Observed and expected multivariate discriminant distribution in the $\ell\ell\ell\ell jj$ SR.

Observed and expected multivariate discriminant distribution in the $\ell\ell\nu\nu jj$ SR.

Correlation matrix between the fiducial cross sections for the four individual decay final states and the $ZZ^{*}$ normalisation factor.

Differential fiducial cross section for the transverse momentum $p_{T}^{4l}$ of the Higgs boson. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 . Measured value in the last bin is un upper limit at 95% CL.

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the transverse momentum $p_{T}^{4l}$ of the Higgs boson.

Differential fiducial cross section for the invariant mass $m_{12}$ of the leading Z boson. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the invariant mass $m_{12}$ of the leading Z boson.

Differential fiducial cross section for the invariant mass $m_{34}$ of the subleading Z boson. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the invariant mass $m_{34}$ of the subleading Z boson.

Differential fiducial cross section for the rapidity $|y_{4l}|$ of the Higgs boson. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the rapidity $|y_{4l}|$ of the Higgs boson.

Differential fiducial cross section for the production angle $|\cos\theta^{*}|$ of the leading Z boson. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the production angle $|\cos\theta^{*}|$ of the leading Z boson.

Differential fiducial cross section for the production angle $\cos\theta_{1}$ of the anti-lepton from the leading Z boson. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the production angle $\cos\theta_{1}$ of the anti-lepton from the leading Z boson.

Differential fiducial cross section for the production angle $\cos\theta_{2}$ of the anti-lepton from the subleading Z boson. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the production angle $\cos\theta_{2}$ of the anti-lepton from the subleading Z boson.

Differential fiducial cross section for the azimuthal angle $\phi$ of the decay planes of the two reconstructed Z bosons. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the azimuthal angle $\phi$ of the decay planes of the two reconstructed Z bosons.

Differential fiducial cross section for the azimuthal angle $\phi_{1}$ of the decay plane of the leading Z boson and the plane formed between its four-momentum and the z-axis. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the azimuthal angle $\phi_{1}$ of the decay plane of the leading Z boson and the plane formed between its four-momentum and the z-axis.

Differential fiducial cross section for the jet multiplicity $N_{jets}$. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the jet multiplicity $N_{jets}$.

Differential fiducial cross section for the inclusive jet multiplicity $N_{jets}$. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Differential fiducial cross section for the number of b-quark initiated jets $N_{b-jets}$. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the number of b-quark initiated jets $N_{b-jets}$.

Differential fiducial cross section for the transverse momentum of the leading jet $p_{T}^{lead.jet}$ in events with at least one jet. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the transverse momentum of the leading jet $p_{T}^{lead.jet}$ in events with at least one jet.

Differential fiducial cross section for the transverse momentum of the subleading jet $p_{T}^{sublead.jet}$ in events with at least two jets. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the transverse momentum of the subleading jet $p_{T}^{sublead.jet}$ in events with at least two jets.

Differential fiducial cross section for the invariant mass of the two highest-pT jets $m_{jj}$ in events with at least two jets. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the invariant mass of the two highest-pT jets $m_{jj}$ in events with at least two jets.

Differential fiducial cross section for the distance between the two highest-pT jets in pseudorapidity $\Delta\eta_{jj}$. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the distance between the two highest-pT jets in pseudorapidity $\Delta\eta_{jj}$.

Differential fiducial cross section for the distance between the two highest-pT jets in $\phi$ $\Delta\phi_{jj}$. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the distance between the two highest-pT jets in $\phi$ $\Delta\phi_{jj}$.

Differential fiducial cross section for the transverse momentum of the four lepton plus jet system, in events with at least one jet $p_{T}^{4lj}$. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the transverse momentum of the four lepton plus jet system, in events with at least one jet $p_{T}^{4lj}$.

Differential fiducial cross section for the transverse momentum of the four lepton plus di-jet system, in events with at least two jets $p_{T}^{4ljj}$. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 . Measured value in the last bin is un upper limit at 95% CL.

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the transverse momentum of the four lepton plus di-jet system, in events with at least two jets $p_{T}^{4ljj}$.

Differential fiducial cross section for the invariant mass of the four lepton plus jet system in events with at least one jet $m_{4lj}$. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the invariant mass of the four lepton plus jet system in events with at least one jet $m_{4lj}$.

Differential fiducial cross section for the invariant mass of the four lepton plus di-jet system in events with at least two jets $m_{4ljj}$. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the invariant mass of the four lepton plus di-jet system in events with at least two jets $m_{4ljj}$.

Differential fiducial cross section for the leading vs. subleading Z boson mass $m_{12}$vs.$m_{34}$. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the leading vs. subleading Z boson mass $m_{12}$vs.$m_{34}$.

Differential fiducial cross section for the leading vs. subleading Z boson mass $m_{12}$vs.$m_{34}$ in $ll\mu\mu$ final states. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Differential fiducial cross section for the leading vs. subleading Z boson mass $m_{12}$vs.$m_{34}$ in $llee$ final states. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the leading vs. subleading Z boson mass m12 vs. m34 in $ll\mu\mu$ and $llee$ final states.

