The $\varepsilon_{\text{reco}}$ values as a function of $E_{g}$, for $\tilde{g}$ R-hadrons that stop in the EB or HB, in the MC simulation, for the calorimeter search. The $\varepsilon_{\text{reco}}$ values are plotted for the two-body gluino decay, when $m_{\tilde{g}}$ is 1200 GeV.

The $\varepsilon_{\text{reco}}$ values as a function of $E_{g}$, for $\tilde{g}$ R-hadrons that stop in the EB or HB, in the MC simulation, for the calorimeter search. The $\varepsilon_{\text{reco}}$ values are plotted for the two-body gluino decay, when $m_{\tilde{g}}$ is 1800 GeV.

The $\varepsilon_{\text{reco}}$ values as a function of $E_{t}$, for $\tilde{t}$ R-hadrons that stop in the EB or HB, in the MC simulation, for the calorimeter search. The $\varepsilon_{\text{reco}}$ values are plotted for the two-body top squark decays, when $m_{\tilde{t}}$ is 400 GeV.

The $\varepsilon_{\text{reco}}$ values as a function of $E_{t}$, for $\tilde{t}$ R-hadrons that stop in the EB or HB, in the MC simulation, for the calorimeter search. The $\varepsilon_{\text{reco}}$ values are plotted for the two-body top squark decays, when $m_{\tilde{t}}$ is 600 GeV.

The $\varepsilon_{\text{reco}}$ values as a function of $E_{t}$, for $\tilde{t}$ R-hadrons that stop in the EB or HB, in the MC simulation, for the calorimeter search. The $\varepsilon_{\text{reco}}$ values are plotted for the two-body top squark decays, when $m_{\tilde{t}}$ is 1000 GeV.

The $\varepsilon_{\text{reco}}$ values as a function of $m_{\tilde{g}} - m_{\tilde{\chi}^{0}}$, for $\tilde{g}$ R-hadrons that stop in the EB or HB, in the MC simulation, for the calorimeter search. The $\varepsilon_{\text{reco}}$ values are plotted for the three-body gluino decay, when $m_{\tilde{g}}$ is 800 and 1000 GeV.

The $\varepsilon_{\text{reco}}$ values as a function of $m_{\tilde{g}} - m_{\tilde{\chi}^{0}}$, for $\tilde{g}$ R-hadrons that stop in the EB or HB, in the MC simulation, for the calorimeter search. The $\varepsilon_{\text{reco}}$ values are plotted for the three-body gluino decay, when $m_{\tilde{g}}$ is 1800 GeV.

The background extrapolation for the muon search. The integral of the fit function to $\Delta t_{DT}$ with the sum of two Gaussian distributions and a Crystal Ball function, for $\Delta t_{DT}$>−20 ns, is plotted as a function of the lower $\Delta t_{RPC}$ selection, for 2015 and 2016 data. The uncertainties correspond to when the fit function parameters are varied by one standard deviation.

The 95% CL upper limits on $\mathcal{B}\sigma$ for gluino pair production, using the cloud model of R-hadron interactions, as a function of lifetime, for combined 2015 and 2016 data for the calorimeter search. We show gluinos that undergo a two-body decay. The discontinuous structure observed between $10^{-7}$ and $10^{-5}$ s is due to the increase of the number of observed events in the search window as the lifetime increases.

The 95% CL upper limits on $\mathcal{B}\sigma$ for top squark pair production, using the cloud model of R-hadron interactions, as a function of lifetime, for combined 2015 and 2016 data for the calorimeter search. We show top squarks that undergo a two-body decay. The discontinuous structure observed between $10^{-7}$ and $10^{-5}$ s is due to the increase of the number of observed events in the search window as the lifetime increases.

The 95% CL upper limits on $\mathcal{B}\sigma$ for gluino pair production, using the cloud model of R-hadron interactions, as a function of lifetime, for combined 2015 and 2016 data for the calorimeter search. We show gluinos that undergo a three-body decay. The discontinuous structure observed between $10^{-7}$ and $10^{-5}$ s is due to the increase of the number of observed events in the search window as the lifetime increases.

