,50] and [50,100] GeV/$c$.

$I_\mathrm{AA} (\Delta\varphi)$ distributions measured for $R=$ 0.4 in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV, in $p_\mathrm{T,ch jet}$ bins [10,20], [20,30], [30,50] and [50,100] GeV/$c$.

$I_\mathrm{AA} (\Delta\varphi)$ distributions measured for $R=$ 0.5 in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV, in $p_\mathrm{T,ch jet}$ bins [10,20], [20,30], [30,50] and [50,100] GeV/$c$.

$\Delta_\mathrm{recoil} (p_\mathrm{T,ch jet})$ ratios $R=$ 0.2 / 0.4 in pp and Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV.

$\Delta_\mathrm{recoil} (p_\mathrm{T,ch jet})$ ratios $R=$ 0.2 / 0.5 in pp and Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV.

$\Delta_\mathrm{recoil} (p_\mathrm{T,ch jet})$ ratios $R=$ 0.4 / 0.5 in pp and Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV.

$\Delta_\mathrm{recoil} (p_\mathrm{T,ch jet})$ for $R=$ 0.2, for various $\mathrm{TT_{sig}}$ selections in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV.

$\Delta_\mathrm{recoil} (p_\mathrm{T,ch jet})$ for $R=$ 0.4, for various $\mathrm{TT_{sig}}$ selections in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV.

Corrected $\Delta_\mathrm{recoil} (\Delta\varphi)$ distributions measured for $R=$ 0.2 in pp collisions at $\sqrt{s}=5.02$ TeV, in $p_\mathrm{T,ch jet}$ bins [10,20], [20,30], [30,50] and [50,100] GeV/$c$.

Corrected $\Delta_\mathrm{recoil} (\Delta\varphi)$ distributions measured for $R=$ 0.4 in pp collisions at $\sqrt{s}=5.02$ TeV, in $p_\mathrm{T,ch jet}$ bins [10,20], [20,30], [30,50] and [50,100] GeV/$c$.

Corrected $\Delta_\mathrm{recoil} (\Delta\varphi)$ distributions measured for $R=$ 0.5 in pp collisions at $\sqrt{s}=5.02$ TeV, in $p_\mathrm{T,ch jet}$ bins [10,20], [20,30], [30,50] and [50,100] GeV/$c$.

Corrected $\Delta_\mathrm{recoil} (\Delta\varphi)$ distributions measured for $R=$ 0.2 in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV, in $p_\mathrm{T,ch jet}$ bins [10,20], [20,30], [30,50] and [50,100] GeV/$c$.

Corrected $\Delta_\mathrm{recoil} (\Delta\varphi)$ distributions measured for $R=$ 0.4 in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV, in $p_\mathrm{T,ch jet}$ bins [10,20], [20,30], [30,50] and [50,100] GeV/$c$.

Corrected $\Delta_\mathrm{recoil} (\Delta\varphi)$ distributions measured for $R=$ 0.5 in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV, in $p_\mathrm{T,ch jet}$ bins [10,20], [20,30], [30,50] and [50,100] GeV/$c$.

$I_\mathrm{AA} (\Delta\varphi)$ distributions measured for $R=$ 0.2 in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV, in $p_\mathrm{T,ch jet}$ bins [10,20], [20,30], [30,50] and [50,100] GeV/$c$.

$I_\mathrm{AA} (\Delta\varphi)$ distributions measured for $R=$ 0.4 in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV, in $p_\mathrm{T,ch jet}$ bins [10,20], [20,30], [30,50] and [50,100] GeV/$c$.

$I_\mathrm{AA} (\Delta\varphi)$ distributions measured for $R=$ 0.5 in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV, in $p_\mathrm{T,ch jet}$ bins [10,20], [20,30], [30,50] and [50,100] GeV/$c$.

$\Delta_\mathrm{recoil} (p_\mathrm{T,ch jet})$ ratios $R=$ 0.2 / 0.4 in pp and Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV.

$\Delta_\mathrm{recoil} (p_\mathrm{T,ch jet})$ ratios $R=$ 0.2 / 0.5 in pp and Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV.

$\Delta_\mathrm{recoil} (p_\mathrm{T,ch jet})$ ratios $R=$ 0.4 / 0.5 in pp and Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV.