Differential fiducial cross section of the $p_{T}^{4l}$ distribution in $|y_{4l}|$ bins. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section of the $p_{T}^{4l}$ distribution in $|y_{4l}|$ bins.

Differential fiducial cross section of the $p_{T}^{4l}$ distribution in $N_{jets}$ bins. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section of the $p_{T}^{4l}$ distribution in $N_{jets}$ bins.

Differential fiducial cross section for transverse momentum of the four lepton system vs. the transverse momentum of the four lepton plus jet system $p_{T}^{4l}$vs.$p_{T}^{4lj}$. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for transverse momentum of the four lepton system vs. the transverse momentum of the four lepton plus jet system $p_{T}^{4l}$vs.$p_{T}^{4lj}$.

Differential fiducial cross section for the transverse momentum of the four lepton plus jet system vs the invariant mass of the four lepton plus jet system $p_{T}^{4l}$vs.$m_{4lj}$. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the transverse momentum of the four lepton plus jet system vs the invariant mass of the four lepton plus jet system $p_{T}^{4l}$vs.$m_{4lj}$.

Differential fiducial cross section for the transverse momentum of the four lepton vs the transverse momentum of the leading jet $p_{T}^{4l}$vs.$p_{T}^{l.jet}$. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the transverse momentum of the four lepton vs the transverse momentum of the leading jet $p_{T}^{4l}$vs.$p_{T}^{lead.jet}$.

Differential fiducial cross section for the transverse momentum of the leading jet vs the rapidity of the leading jet $p_{T}^{lead.jet}$vs.$|y^{lead.jet}|$. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the transverse momentum of the leading jet vs the rapidity of the leading jet $p_{T}^{lead.jet}$vs.$|y^{lead.jet}|$.

Differential fiducial cross section for the transverse momentum of the leading jet vs the transverse momentum of the subleading jet $p_{T}^{lead.jet}$vs.$p_{T}^{sublead.jet}$. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the transverse momentum of the leading jet vs the transverse momentum of the subleading jet $p_{T}^{lead.jet}$vs.$p_{T}^{sublead.jet}$.

Differential fiducial cross section for the leading Z boson mass $m_{12}$ in $4\mu$ and $4e$ final states. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Differential fiducial cross section for the leading Z boson mass $m_{12}$ in $2e2\mu$ and $2\mu2e$ final states. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the leading Z boson mass $m_{12}$ in $4l$ and $2l2l$ final states.

Differential fiducial cross section for the subleading Z boson mass $m_{34}$ in $4\mu$ and $4e$ final states. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Differential fiducial cross section for the subleading Z boson mass $m_{34}$ in $2e2\mu$ and $2\mu2e$ final states. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the subleading Z boson mass $m_{34}$ in $4l$ and $2l2l$ final states.

Differential fiducial cross section for the azimuthal angle $\phi$ of the decay planes of the two reconstructed Z bosons in $4\mu$ and $4e$ final states. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Differential fiducial cross section for the azimuthal angle $\phi$ of the decay planes of the two reconstructed Z bosons in $2e2\mu$ and $2\mu2e$ final states. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the azimuthal angle $\phi$ of the decay planes of the two reconstructed Z bosons in $4l$ and $2l2l$ final states.

Differential fiducial cross section for the leading vs. subleading Z boson mass $m_{12}$vs.$m_{34}$ in $4\mu$ and $4e$ final states. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Differential fiducial cross section for the leading vs. subleading Z boson mass $m_{12}$vs.$m_{34}$ in $2\mu2e$ and $2e2\mu$ final states. The measured cross sections are compared to predictions provided by NNLOPS + XH. NNLOPS is normalised to the N3LO total cross section with a K-factor = 1.1 .

Correlation matrix between the measured cross sections and the $ZZ^{*}$ background normalization corresponding to the differential fiducial cross section for the leading vs. subleading Z boson mass $m_{12}$vs.$m_{34}$ in $4l$ and $2l2l$ final states.

The expected (pre-fit) and observed numbers of events for an integrated luminosity of 139 fb$^{-1}$ at $\sqrt{s}$=13 TeV in the signal region 115 < $m_{4l}$< 130 GeV and sideband region $m_{4l}$ in 105-115 GeV or 130-160 GeV (350 GeV for $tXX$-enriched) in each reconstructed event category assuming the SM Higgs boson signal with a mass $m_{H}$= 125 GeV. Combined statistical and systematic uncertainties are included for the predictions. Expected contributions that are below 0.2% of the total yield in each reconstructed event category are not shown and replaced by -.

The expected and the observed (post-fit) the jet multiplicity distribution after the inclusive event selection for an integrated luminosity of 139fb$^{-1}$ at $\sqrt{s}$=13TeV. The SM Higgs boson signal is assumed to have a mass $m_{H}$=125 GeV.