The 95% CL upper limits on the gluino mass, using the cloud model of R-hadron interactions, as a function of lifetime, for combined 2015 and 2016 data for the calorimeter search. We show gluinos that undergo a two-body decay. The discontinuous structure observed between $10^{-7}$ and $10^{-5}$ s is due to the increase of the number of observed events in the search window as the lifetime increases.

The 95% CL upper limits on the top squark mass, using the cloud model of R-hadron interactions, as a function of lifetime, for combined 2015 and 2016 data for the calorimeter search. We show top squarks that undergo a two-body decay. The discontinuous structure observed between $10^{-7}$ and $10^{-5}$ s is due to the increase of the number of observed events in the search window as the lifetime increases.

The 95% CL upper limits on the gluino mass, using the cloud model of R-hadron interactions, as a function of lifetime, for combined 2015 and 2016 data for the calorimeter search. We show gluinos that undergo a three-body decay. The discontinuous structure observed between $10^{-7}$ and $10^{-5}$ s is due to the increase of the number of observed events in the search window as the lifetime increases.

The 95% CL upper limits in the neutralino mass vs.~gluino mass plane, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the calorimeter search. The mostly triangular region shows the excluded observed region. We show gluinos that undergo a two-body decay.

The 95% CL upper limits in the neutralino mass vs.~gluino mass plane, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the calorimeter search. The mostly triangular region shows the excluded expected region. We show gluinos that undergo a two-body decay.

The 95% CL upper limits in the neutralino mass vs.~gluino mass plane, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the calorimeter search. The mostly triangular region shows the excluded expected +1 s.d. region. We show gluinos that undergo a two-body decay.

The 95% CL upper limits in the neutralino mass vs.~gluino mass plane, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the calorimeter search. The mostly triangular region shows the excluded expected -1 s.d. region. We show gluinos that undergo a two-body decay.

The 95% CL upper limits in the neutralino mass vs.~top squark mass plane, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the calorimeter search. The mostly triangular region shows the excluded observed region. We show top squarks that undergo a two-body decay.

The 95% CL upper limits in the neutralino mass vs.~top squark mass plane, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the calorimeter search. The mostly triangular region shows the excluded expected region. We show top squarks that undergo a two-body decay.

The 95% CL upper limits in the neutralino mass vs.~top squark mass plane, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the calorimeter search. The mostly triangular region shows the excluded expected +1 s.d. region. We show top squarks that undergo a two-body decay.

The 95% CL upper limits in the neutralino mass vs.~top squark mass plane, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the calorimeter search. The mostly triangular region shows the excluded expected -1 s.d. region. We show top squarks that undergo a two-body decay.

The 95% CL upper limits in the neutralino mass vs.~gluino mass plane, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the calorimeter search. The mostly triangular region shows the excluded observed region. We show gluinos that undergo a three-body decay.

The 95% CL upper limits in the neutralino mass vs.~gluino mass plane, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the calorimeter search. The mostly triangular region shows the excluded expected region. We show gluinos that undergo a three-body decay.

The 95% CL upper limits in the neutralino mass vs.~gluino mass plane, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the calorimeter search. The mostly triangular region shows the excluded expected +1 s.d. region. We show gluinos that undergo a three-body decay.

The 95% CL upper limits in the neutralino mass vs.~gluino mass plane, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the calorimeter search. The mostly triangular region shows the excluded expected -1 s.d. region. We show gluinos that undergo a three-body decay.

The 95% CL upper limits on $\mathcal{B}\sigma$ for 1000 GeV gluino pair production as a function of lifetime, for combined 2015 and 2016 data for the muon search.

The 95% CL upper limits on $\mathcal{B}\sigma$ for 400 GeV MCHAMP pair production as a function of lifetime, for combined 2015 and 2016 data for the muon search.