$\Delta_\mathrm{recoil} (p_\mathrm{T,ch jet})$ for $R=$ 0.2, for various $\mathrm{TT_{sig}}$ selections in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV.

$\Delta_\mathrm{recoil} (p_\mathrm{T,ch jet})$ for $R=$ 0.4, for various $\mathrm{TT_{sig}}$ selections in Pb--Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV.

Non-prompt J/$\psi$ fraction as a function of average number of participants in Pb-Pb at 5.02 TeV

Non-prompt J/$\psi$ yields as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 0-10%

Prompt J/$\psi$ yields as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 0-10%

Prompt J/$\psi$ nuclear modification factor as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 0-10%. Global uncertainty 2.3%

Prompt J/$\psi$ nuclear modification factor as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 10-30%. Global uncertainty 2.3%

Prompt J/$\psi$ nuclear modification factor as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 30-50%. Global uncertainty 2.7%

Prompt J/$\psi$ nuclear modification factor as a function of average number of participants in Pb-Pb at 5.02 TeV. Global uncertainty 2.2%

Non-prompt J/$\psi$ nuclear modification factor as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 0-10%. Global uncertainty 2.3%

Non-prompt J/$\psi$ nuclear modification factor as a function of transverse momentum in Pb-Pb at 5.02 TeV,, centrality 10-30%. Global uncertainty 2.3%

Non-prompt J/$\psi$ nuclear modification factor as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 30-50%. Global uncertainty 2.7%

Non-prompt J/$\psi$ nuclear modification factor as a function of average number of participants in Pb-Pb at 5.02 TeV. Global uncertainty 2.7%

Prompt J/$\psi$ yields as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 30-50%

Non-prompt J/$\psi$ yields as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 30-50%

Fully-corrected $\Delta_{\mathrm{recoil}} (\Delta\phi)$ distributions for $p_{\mathrm{T, jet}}^{\mathrm{ch}} \in (40, 60)$ GeV/$c$ measured in MB and HM-selected events in pp collisions at $\sqrt{s}= 13$ TeV.

Ratio of $\Delta_{\mathrm{recoil}} (p_{\mathrm{T, jet}}^{\mathrm{ch}})$ distributions measured in MB and HM-selected events in pp collisions at $\sqrt{s}= 13$ TeV.

Ratio of $\Delta_{\mathrm{recoil}} (\Delta\phi)$ distributions for jets with $p_{\mathrm{T, jet}}^{\mathrm{ch}} \in (20, 40)$ GeV/$c$ measured in MB and HM-selected events in pp collisions at $\sqrt{s}= 13$ TeV.

Ratio of $\Delta_{\mathrm{recoil}} (\Delta\phi)$ distributions for jets with $p_{\mathrm{T, jet}}^{\mathrm{ch}} \in (40, 60)$ GeV/$c$ measured in MB and HM-selected events in pp collisions at $\sqrt{s}= 13$ TeV.

Distribution of probability per trigger hadron of the number of jets with $p_{\mathrm{T, jet}}^{\mathrm{ch}} > 15$ GeV/$c$ and $|\eta_{\mathrm{jet}}| < 0.5$ recoiling from a high-$p_{\mathrm{T}}$ hadron (TT$\{20, 30\}$) for MB and HM-selected events in pp collisions at $\sqrt{s} = 13$ TeV.

Expected CLs values in the High mA SR, mA vs ma signal grid.

Observed CLs values in the High mA SR, mA vs ma signal grid.

Expected CLs values in the Low mA SR, mA vs ma signal grid.

Observed CLs values in the High mA SR, mA vs ma signal grid.

CLs+b values in the Low mA SR, mA vs tanB signal grid.

CLs+b values in the High mA SR, mA vs ma signal grid.

CLs+b values in the Low mA SR, mA vs ma signal grid.

Cut flow of the 2HDM+a signal points, gluon–gluon fusion production, Low mA SR. tanB = 1, $sin\theta$ = 0.35. The first two entries in the tables are number of raw MC events, third entry is theoretical prediction, and all other lines include the correct weights. Note that during the generation Higgs boson’s branching ratio to taus has been set to 1. An additional factor of 0.0627 is used to account for that, starting from the ‘Initial’ entry.