The expected and the observed (post-fit) the four-lepton transverse momentum distribution for events with zero jets, after the inclusive event selection for an integrated luminosity of 139fb$^{-1}$ at $\sqrt{s}$=13TeV. The SM Higgs boson signal is assumed to have a mass $m_{H}$=125 GeV.

The expected and the observed (post-fit) the four-lepton transverse momentum distribution for events with one jet, after the inclusive event selection for an integrated luminosity of 139fb$^{-1}$ at $\sqrt{s}$=13TeV. The SM Higgs boson signal is assumed to have a mass $m_{H}$=125 GeV.

The expected and the observed (post-fit) the four-lepton transverse momentum distribution for events with at least two jets, after the inclusive event selection for an integrated luminosity of 139fb$^{-1}$ at $\sqrt{s}$=13TeV. The SM Higgs boson signal is assumed to have a mass $m_{H}$=125 GeV.

The expected and the observed (post-fit) the dijet invariant mass distribution for events with at least two jets, after the inclusive event selection for an integrated luminosity of 139fb$^{-1}$ at $\sqrt{s}$=13TeV. The SM Higgs boson signal is assumed to have a mass $m_{H}$=125 GeV.

The expected and the observed $NN_{ggF}$ output (post-fit) distribution in 0$j$-$p_{T}^{4l}$-Low category for an integrated luminosity of 139fb$^{-1}$ at $\sqrt{s}$=13TeV. The SM Higgs boson signal is assumed to have a mass $m_{H}$=125 GeV.

The expected and the observed $NN_{ggF}$ output (post-fit) distribution in 0$j$-$p_{T}^{4l}$-Med category for an integrated luminosity of 139fb$^{-1}$ at $\sqrt{s}$=13TeV. The SM Higgs boson signal is assumed to have a mass $m_{H}$=125 GeV.

The expected and the observed $NN_{VBF}$ output (post-fit) distribution in 1$j$-$p_{T}^{4l}$-Low category with $NN_{ZZ}$<0.25 for an integrated luminosity of 139fb$^{-1}$ at $\sqrt{s}$=13TeV. The SM Higgs boson signal is assumed to have a mass $m_{H}$=125 GeV.

The expected and the observed $NN_{ZZ}$ output (post-fit) distribution in 1$j$-$p_{T}^{4l}$-Low category with $NN_{ZZ}$>0.25 for an integrated luminosity of 139fb$^{-1}$ at $\sqrt{s}$=13TeV. The SM Higgs boson signal is assumed to have a mass $m_{H}$=125 GeV.

The expected and the observed $NN_{VBF}$ output (post-fit) distribution in 1$j$-$p_{T}^{4l}$-Med category with $NN_{ZZ}$<0.25 for an integrated luminosity of 139fb$^{-1}$ at $\sqrt{s}$=13TeV. The SM Higgs boson signal is assumed to have a mass $m_{H}$=125 GeV.

The expected and the observed $NN_{ZZ}$ output (post-fit) distribution in 1$j$-$p_{T}^{4l}$-Med category with $NN_{ZZ}$>0.25 for an integrated luminosity of 139fb$^{-1}$ at $\sqrt{s}$=13TeV. The SM Higgs boson signal is assumed to have a mass $m_{H}$=125 GeV.

The expected and the observed $NN_{VBF}$ output (post-fit) distribution in 1$j$-$p_{T}^{4l}$-High category for an integrated luminosity of 139fb$^{-1}$ at $\sqrt{s}$=13TeV. The SM Higgs boson signal is assumed to have a mass $m_{H}$=125 GeV.

The expected and the observed $NN_{VBF}$ output (post-fit) distribution in 2$j$ category with $NN_{VH}$<0.2 for an integrated luminosity of 139fb$^{-1}$ at $\sqrt{s}$=13TeV. The SM Higgs boson signal is assumed to have a mass $m_{H}$=125 GeV.

The expected and the observed $NN_{VH}$ output (post-fit) distribution in 2$j$ category with $NN_{VH}$>0.2 for an integrated luminosity of 139fb$^{-1}$ at $\sqrt{s}$=13TeV. The SM Higgs boson signal is assumed to have a mass $m_{H}$=125 GeV.

The expected and the observed $NN_{VBF}$ output (post-fit) distribution in 2$j$-BSM-like category for an integrated luminosity of 139fb$^{-1}$ at $\sqrt{s}$=13TeV. The SM Higgs boson signal is assumed to have a mass $m_{H}$=125 GeV.

The expected and the observed $NN_{ttH}$ output (post-fit) distribution in $ttH$-Had-enriched category with $NN_{tXX}$<0.4 for an integrated luminosity of 139fb$^{-1}$ at $\sqrt{s}$=13TeV. The SM Higgs boson signal is assumed to have a mass $m_{H}$=125 GeV.

The expected and the observed $NN_{tXX}$ output (post-fit) distribution in $ttH$-Had-enriched category with $NN_{tXX}$>0.4 for an integrated luminosity of 139fb$^{-1}$ at $\sqrt{s}$=13TeV. The SM Higgs boson signal is assumed to have a mass $m_{H}$=125 GeV.