95% CL upper limits on $\mathcal{B}\sigma$ for gluino pair production as a function of mass, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the muon search. The theory curves assume $\mathcal{B}=100\%$.

95% CL upper limits on $\mathcal{B}\sigma$ for MCHAMP pair production as a function of mass, for lifetimes between 10 $\mu$s and 1000 s, for combined 2015 and 2016 data for the muon search. The theory curves assume $\mathcal{B}=100\%$.

Measured signal cross section for dielectron, dimuon and combined dilepton channels. The measurement is performed in a kinematic region defined by invariant masses $m_{ll}~>~50$ GeV, $m_{jj}~>~120$ GeV, and transverse momenta $p_{Tj}~>~25$ GeV, where $l$ denotes electrons and muons, and $j$ - quarks produced in the hard interaction.

Distributions of $p_{TZ}$ in data and total SM background, EW Zjj signal and two ATGC scenarios in the dimuon channel

Distributions of $p_{TZ}$ in data and total SM background, EW Zjj signal and two ATGC scenarios in the dielectron channel

Distributions of $m_{jj}$ in data and total SM background and EW Zjj signal in the dimuon channel. Kinematic region is defined by invariant masses $m_{ll}~>~50$ GeV, $m_{jj}~>~120$ GeV, and transverse momenta $p_{Tj}~>~25$ GeV, where $l$ denotes electrons and muons, and $j$ - quarks produced in the hard interaction.

Distributions of $m_{jj}$ in data and total SM background and EW Zjj signal in the dimuon channel. Kinematic region is defined by invariant masses $m_{ll}~>~50$ GeV, $m_{jj}~>~120$ GeV, and transverse momenta $p_{Tj}~>~25$ GeV, where $l$ denotes electrons and muons, and $j$ - quarks produced in the hard interaction.

Distributions of the transformed BDT discriminant in data and total SM background and EW Zjj signal in the dimuon channel. Kinematic region is defined by invariant masses $m_{ll}~>~50$ GeV, $m_{jj}~>~120$ GeV, and transverse momenta $p_{Tj}~>~25$ GeV, where $l$ denotes electrons and muons, and $j$ - quarks produced in the hard interaction.

Distributions of the transformed BDT discriminant in data and total SM background and EW Zjj signal in the dimuon channel. Kinematic region is defined by invariant masses $m_{ll}~>~50$ GeV, $m_{jj}~>~120$ GeV, and transverse momenta $p_{Tj}~>~25$ GeV, where $l$ denotes electrons and muons, and $j$ - quarks produced in the hard interaction.

Efficiency of a gap activity veto in dielectron and dimuon events with BDT > 0.92, as a function of the additional jet $p_T$ for data, MC expectations with only DY events, including signal with the PYTHIA PS model, or the HERWIG++ PS model.

Efficiency of a gap activity veto in dielectron and dimuon events with BDT > 0.92, as a function of total $H_T$ of additional jets for data, MC expectations with only DY events, including signal with the PYTHIA PS model, or the HERWIG++ PS model.

Efficiency of a gap activity veto in dielectron and dimuon events with BDT > 0.92, as a function of total soft $H_T$ for data, MC expectations with only DY events, including signal with the PYTHIA PS model, or the HERWIG++ PS model.

Efficiency of a gap activity veto in dielectron and dimuon events with BDT > 0.92, as a function of the leading soft track-jet $p_T$ for data, MC expectations with only DY events, including signal with the PYTHIA PS model, or the HERWIG++ PS model.

Figure 8. Gluino pair production cross section.

Table 1. Post-fit yields for the background-only fit, observed data, and expected yields for mgluino = 1600 GeV in each search bin.

Differential cross section of J/psi mesons from b hadrons as a function of dimuon pT in pp and PbPb collisions. The PbPb cross sections are normalised by TAA for direct comparison. Global uncertainties arise from the integrated luminosity uncertainty in pp collisions, and the number of minimum bias events and TAA uncertainties for PbPb collisions.