Cut flow of the 2HDM+a signal points, gluon–gluon fusion production, High mA SR. tanB = 1, $sin\theta$ = 0.35. The first two entries in the tables are number of raw MC events, third entry is theoretical prediction, and all other lines include the correct weights. Note that during the generation Higgs boson’s branching ratio to taus has been set to 1. An additional factor of 0.0627 is used to account for that, starting from the ‘Initial’ entry.

Cut flow of the 2HDM+a signal points, bb annihilation production, Low mA SR. tanB = 1, $sin\theta$ = 0.35. The first two entries in the tables are number of raw MC events, third entry is theoretical prediction, and all other lines include the correct weights. Note that during the generation Higgs boson’s branching ratio to taus has been set to 1. An additional factor of 0.0627 is used to account for that, starting from the ‘Initial’ entry.

Cut flow of the 2HDM+a signal points, bb annihilation production, High mA SR. tanB = 1, $sin\theta$ = 0.35. The first two entries in the tables are number of raw MC events, third entry is theoretical prediction, and all other lines include the correct weights. Note that during the generation Higgs boson’s branching ratio to taus has been set to 1. An additional factor of 0.0627 is used to account for that, starting from the ‘Initial’ entry.

A comparison of the observed and expected yields in the four bins of the Low mA SR.

A comparison of the observed and expected yields in the two bins of the High mA SR.

Expected exclusion contours at 95% CL as a function of mA and ma.

Observed exclusion contours at 95% CL as a function of mA and ma.

Expected +- 1sigma exclusion contours at 95% CL as a function of mA and ma.

Expected exclusion contours at 95% CL as a function of mA and ma.

Observed exclusion contours at 95% CL as a function of mA and ma.

Expected +- 1sigma exclusion contours at 95% CL as a function of mA and ma.