The expected and the observed $NN_{ttH}$ output (post-fit) distribution in $VH$-Lep-enriched category for an integrated luminosity of 139fb$^{-1}$ at $\sqrt{s}$=13TeV. The SM Higgs boson signal is assumed to have a mass $m_{H}$=125 GeV.

The expected and the observed events in the categories where no NN discriminant is used for an integrated luminosity of 139fb$^{-1}$ at $\sqrt{s}$=13TeV. The SM Higgs boson signal is assumed to have a mass $m_{H}$=125 GeV.

The expected and the observed events in the side bands used to constraint the $ZZ^{*}$ and $tXX$ backgrounds for an integrated luminosity of 139fb$^{-1}$ at $\sqrt{s}$=13TeV. The SM Higgs boson signal is assumed to have a mass $m_{H}$=125 GeV.

The expected SM cross section $(\sigma \cdot BR)_{SM}$, the observed value of $(\sigma \cdot BR)$, and their ratio $(\sigma \cdot BR)/(\sigma \cdot BR)_{SM}$ for the inclusive production and for each Production Mode and Reduced Stage-1.1 production bin for an integrated luminosity of 139fb$^{-1}$ at $\sqrt{s}$=13 TeV.

The correlation matrices between the measured cross-sections and the $ZZ$ and $tXX$ normalisation factors for Production Mode Stage.

The correlation matrices between the measured cross-sections and the $ZZ$ and $tXX$ normalisation factors for Reduced Stage 1.1.

Likelihood contours at 68% CLs in the (ggF,VBF) plane. The observed best fit value is the first value of the table.

Likelihood contours at 95% CLs in the (ggF,VBF) plane. The observed best fit value is the first value of the table.

Likelihood contours at 68% CLs in the (ggF,VH) plane. The observed best fit value is the first value of the table.

Likelihood contours at 95% CLs in the (ggF,VH) plane. The observed best fit value is the first value of the table.

Likelihood contours at 68% CLs in the (VBF,VH) plane. The observed best fit value is the first value of the table.

Likelihood contours at 95% CLs in the (VBF,VH) plane. The observed best fit value is the first value of the table.

Likelihood contours at 68% CLs in the ($gg2H-0j-p_T^H-Low$,$gg2H-0j-p_T^H-High$) plane. The observed best fit value is the first value of the table.

Likelihood contours at 95% CLs in the ($gg2H-0j-p_T^H-Low$,$gg2H-0j-p_T^H-High$) plane. The observed best fit value is the first value of the table.

Likelihood contours at 68% CLs in the ($\kappa_{V}$vs.$\kappa_{F}$) plane. The observed best fit value is the first value of the table.

Likelihood contours at 95% CLs in the ($\kappa_{V}$vs.$\kappa_{F}$) plane. The observed best fit value is the first value of the table.

The expected signal yield ratio for chosen CP-even and CP-odd EFT parameter values together with the corresponding cross-section measurement in each production bin of Reduced Stage 1.1. The parameter values correspond approximately to the expected confidence intervals at the 68% CLs obtained from the statistical interpretation of data.

The expected and observed confidence intervals at 68% and 95% CLs of the SMEFT Wilson coefficients for an integrated luminosity of 139fb$^{-1}$ at $\sqrt{s}$=13 TeV. For the coupling with two best fit values, the two values have been splitted in the two different columns 'Two Best-fit value - first' and 'Two Best-fit value - second', and the symbol '-' has been inserted in the missing fields.

Expected 2D-fit likelihood curves at the 95% CLs for the $c_{HW}$ versus $c_{HB}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

Observed 2D-fit likelihood curves at the 95% CLs for the $c_{HW}$ versus $c_{HB}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

Expected 2D-fit likelihood curves at the 95% CLs for the $c_{HB}$ versus $c_{HG}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

Observed 2D-fit likelihood curves at the 95% CLs for the $c_{HB}$ versus $c_{HG}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

Expected 2D-fit likelihood curves at the 95% CLs for the $c_{uH}$ versus $c_{HG}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

Observed 2D-fit likelihood curves at the 95% CLs for the $c_{uH}$ versus $c_{HG}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

The best-fit values and the corresponding deviation from the SM prediction obtained from two-dimensional likelihood scans of the CP-odd BSM coupling parameters with 139fb$^{-1}$ data at $\sqrt{s}$=13 TeV. For the coupling with two best fit values, the two values have been splitted in the two different columns 'Two Observed best-fit first/second_POI - first' and 'Two Observed best-fit first/second_POI - second', and the symbol '-' has been inserted in the missing fields.