Differential cross section of prompt J/psi mesons as a function of dimuon rapidty in pp and PbPb collisions. The PbPb cross sections are normalised by TAA for direct comparison. Global uncertainties arise from the integrated luminosity uncertainty in pp collisions, and the number of minimum bias events and TAA uncertainties for PbPb collisions.

Differential cross section of J/psi mesons from b hadrons as a function of dimuon rapidty in pp and PbPb collisions. The PbPb cross sections are normalised by TAA for direct comparison. Global uncertainties arise from the integrated luminosity uncertainty in pp collisions, and the number of minimum bias events and TAA uncertainties for PbPb collisions.

Nuclear modification factor of prompt J/psi mesons as a function of dimuon rapidity. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of collision centrality. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of dimuon pT. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of dimuon pT in the mid-rapidity interval. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of dimuon pT in the most forward rapidity interval. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of collision centrality in the mid- and most forward rapidity intervals. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of pT in three centrality bins. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of collision centrality in the most forward rapidity range at moderate and high pT. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of collision centrality in the mid-rapidity range. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Nuclear modification factor of prompt psi(2S) mesons as a function of collision centrality in the mid-rapidity range. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

95% CL intervals on the nuclear modification factor of prompt psi(2S) mesons as a function of collision centrality in the mid-rapidity range. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Nuclear modification factor of prompt J/psi and psi(2S) mesons as a function of dimuon pT in the mid-rapidity range. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of collision centrality in the forward rapidity range. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Nuclear modification factor of prompt psi(2S) mesons as a function of collision centrality in the forward rapidity range. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

95% CL intervals on the nuclear modification factor of prompt psi(2S) mesons as a function of collision centrality in the forward rapidity range. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Nuclear modification factor of prompt J/psi mesons as a function of dimuon pT in the forward rapidity range. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of prompt psi(2S) mesons as a function of dimuon pT in the forward rapidity range. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

95% CL intervals on the nuclear modification factor of prompt psi(2S) mesons as a function of dimuon pT in the forward rapidity range. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of nonprompt J/psi mesons as a function of dimuon rapidity. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of nonprompt J/psi mesons as a function of collision centrality. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Nuclear modification factor of nonprompt J/psi mesons as a function of dimuon pT. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of nonprompt J/psi mesons as a function of dimuon pT in the mid-rapidity interval. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of nonprompt J/psi mesons as a function of dimuon pT in the most forward rapidity interval. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of nonprompt J/psi mesons as a function of collision centrality in the mid- and most forward rapidity intervals. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Nuclear modification factor of nonprompt J/psi mesons as a function of pT in three centrality bins. Global uncertainties arise from the integrated luminosity uncertainty of the pp data, and the number of minimum bias events and TAA uncertainties of the PbPb data.

Nuclear modification factor of nonprompt J/psi mesons as a function of collision centrality in the most forward rapidity range at moderate and high pT. Global uncertainties arise from the full pp statistical and systematic uncertainties (including integrated luminosity uncertainty), and the number of minimum bias events uncertainty of the PbPb data.

Expected and observed 95 percent CL upper limits on BR(H to etau) for each individual category and combined from collinear mass fit analysis

Summary of the observed and expected upper limits at the 95percent CL and the best fit branching fractions in percent for the H->mutau and H->etau processes, for the main analysis (BDT fit) and the cross check (Mcol fit) method.

95 percent CL observed upper limit on the Yukawa couplings for the main analysis (BDT fit) and the cross check (Mcol fit) method

Normalized inclusive 2-jet cross section differential in $\Delta\phi_{1,2}$ for $500 < p_{T}^{max} < 600$ GeV

Normalized inclusive 2-jet cross section differential in $\Delta\phi_{1,2}$ for $600 < p_{T}^{max} < 700$ GeV

Normalized inclusive 2-jet cross section differential in $\Delta\phi_{1,2}$ for $700 < p_{T}^{max} < 800$ GeV

