Data from Table 2. Observed and expected exclusion limits for the aQGC parameters at 95% CL, without any form factors.

Data from Fig.4. Observed yields of four lepton invariant mass distribution. The last bin includes overflow.

Data from Fig.4. Expected yields of four lepton invariant mass distribution for the EW ZZjj signal process. The last bin includes overflow.

Data from Fig.4. Expected yields of four lepton invariant mass distribution for the mixed EW-QCD qqZZjj background. The last bin includes overflow.

Data from Fig.4. Expected yields of four lepton invariant mass distribution for the mixed EW-QCD ggZZjj background. The last bin includes overflow.

Data from Fig.4. Expected yields of four lepton invariant mass distribution for the WWZ background. The last bin includes overflow.

Data from Fig.4. Expected yields of four lepton invariant mass distribution for the ttZ background. The last bin includes overflow.

Data from Fig.4. Expected yields of four lepton invariant mass distribution for the Z+X reducible background. The last bin includes overflow.

Data from Fig. 3 lower right panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 13$ TeV as a function of the jet multiplicity with $|\eta_{j}| < 2.4$.

Data from Fig. 4 upper right panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 13$ TeV as a function of the p$_T$-leading jet transverse momentum with $|\eta_{j}| < 4.7$.

Data from Fig. 5 left panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 13$ TeV as a function of the p$_T$-leading jet transverse momentum with $|\eta_{j}| < 4.7$.

Data from Fig. 4 lower right panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 13$ TeV as a function of the p$_T$-leading jet $|\eta_{j}|$ with $|\eta_{j}| < 4.7$.

Data from Fig. 5 right panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 13$ TeV as a function of the p$_T$-subleading jet $|\eta_{j}|$ with $|\eta_{j}| < 4.7$.

Data from Fig. 6 left panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 13$ TeV as a function of the invariant mass of the two p$_T$ leading jets with $|\eta_{j}| < 4.7$.

Data from Fig. 6 right panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 13$ TeV as a function of the invariant of pseudorapidity separation of the two $p$_T$ leading jets with $|\eta_{j}| < 4.7$.

Data from Fig. 2 upper left. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ differential cross section at $\sqrt{s} = 8$ TeV as a function of the jet multiplicity with $|\eta| < 4.7$.

Data from Fig. 3 upper left panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 8$ TeV as a function of the jet multiplicity with $|\eta| < 4.7$.

Data from Fig. 2 lower left panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ differential cross section at $\sqrt{s} = 8$ TeV as a function of the jet multiplicity with $|\eta| < 2.4$.

Data from Fig. 3 lower left panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 8$ TeV as a function of the jet multiplicity with $|\eta| < 2.4$.

Data from Fig. 4 upper left panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 8$ TeV as a function of the p$_T$-leading jet transverse momentum with $|\eta| < 4.7$.

Data from Fig. 4 lower left panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 8$ TeV as a function of the p$_T$-leading jet transverse $\eta$ with $|\eta| < 4.7$.

The distributions of likelihood discriminant for data, simulated QCD multijet events, and simulated signal events. Data and simulated events are selected with the displaced-jet trigger. The offline $H_{T}$ is required to be larger than 400 GeV, and the jets are required to have $p_{T}>50\ \mathrm{GeV}$ and $|\eta|<2.0$. Three benchmark signal distributions are shown (dashed lines) for the jet-jet model with $m_{X}=300\ \mathrm{GeV}$ and varying lifetimes. For visualization each signal process is given a cross section, $\sigma$, such that $\sigma\ 35.9 \mathrm{fb}^{-1} = 1 \times 10^{6}$.

Numbers of predicted and observed background events for the nominal background method and the three cross-checks in the control region. Shown are the comparisons for likelihood discriminant thresholds of 0.3, 0.4, 0.5, 0.6, 0.7, 0.8, and 0.9. The error bars represent the statistical uncertainties of the predictions and the observations. The data points at different likelihood discriminant thresholds are correlated, since the events passing higher likelihood discriminant thresholds also pass lower likelihood discriminant thresholds.

Numbers of predicted and observed background events for the nominal background method and the three cross-checks in the control region. Shown are the comparisons for likelihood discriminant thresholds of 0.95, 0.96, 0.97, 0.98, 0.99, and 0.9993. The error bars represent the statistical uncertainties of the predictions and the observations. The data points at different likelihood discriminant thresholds are correlated, since the events passing higher likelihood discriminant thresholds also pass lower likelihood discriminant thresholds.