Expected 2D-fit likelihood curves at the 95% CLs for the $c_{H\tilde{W}}$ versus $c_{H\tilde{B}}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

Observed 2D-fit likelihood curves at the 95% CLs for the $c_{H\tilde{W}}$ versus $c_{H\tilde{B}}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

Expected 2D-fit likelihood curves at the 95% CLs for the $c_{H\tilde{B}}$ versus $c_{H\tilde{G}}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

Observed 2D-fit likelihood curves at the 95% CLs for the $c_{H\tilde{B}}$ versus $c_{H\tilde{G}}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

Expected 2D-fit likelihood curves at the 95% CLs for the $c_{\tilde{u}H}$ versus $c_{H\tilde{G}}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

Observed 2D-fit likelihood curves at the 95% CLs for the $c_{\tilde{u}H}$ versus $c_{H\tilde{G}}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

Signal acceptance times efficiency, expressed as a percentage, obtained from the ratio of the number of simulated signal events satisfying the event selection criteria in each reconstructed category to the total number of events generated in the phase space specified by a given Production model bin.

Signal acceptance times efficiency, expressed as a percentage, obtained from the ratio of the number of simulated signal events satisfying the event selection criteria in each reconstructed category to the total number of events generated in the phase space specified by a given Reduced Stage-1.1 production bin.

Observed covariance matrix for the different parameters of interest when fitting the for Production Mode Stage.

Observed covariance matrix for the different parameters of interest when fitting the for Reduced Stage 1.1.

The expected SM cross section $(\sigma\cdot BR)_{SM}$, the observed value of $(\sigma\cdot BR)$, and their ratio $(\sigma\cdot BR)/(\sigma\cdot BR)_{SM}$ for the alternate Reduced Stage-1.1 scheme for an integrated luminosity of 139fb$^{-1}$ at $\sqrt{s}$=13 TeV.

The correlation matrices between the measured cross-sections and the ZZ and $tXX$ normalisation factors for alternative Reduced Stage 1.1.

Expected 2D-fit likelihood curves at the 95% CLs for the $c_{HW}$ versus $c_{HWB}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

Observed 2D-fit likelihood curves at the 95% CLs for the $c_{HW}$ versus $c_{HWB}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

Expected 2D-fit likelihood curves at the 95% CLs for the $c_{HB}$ versus $c_{HWB}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

Observed 2D-fit likelihood curves at the 95% CLs for the $c_{HB}$ versus $c_{HWB}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

Expected 2D-fit likelihood curves at the 95% CLs for the $c_{HW}$ versus $c_{HG}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

Observed 2D-fit likelihood curves at the 95% CLs for the $c_{HW}$ versus $c_{HG}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

Expected 2D-fit likelihood curves at the 95% CLs for the $c_{HWB}$ versus $c_{HG}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

Observed 2D-fit likelihood curves at the 95% CLs for the $c_{HWB}$ versus $c_{HG}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

Expected 2D-fit likelihood curves at the 95% CLs for the $c_{H\tilde{W}}$ versus $c_{H\tilde{W}B}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

Observed 2D-fit likelihood curves at the 95% CLs for the $c_{H\tilde{W}}$ versus $c_{H\tilde{W}B}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

Expected 2D-fit likelihood curves at the 95% CLs for the $c_{H\tilde{B}}$ versus $c_{H\tilde{W}B}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

Observed 2D-fit likelihood curves at the 95% CLs for the $c_{H\tilde{B}}$ versus $c_{H\tilde{W}B}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

Expected 2D-fit likelihood curves at the 95% CLs for the $c_{H\tilde{W}}$ versus $c_{H\tilde{G}}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

Observed 2D-fit likelihood curves at the 95% CLs for the $c_{H\tilde{W}}$ versus $c_{H\tilde{G}}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

Expected 2D-fit likelihood curves at the 95% CLs for the $c_{H\tilde{W}B}$ versus $c_{H\tilde{G}}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

Observed 2D-fit likelihood curves at the 95% CLs for the $c_{H\tilde{W}B}$ versus $c_{H\tilde{G}}$ coupling parameters at an integrated luminosity of 139 fb$^{-1}$ and $\sqrt{s}$=13 TeV. Except for the two fitted Wilson coefficients, all others are set to zero.

Expected and observed 95% CL upper limits on $\sigma(pp\to H)B(H\to Z(\eta_c~\text{or}~J/\psi))/$pb. The smaller (larger) quoted ranges around the expected limits represent $\pm 1\sigma$ ($\pm 2\sigma$) fluctuations.

The 95% CL upper limits of the cross section times branching fraction of $\Phi \to \mu^+\mu^-$ for b-associated production

The observed/expected 95% CL upper limits of the cross section times branching fraction of $\Phi \to \mu^+\mu^-$ as a function of $\Phi$ mass and the cross section fraction of the b-associated production.

Signal acceptance for different masses in bTag and bVeto signal regions.

Expected and observed 95% CL lower limits on the mass of a vector-like $T$ quark in the branching-ratio plane.

Expected and observed 95% CL lower limits on the mass of a vector-like $B$ quark in the branching-ratio plane.

Expected and observed upper limits at the 95% CL on the $T\bar T$ cross section as a function of $T$ mass under the assumption BR($T\to Wb$)=1.

Expected and observed upper limits at the 95% CL on the $B\bar B$ cross section as a function of $B$ mass under the assumption BR($T\to Zt$)=1.

Expected and observed upper limits at the 95% CL on the $B\bar B$ cross section as a function of $B$ mass under the assumption BR($B\to Wt$)=1.