Normalized inclusive 2-jet cross section differential in $\Delta\phi_{1,2}$ for $800 < p_{T}^{max} < 1000$ GeV

Normalized inclusive 2-jet cross section differential in $\Delta\phi_{1,2}$ for $1000 < p_{T}^{max} < 1200$ GeV

Normalized inclusive 2-jet cross section differential in $\Delta\phi_{1,2}$ for $p_{T}^{max} > 1200$ GeV

Normalized inclusive 3-jet cross section differential in $\Delta\phi_{1,2}$ for $200 < p_{T}^{max} < 300$ GeV

Normalized inclusive 3-jet cross section differential in $\Delta\phi_{1,2}$ for $300 < p_{T}^{max} < 400$ GeV

Normalized inclusive 3-jet cross section differential in $\Delta\phi_{1,2}$ for $400 < p_{T}^{max} < 500$ GeV

Normalized inclusive 3-jet cross section differential in $\Delta\phi_{1,2}$ for $500 < p_{T}^{max} < 600$ GeV

Normalized inclusive 3-jet cross section differential in $\Delta\phi_{1,2}$ for $600 < p_{T}^{max} < 700$ GeV

Normalized inclusive 3-jet cross section differential in $\Delta\phi_{1,2}$ for $700 < p_{T}^{max} < 800$ GeV

Normalized inclusive 3-jet cross section differential in $\Delta\phi_{1,2}$ for $800 < p_{T}^{max} < 1000$ GeV

Normalized inclusive 3-jet cross section differential in $\Delta\phi_{1,2}$ for $p_{T}^{max} > 1000$ GeV

Normalized inclusive 4-jet cross section differential in $\Delta\phi_{1,2}$ for $200 < p_{T}^{max} < 300$ GeV

Normalized inclusive 4-jet cross section differential in $\Delta\phi_{1,2}$ for $300 < p_{T}^{max} < 400$ GeV

Normalized inclusive 4-jet cross section differential in $\Delta\phi_{1,2}$ for $400 < p_{T}^{max} < 500$ GeV

Normalized inclusive 4-jet cross section differential in $\Delta\phi_{1,2}$ for $500 < p_{T}^{max} < 600$ GeV

Normalized inclusive 4-jet cross section differential in $\Delta\phi_{1,2}$ for $600 < p_{T}^{max} < 700$ GeV

Normalized inclusive 4-jet cross section differential in $\Delta\phi_{1,2}$ for $700 < p_{T}^{max} < 800$ GeV

Normalized inclusive 4-jet cross section differential in $\Delta\phi_{1,2}$ for $800 < p_{T}^{max} < 1000$ GeV

Normalized inclusive 4-jet cross section differential in $\Delta\phi_{1,2}$ for $p_{T}^{max} > 1000$ GeV

Normalized inclusive 3-jet cross section differential in $\Delta\phi_{2j}^{min}$ for $200 < p_{T}^{max} < 300$ GeV

Normalized inclusive 3-jet cross section differential in $\Delta\phi_{2j}^{min}$ for $300 < p_{T}^{max} < 400$ GeV

Normalized inclusive 3-jet cross section differential in $\Delta\phi_{2j}^{min}$ for $400 < p_{T}^{max} < 500$ GeV

Normalized inclusive 3-jet cross section differential in $\Delta\phi_{2j}^{min}$ for $500 < p_{T}^{max} < 600$ GeV

Normalized inclusive 3-jet cross section differential in $\Delta\phi_{2j}^{min}$ for $600 < p_{T}^{max} < 700$ GeV

Normalized inclusive 3-jet cross section differential in $\Delta\phi_{2j}^{min}$ for $700 < p_{T}^{max} < 800$ GeV

Normalized inclusive 3-jet cross section differential in $\Delta\phi_{2j}^{min}$ for $800 < p_{T}^{max} < 1000$ GeV

Normalized inclusive 3-jet cross section differential in $\Delta\phi_{2j}^{min}$ for $p_{T}^{max} > 1000$ GeV