The expected and observed $95\%$ $\text{CL}$ upper limits on the pair production cross section of the long-lived particle X, assuming a $100\%$ branching fraction for X to decay to a quark-antiquark pair, shown at different masses and different proper decay lengths for the jet-jet model.

the expected and observed $95\%$ $\text{CL}$ upper limits on the pair production cross section of the long-lived gluino, assuming a $100\%$ branching fraction for $\widetilde{\mathrm{g}}\to\mathrm{g}\widetilde{\mathrm{G}}$ decays.

the expected and observed $95\%$ $\text{CL}$ limits for the long-lived gluino model in the mass-lifetime plane, assuming a $100\%$ branching fraction for $\widetilde{\mathrm{g}}\to\mathrm{g}\widetilde{\mathrm{G}}$ decays, based on the NLO+NLL calculation of the gluino pair production cross section at $\sqrt{s}=13\ \mathrm{TeV}$.

the expected and observed $95\%$ $\text{CL}$ upper limits on the pair production cross section of the long-lived gluino, assuming a $100\%$ branching fraction for $\widetilde{\mathrm{g}}\to\mathrm{tbs}$ decays.

the expected and observed $95\%$ $\text{CL}$ limits for the long-lived gluino model in the mass-lifetime plane, assuming a $100\%$ branching fraction for $\widetilde{\mathrm{g}}\to\mathrm{tbs}$ decays, based on the NLO+NLL calculation of the gluino pair production cross section at $\sqrt{s}=13\ \mathrm{TeV}$.

the expected and observed $95\%$ $\text{CL}$ upper limits on the pair production cross section of the long-lived top squark, assuming a $100\%$ branching fraction for $\widetilde{\mathrm{t}}\to\mathrm{b}\ell$ decays.

the expected and observed $95\%$ $\text{CL}$ limits for the long-lived top squark model in the mass-lifetime plane, assuming a $100\%$ branching fraction for $\widetilde{\mathrm{t}}\to\mathrm{b}\ell$ decays, based on the NLO+NLL calculation of the top squark pair production cross section at $\sqrt{s}=13\ \mathrm{TeV}$.

the expected and observed $95\%$ $\text{CL}$ upper limits on the the pair production cross section of the long-lived top squark, assuming a $100\%$ branching fraction for $\widetilde{\mathrm{t}}\to\mathrm{\overline{d}\overline{d}}$ decays.

the expected and observed $95\%$ $\text{CL}$ limits for the long-lived top squark model in the mass-lifetime plane, assuming a $100\%$ branching fraction for $\widetilde{\mathrm{t}}\to\mathrm{\overline{d}\overline{d}}$ decays, based on an NLO+NLL calculation of the top squark pair production cross section at $\sqrt{s}=13\ \mathrm{TeV}$.

The likelihood ratio for vertex track multiplicity

The likelihood ratio for vertex $L_{xy}$ significance

The likelihood ratio for cluster RMS, the point where cluster RMS equals $-1.0$ represents the case where there is no cluster being reconstructed for the dijet candidate

The theoretical EWK WZ cross section in the tight EWK fiducial region. Can be multiplied by the measured EWK WZ scale factor to find the measured EWK WZ cross section.

aQGC limits on effective field theory parameters in EWK WZ events

Expected and observed 95\% \CL exclusion limits on the HH production cross section for the different channels and their combination for each benchmark model.

Expected and observed 95\% \CL exclusion limits on the HH production cross section for the bbVV channel and for each benchmark model.

Expected and observed 95\% \CL exclusion limits on the HH production cross section for the bbbb channel and for each benchmark model.

Expected and observed 95\% \CL exclusion limits on the HH production cross section for the bbtt channel and for each benchmark model.

Expected and observed 95\% \CL exclusion limits on the HH production cross section for the bbgg channel and for each benchmark model.

Expected and observed 95\% \CL exclusion limits on the HH production cross section for the combination of all channels and for each benchmark model.

Expected and observed 95\% \CL exclusion limits on the production of a narrow, spin two resonance (X) decaying into a pair of Higgs bosons.

NMSSM 95% CL upper limit on cross section times branching ratio

NMSSM 95% CL upper limit on cross section times branching ratio

NMSSM 95% CL upper limit on cross section times branching ratio

NMSSM 95% CL upper limit on cross section times branching ratio

90% CL upper limit on MSSMD kinetic mixing parameter epsilon

90% CL upper limit on MSSMD kinetic mixing parameter epsilon

90% CL upper limit on MSSMD kinetic mixing parameter epsilon

90% CL upper limit on MSSMD kinetic mixing parameter epsilon

Higgs boson transverse momentum spectrum, $H\rightarrow b\overline{b}$

Combined Higgs boson transverse momentum spectrum, ggH only

Combined Higgs boson jet multiplicity spectrum

Higgs boson jet multiplicity spectrum, $H\rightarrow\gamma\gamma$

Higgs boson jet multiplicity spectrum, $H\rightarrow ZZ$

Combined Higgs boson rapidity spectrum

Higgs boson rapidity spectrum, $H\rightarrow\gamma\gamma$

Higgs boson rapidity spectrum, $H\rightarrow ZZ$

Combined leading jet transverse momentum spectrum

Leading jet transverse momentum spectrum, $H\rightarrow\gamma\gamma$

Leading jet transverse momentum spectrum, $H\rightarrow ZZ$

Measured cross sections obtained with the BDT-based analyses. The uncertainties listed are statistical and systematic. For the results listed in the left (right) half of the table, Higgs boson contributions are counted as signal (background). The VVV cross section is calculated from the fit for \mu_{comb}. For ZZZ production, 95% confidence level upper limits are reported.