Expected and observed upper limits at the 95% CL on the $B\bar B$ cross section as a function of $B$ mass under the assumption BR($B\to Zb$)=1.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-W/Z signal region with the merged event topology after the profile-likelihood fit. This is shown for the 0b-tagged jet, low purity, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-W/Z signal region with the merged event topology after the profile-likelihood fit. This is shown for the 1b-tagged jet, high purity, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-W/Z signal region with the merged event topology after the profile-likelihood fit. This is shown for the 1b-tagged jet, low purity, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-W/Z signal region with the merged event topology after the profile-likelihood fit. This is shown for the 2b-tagged jet event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-W/Z signal region with the resolved event topology after the profile-likelihood fit. This is shown for the 0b-tagged jet event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-W/Z signal region with the resolved event topology after the profile-likelihood fit. This is shown for the 1b-tagged jet event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-W/Z signal region with the resolved event topology after the profile-likelihood fit. This is shown for the 2b-tagged jet event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the merged event topology for a Z' mass of 90 GeV after the profile-likelihood fit. This is shown for the 0b-tagged jet, high purity, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the merged event topology for a Z' mass of 90 GeV after the profile-likelihood fit. This is shown for the 0b-tagged jet, low purity, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the merged event topology for a Z' mass of 90 GeV after the profile-likelihood fit. This is shown for the 1b-tagged jet, high purity, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the merged event topology for a Z' mass of 90 GeV after the profile-likelihood fit. This is shown for the 1b-tagged jet, low purity, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the merged event topology for a Z' mass of 90 GeV after the profile-likelihood fit. This is shown for the 2b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 90 GeV after the profile-likelihood fit. This is shown for the 0b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 350 GeV after the profile-likelihood fit. This is shown for the 0b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 90 GeV after the profile-likelihood fit. This is shown for the 1b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 350 GeV after the profile-likelihood fit. This is shown for the 1b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 90 GeV after the profile-likelihood fit. This is shown for the 2b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 350 GeV after the profile-likelihood fit. This is shown for the 2b-tagged jet, event category.

Expected exclusion contours at 95% C.L. of the dark matter mediator particles (m_chi, m_Zp) for the combined mono-W and mono-Z search in the frame of the simplified model with the Dirac DM particles and couplings g_SM = 0.25 and g_DM = 1.

Observed exclusion contours at 95% C.L. of the dark matter mediator particles (m_chi, m_Zp) for the combined mono-W and mono-Z search in the frame of the simplified model with the Dirac DM particles and couplings g_SM = 0.25 and g_DM = 1.

Exclusion contours at 95% C.L. of the cross section as a function of Z' mass (mZp), for the mono-Z' dark fermion model, with the light dark sector scenario, with parameters g_SM = 0.1 and g_DM = 1.

Exclusion contours at 95% C.L. of the cross section as a function of Z' mass (mZp), for the mono-Z' dark fermion model, with the heavy dark sector scenario, with parameters g_SM = 0.1 and g_DM = 1.

Exclusion contours at 95% C.L. of the cross section as a function of Z' mass (mZp), for the mono-Z' dark Higgs model, with the light dark sector scenario, with parameters g_SM = 0.1 and g_DM = 1.

Exclusion contours at 95% C.L. of the cross section as a function of Z' mass (mZp), for the mono-Z' dark Higgs model, with the heavy dark sector scenario, with parameters g_SM = 0.1 and g_DM = 1.

Exclusion contours at 95% C.L. of the product of the couplings g_SM g_DM as a function of Z' mass (mZp), for the mono-Z' dark fermion model, with the light dark sector scenario, with parameter g_DM = 1.

Exclusion contours at 95% C.L. of the product of the couplings g_SM g_DM as a function of Z' mass (mZp), for the mono-Z' dark fermion model, with the heavy dark sector scenario, with parameter g_DM = 1.

Exclusion contours at 95% C.L. of the product of the couplings g_SM g_DM as a function of Z' mass (mZp), for the mono-Z' dark Higgs model, with the light dark sector scenario, with parameter g_DM = 1.