Normalized inclusive 4-jet cross section differential in $\Delta\phi_{2j}^{min}$ for $200 < p_{T}^{max} < 300$ GeV

Normalized inclusive 4-jet cross section differential in $\Delta\phi_{2j}^{min}$ for $300 < p_{T}^{max} < 400$ GeV

Normalized inclusive 4-jet cross section differential in $\Delta\phi_{2j}^{min}$ for $400 < p_{T}^{max} < 500$ GeV

Normalized inclusive 4-jet cross section differential in $\Delta\phi_{2j}^{min}$ for $500 < p_{T}^{max} < 600$ GeV

Normalized inclusive 4-jet cross section differential in $\Delta\phi_{2j}^{min}$ for $600 < p_{T}^{max} < 700$ GeV

Normalized inclusive 4-jet cross section differential in $\Delta\phi_{2j}^{min}$ for $700 < p_{T}^{max} < 800$ GeV

Normalized inclusive 4-jet cross section differential in $\Delta\phi_{2j}^{min}$ for $800 < p_{T}^{max} < 1000$ GeV

Normalized inclusive 4-jet cross section differential in $\Delta\phi_{2j}^{min}$ for $p_{T}^{max} > 1000$ GeV

Comparison between data and MC simulation in the dimuon control samples before and after performing the simultaneous fit across all the control samples and the signal region assuming the absence of any signal. Plot correspond to the mono-V category. The hadronic recoil $p_{T}$ in dilepton events is used as a proxy for $p_{T}^{miss}$ in the signal region. The leading contribution is represented by Z+jets production. The other backgrounds include top quark, diboson, and W+jets processes.

Comparison between data and MC simulation in the dielectron control samples before and after performing the simultaneous fit across all the control samples and the signal region assuming the absence of any signal. Plot correspond to the monojet category. The hadronic recoil $p_{T}$ in dilepton events is used as a proxy for $p_{T}^{miss}$ in the signal region. The leading contribution is represented by Z+jets production. The other backgrounds include top quark, diboson, and W+jets processes.

Comparison between data and MC simulation in the dielectron control samples before and after performing the simultaneous fit across all the control samples and the signal region assuming the absence of any signal. Plot correspond to the mono-V category. The hadronic recoil $p_{T}$ in dilepton events is used as a proxy for $p_{T}^{miss}$ in the signal region. The leading contribution is represented by Z+jets production. The other backgrounds include top quark, diboson, and W+jets processes.

Comparison between data and MC simulation in the single-muon control samples before and after performing the simultaneous fit across all the control samples and the signal region assuming the absence of any signal. Plot correspond to the monojet category. The hadronic recoil $p_{T}$ in dilepton events is used as a proxy for $p_{T}^{miss}$ in the signal region. The leading contribution is represented by W+jets production. The other backgrounds include top quark, diboson, Z+jets, and QCD multijet processes.

Comparison between data and MC simulation in the single-muon control samples before and after performing the simultaneous fit across all the control samples and the signal region assuming the absence of any signal. Plot correspond to the mono-V category. The hadronic recoil $p_{T}$ in dilepton events is used as a proxy for $p_{T}^{miss}$ in the signal region. The leading contribution is represented by W+jets production. The other backgrounds include top quark, diboson, Z+jets, and QCD multijet processes.

Comparison between data and MC simulation in the single-electron control samples before and after performing the simultaneous fit across all the control samples and the signal region assuming the absence of any signal. Plot correspond to the monojet category. The hadronic recoil $p_{T}$ in dilepton events is used as a proxy for $p_{T}^{miss}$ in the signal region. The leading contribution is represented by Z+jets production. The other backgrounds include top quark, diboson, Z+jets, and QCD multijet processes.

Comparison between data and MC simulation in the single-electron control samples before and after performing the simultaneous fit across all the control samples and the signal region assuming the absence of any signal. Plot correspond to the mono-V category. The hadronic recoil $p_{T}$ in dilepton events is used as a proxy for $p_{T}^{miss}$ in the signal region. The leading contribution is represented by W+jets production. The other backgrounds include top quark, diboson, Z+jets, and QCD multijet processes.