Acceptance, High mA SR, mA vs tanB grid, 400-750 GeV, bb prod

Acceptance, High mA SR, mA vs tanB grid, >750 GeV, bb prod

Acceptance, Low mA SR, mA vs tanB grid, 100-250 GeV, bb prod

Acceptance, Low mA SR, mA vs tanB grid, 250-400 GeV, bb prod

Acceptance, Low mA SR, mA vs tanB grid, 400-550 GeV, bb prod

Acceptance, Low mA SR, mA vs tanB grid, >550 GeV, bb prod

Acceptance, High mA SR, mA vs ma grid, 400-750 GeV, bb prod

Acceptance, High mA SR, mA vs ma grid, >750 GeV, bb prod

Acceptance, Low mA SR, mA vs ma grid, 100-250 GeV, bb prod

Acceptance, Low mA SR, mA vs ma grid, 250-400 GeV, bb prod

Acceptance, Low mA SR, mA vs ma grid, 400-550 GeV, bb prod

Acceptance, Low mA SR, mA vs ma grid, >550 GeV, bb prod

Acceptance, High mA SR, mA vs tanB grid, 400-750 GeV, ggF prod

Acceptance, High mA SR, mA vs tanB grid, >750 GeV, ggF prod

Acceptance, Low mA SR, mA vs tanB grid, 100-250 GeV, ggF prod

Acceptance, Low mA SR, mA vs tanB grid, 250-400 GeV, ggF prod

Acceptance, Low mA SR, mA vs tanB grid, 400-550 GeV, ggF prod

Acceptance, Low mA SR, mA vs tanB grid, >550 GeV, ggF prod

Acceptance, High mA SR, mA vs ma grid, 400-750 GeV, ggF prod

Acceptance, High mA SR, mA vs ma grid, >750 GeV, ggF prod

Acceptance, Low mA SR, mA vs ma grid, 100-250 GeV, ggF prod

Acceptance, Low mA SR, mA vs ma grid, 250-400 GeV, ggF prod

Acceptance, Low mA SR, mA vs ma grid, 400-550 GeV, ggF prod

Acceptance, Low mA SR, mA vs ma grid, >550 GeV, ggF prod

Efficiency, High mA SR, mA vs tanB grid, 400-750 GeV, bb prod

Efficiency, High mA SR, mA vs tanB grid, >750 GeV, bb prod

Efficiency, Low mA SR, mA vs tanB grid, 100-250 GeV, bb prod

Efficiency, Low mA SR, mA vs tanB grid, 250-400 GeV, bb prod

Efficiency, Low mA SR, mA vs tanB grid, 400-550 GeV, bb prod

Efficiency, Low mA SR, mA vs tanB grid, >550 GeV, bb prod

Efficiency, High mA SR, mA vs ma grid, 400-750 GeV, bb prod

Efficiency, High mA SR, mA vs ma grid, >750 GeV, bb prod

Efficiency, Low mA SR, mA vs ma grid, 100-250 GeV, bb prod

Efficiency, Low mA SR, mA vs ma grid, 250-400 GeV, bb prod

Efficiency, Low mA SR, mA vs ma grid, 400-550 GeV, bb prod

Efficiency, Low mA SR, mA vs ma grid, >550 GeV, bb prod

Efficiency, High mA SR, mA vs tanB grid, 400-750 GeV, ggF prod

Efficiency, High mA SR, mA vs tanB grid, >750 GeV, ggF prod

Efficiency, Low mA SR, mA vs tanB grid, 100-250 GeV, ggF prod

Efficiency, Low mA SR, mA vs tanB grid, 250-400 GeV, ggF prod

Efficiency, Low mA SR, mA vs tanB grid, 400-550 GeV, ggF prod

Efficiency, Low mA SR, mA vs tanB grid, >550 GeV, ggF prod

Efficiency, High mA SR, mA vs ma grid, 400-750 GeV, ggF prod

Efficiency, High mA SR, mA vs ma grid, >750 GeV, ggF prod

Efficiency, Low mA SR, mA vs ma grid, 100-250 GeV, ggF prod

Efficiency, Low mA SR, mA vs ma grid, 250-400 GeV, ggF prod

Efficiency, Low mA SR, mA vs ma grid, 400-550 GeV, ggF prod

Efficiency, Low mA SR, mA vs ma grid, >550 GeV, ggF prod

Inclusive $e^+e^-$ cross section in p-Pb collisions at $\sqrt{s}$ = 5.02 TeV as a function of $p_{\rm T,ee}$ for $0.5 < m_{\rm ee} < 1.1$ GeV/$c$. Electrons are measured within $|\eta_{\rm e}| < 0.8$ and $p_{\rm T,e} > 0.2$ GeV/$c$.

Inclusive $e^+e^-$ cross section in pp collisions at $\sqrt{s}$ = 5.02 TeV as a function of $p_{\rm T,ee}$ for $1.1 < m_{\rm ee} < 2.7$ GeV/$c$. Electrons are measured within $|\eta_{\rm e}| < 0.8$ and $p_{\rm T,e} > 0.2$ GeV/$c$.

Inclusive $e^+e^-$ cross section in p-Pb collisions at $\sqrt{s}$ = 5.02 TeV as a function of $p_{\rm T,ee}$ for $1.1 < m_{\rm ee} < 2.7$ GeV/$c$. Electrons are measured within $|\eta_{\rm e}| < 0.8$ and $p_{\rm T,e} > 0.2$ GeV/$c$.

Dielectron nuclear modification factor $R_{\rm pPb}$ at $\sqrt{s}$ = 5.02 TeV as a function of $m_{\rm ee}$. Electrons are measured within $|\eta_{\rm e}| < 0.8$ and $p_{\rm T,e} > 0.2$ GeV/$c$.

Dielectron nuclear modification factor $R_{\rm pPb}$ at $\sqrt{s}$ = 5.02 TeV as a function of $p_{\rm T,ee}$ for $0.5 < m_{\rm ee} < 1.1$ GeV/$c$. Electrons are measured within $|\eta_{\rm e}| < 0.8$ and $p_{\rm T,e} > 0.2$ GeV/$c$.

Dielectron nuclear modification factor $R_{\rm pPb}$ at $\sqrt{s}$ = 5.02 TeV as a function of $p_{\rm T,ee}$ for $1.1 < m_{\rm ee} < 2.7$ GeV/$c$. Electrons are measured within $|\eta_{\rm e}| < 0.8$ and $p_{\rm T,e} > 0.2$ GeV/$c$.