Exclusion contours at 95% C.L. of the product of the couplings g_SM g_DM as a function of Z' mass (mZp), for the mono-Z' dark Higgs model, with the heavy dark sector scenario, with parameter g_DM = 1.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the merged event topology for a Z' mass of 80 GeV after the profile-likelihood fit. This is shown for the 0b-tagged jet, low purity, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the merged event topology for a Z' mass of 80 GeV after the profile-likelihood fit. This is shown for the 1b-tagged jet, low purity, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the merged event topology for a Z' mass of 80 GeV after the profile-likelihood fit. This is shown for the 0b-tagged jet, high purity, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the merged event topology for a Z' mass of 80 GeV after the profile-likelihood fit. This is shown for the 1b-tagged jet, high purity, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the merged event topology for a Z' mass of 80 GeV after the profile-likelihood fit. This is shown for the 2b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 80 GeV after the profile-likelihood fit. This is shown for the 0b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 80 GeV after the profile-likelihood fit. This is shown for the 1b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 80 GeV after the profile-likelihood fit. This is shown for the 2b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the merged event topology for a Z' mass of 100 GeV after the profile-likelihood fit. This is shown for the 0b-tagged jet, low purity, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the merged event topology for a Z' mass of 100 GeV after the profile-likelihood fit. This is shown for the 1b-tagged jet, low purity, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the merged event topology for a Z' mass of 100 GeV after the profile-likelihood fit. This is shown for the 0b-tagged jet, high purity, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the merged event topology for a Z' mass of 100 GeV after the profile-likelihood fit. This is shown for the 1b-tagged jet, high purity, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the merged event topology for a Z' mass of 100 GeV after the profile-likelihood fit. This is shown for the 2b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 100 GeV after the profile-likelihood fit. This is shown for the 0b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 100 GeV after the profile-likelihood fit. This is shown for the 1b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 100 GeV after the profile-likelihood fit. This is shown for the 2b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 110 GeV after the profile-likelihood fit. This is shown for the 0b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 110 GeV after the profile-likelihood fit. This is shown for the 1b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 110 GeV after the profile-likelihood fit. This is shown for the 2b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 120 GeV after the profile-likelihood fit. This is shown for the 0b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 120 GeV after the profile-likelihood fit. This is shown for the 1b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 120 GeV after the profile-likelihood fit. This is shown for the 2b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 130 GeV after the profile-likelihood fit. This is shown for the 0b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 130 GeV after the profile-likelihood fit. This is shown for the 1b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 130 GeV after the profile-likelihood fit. This is shown for the 2b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 140 GeV after the profile-likelihood fit. This is shown for the 0b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 140 GeV after the profile-likelihood fit. This is shown for the 1b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 140 GeV after the profile-likelihood fit. This is shown for the 2b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 150 GeV after the profile-likelihood fit. This is shown for the 0b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 150 GeV after the profile-likelihood fit. This is shown for the 1b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 150 GeV after the profile-likelihood fit. This is shown for the 2b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 160 GeV after the profile-likelihood fit. This is shown for the 0b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 160 GeV after the profile-likelihood fit. This is shown for the 1b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 160 GeV after the profile-likelihood fit. This is shown for the 2b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 170 GeV after the profile-likelihood fit. This is shown for the 0b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 170 GeV after the profile-likelihood fit. This is shown for the 1b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 170 GeV after the profile-likelihood fit. This is shown for the 2b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 180 GeV after the profile-likelihood fit. This is shown for the 0b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 180 GeV after the profile-likelihood fit. This is shown for the 1b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 180 GeV after the profile-likelihood fit. This is shown for the 2b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 190 GeV after the profile-likelihood fit. This is shown for the 0b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 190 GeV after the profile-likelihood fit. This is shown for the 1b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 190 GeV after the profile-likelihood fit. This is shown for the 2b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 200 GeV after the profile-likelihood fit. This is shown for the 0b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 200 GeV after the profile-likelihood fit. This is shown for the 1b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 200 GeV after the profile-likelihood fit. This is shown for the 2b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 250 GeV after the profile-likelihood fit. This is shown for the 0b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 250 GeV after the profile-likelihood fit. This is shown for the 1b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 250 GeV after the profile-likelihood fit. This is shown for the 2b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 300 GeV after the profile-likelihood fit. This is shown for the 0b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 300 GeV after the profile-likelihood fit. This is shown for the 1b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 300 GeV after the profile-likelihood fit. This is shown for the 2b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 400 GeV after the profile-likelihood fit. This is shown for the 0b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 400 GeV after the profile-likelihood fit. This is shown for the 1b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 400 GeV after the profile-likelihood fit. This is shown for the 2b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 450 GeV after the profile-likelihood fit. This is shown for the 0b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 450 GeV after the profile-likelihood fit. This is shown for the 1b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 450 GeV after the profile-likelihood fit. This is shown for the 2b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 500 GeV after the profile-likelihood fit. This is shown for the 0b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 500 GeV after the profile-likelihood fit. This is shown for the 1b-tagged jet, event category.

The observed and expected MET distributions with 36.1fb-1 of data with sqrt(s) = 13 TeV in the mono-Z' signal region with the resolved event topology for a Z' mass of 500 GeV after the profile-likelihood fit. This is shown for the 2b-tagged jet, event category.

Number of data events for the 2-tag category with the loose selection in bins of diphoton mass.

Number of data events for the 1-tag category with the tight selection in bins of diphoton mass.

Number of data events for the 2-tag category with the tight selection in bins of diphoton mass.

Number of data events for the 1-tag category with the loose selection in bins of four-body mass.

Number of data events for the 2-tag category with the loose selection in bins of four-body mass.

Number of data events for the 1-tag category with the tight selection in bins of four-body mass.

Number of data events for the 2-tag category with the tight selection in bins of four-body mass.

Expected and observed upper limits at the 95% CL on the cross-section of gluon-fusion initiated Higgs boson pair production as a function of $\kappa_{\lambda}$.

Expected and observed upper limits at the 95% CL on the cross-section of gluon-fusion initiated resonant production of a Higgs boson pair as a function of the mass of the resonance, $m_X$.

Exclusion limits on higgsino pair production divided by the theory cross-section.The results of the low-mass analysis are used below m(higgsino) = 300 GeV, while those of the high-mass analysis are used above. The figure shows the observed and expected 95% upper limits on the higgsino pair production cross-section as a function of m(higgsino).

Observed and expected 95% limits in the m(higgsino) vs BR(higgsino to higgs+gravitino) plane. The regions above the lines are excluded by the analyses.

The observed and expected 95% upper limits on the total pair production cross section for degenerate higgsinos as a function of m(higgsino) for the high-mass search. Only the high-mass analysis results are used in this figure.

The observed and expected 95% upper limits on the total pair production cross section for degenerate higgsinos as a function of m(higgsino) for the high-mass search, divided by the theory cross section. Only the high-mass analysis results are used in this figure.

The observed and expected 95% upper limits on the total pair production cross section for degenerate higgsinos as a function of m(higgsino) for the low-mass search. Only the low-mass analysis results are used in this figure.

The observed and expected 95% upper limits on the total pair production cross section for degenerate higgsinos as a function of m(higgsino) for the low-mass search, divided by the theory cross section. Only the low-mass analysis results are used in this figure.

Particle-level acceptance for the low-mass discovery signal regions low-SR-MET0-meff440 and low-SR-MET150-meff440, shown as a function of higgsino mass. The acceptance is defined as the fraction of signal events passing the particle-level event selection that emulates the detector-level selection. The acceptance calculation considers only those signal events where both higgsinos decay to Higgs bosons that subsequently both decay to b-quarks.

The experimental efficiency of the low-mass analysis, for the two discovery signal regions low-SR-MET0-meff440 and low-SR-MET150-meff440, as a function of higgsino mass. The experimental efficiency is defined as the number of events passing the detector-level event selection divided by the number of events passing the event selection for a perfect detector. The denominator is obtained by implementing particle-level event selection that emulate the detector-level selection. Such particle-level selection is not applied on the numerator.

Particle-level acceptance for the high-mass discovery signal regions SR-4b-meff1-A-disc and SR-3b-meff3-A, shown as a function of higgsino mass. The acceptance is defined as the fraction of signal events passing the particle-level event selection that emulates the detector-level selection. The acceptance calculation considers only those signal events where both higgsinos decay to Higgs bosons that subsequently both decay to b-quarks.

The experimental efficiency of the high-mass analysis, for the two discovery signal regions SR-4b-meff1-A-disc and SR-3b-meff3-A, as a function of higgsino mass. The experimental efficiency is defined as the number of events passing the detector-level event selection divided by the number of events passing the event selection for a perfect detector. The denominator is obtained by implementing particle-level event selection that emulate the detector-level selection. Such particle-level selection is not applied on the numerator.

Example cutflow for SR-3b-meff3-A.

Example cutflow for SR-4b-meff1-A-disc.

Cutflow for low-mass analysis for each signal mass point.

Observed and expected distributions of the $WZ$ invariant mass in the q$\bar{\mathrm q}$ category after applying all selection cuts. Background contributions are obtained from background-only likelihood fit to the data.

Observed and expected distributions of the $WZ$ invariant mass in the $VBF$ category after applying all selection cuts. Background contributions are obtained from background-only likelihood fit to the data.

Observed and expected 95% C.L. upper limits on $\sigma\times$BR($W'\to W^\pm Z$) for the q$\bar{\mathrm q}$ production of a $W'$ boson in the HVT model as a function of its mass. The $\pm1\sigma$ and $\pm2\sigma$ uncertainty in the expected limits are given. Limits are calculated in the asymptotic approximation below 900 GeV and are obtained from pseudo-experiments above that.

Observed and expected 95% C.L. upper limits on $\sigma\times$BR($W'\to W^\pm Z$) for the $VBF$ production of a $W'$ boson in the HVT model as a function of its mass. The $\pm1\sigma$ and $\pm2\sigma$ uncertainty are given in the expected limits. Limits are calculated in the asymptotic approximation below 700 GeV and are obtained from pseudo-experiments above that.

Observed and expected 95% C.L. upper limits on $\sigma\times$BR($H_5^\pm\to W^\pm Z$) of the Georgi-Machacek Model as a function of $m_{H_5^\pm}$. The $\pm1\sigma$ and $\pm2\sigma$ uncertainty in the expected limits are given. Limits are calculated in the asymptotic approximation below 700 GeV and are obtained from pseudo-experiments above that.

Observed and expected 95% C.L. upper limits on the parameter $\sin(\theta_H)$ of the Georgi-Machacek Model as a function of $m_{H_5^\pm}$. The $\pm1\sigma$ and $\pm2\sigma$ uncertainty are given in the expected limits. Limits are calculated in the asymptotic approximation below 700 GeV and are obtained from pseudo-experiments above that.