Observed $p_{T}^{miss}$ distribution in the monojet signal region compared with the post-fit background expectations for various SM processes. The last bin includes all events with $p_{T}^{miss} > 1250$ GeV for the monojet category. The expected background distributions are evaluated after performing a combined fit to the data in all the control samples, not including the signal region. Expected signal distribution for a 2 TeV axial-vector mediator, decaying to 1 GeV DM particles, is overlaid.

Observed $p_{T}^{miss}$ distribution in the mono-V signal region compared with the post-fit background expectations for various SM processes. The last bin includes all events with $p_{T}^{miss} > 750$ GeV for the mono-V category. The expected background distributions are evaluated after performing a combined fit to the data in all the control samples, not including the signal region. Expected signal distribution for a 2 TeV axial-vector mediator, decaying to 1 GeV DM particles, is overlaid.

Observed $p_{T}^{miss}$ distribution in the monojet signal region compared with the post-fit background expectations for various SM processes. The last bin includes all events with $p_{T}^{miss} > 1250$ GeV for the monojet category. The expected background distributions are evaluated after performing a combined fit to the data in all the control samples, as well as in the signal region. The fit is performed assuming the absence of any signal. Expected signal distribution for a 2 TeV axial-vector mediator, decaying to 1 GeV DM particles, is overlaid.

Observed $p_{T}^{miss}$ distribution in the mono-V signal region compared with the post-fit background expectations for various SM processes. The last bin includes all events with $p_{T}^{miss} > 750$ GeV for the mono-V category. The expected background distributions are evaluated after performing a combined fit to the data in all the control samples, not including as well as in the signal region. The fit is performed assuming the absence of any signal. Expected signal distribution for a 2 TeV axial-vector mediator, decaying to 1 GeV DM particles, is overlaid.

Observed exclusion limits at 95% CL on $\mu = \sigma/\sigma_{th}$ in the $m_{med}-m_{DM}$ plane assuming a vector mediator. N.B.: the granularity in the presented limit values is reduced with respect to the published result.

Expected exclusion limits at 95% CL on $\mu = \sigma/\sigma_{th}$ in the $m_{med}-m_{DM}$ plane assuming a vector mediator. N.B.: the granularity in the presented limit values is reduced with respect to the published result.

Observed exclusion limits at 95% CL on $\mu = \sigma/\sigma_{th}$ in the $m_{med}-m_{DM}$ plane assuming an axial-vector mediator. N.B.: the granularity in the presented limit values is reduced with respect to the published result.

Expected exclusion limits at 95% CL on $\mu = \sigma/\sigma_{th}$ in the $m_{med}-m_{DM}$ plane assuming an axial-vector mediator. N.B.: the granularity in the presented limit values is reduced with respect to the published result.

Observed exclusion contour at 95% CL on $\mu = \sigma/\sigma_{th}$ in the $m_{med}-m_{DM}$ plane assuming a vector mediator.

Expected exclusion contour at 95% CL on $\mu = \sigma/\sigma_{th}$ in the $m_{med}-m_{DM}$ plane assuming a vector mediator.

Observed exclusion contour at 95% CL on $\mu = \sigma/\sigma_{th}$ in the $m_{med}-m_{DM}$ plane assuming an axial-vector mediator.

Expected exclusion contour at 95% CL on $\mu = \sigma/\sigma_{th}$ in the $m_{med}-m_{DM}$ plane assuming an axial-vector mediator.

Exclusion limits at 95% CL on $\mu = \sigma/\sigma_{th}$ vs $m_{med}$ for $m_{DM} = 1$ GeV assuming a scalar mediator.

Observed exclusion limits at 95% CL on $\mu = \sigma/\sigma_{th}$ in the $m_{med}-m_{DM}$ plane assuming a pseudoscalar mediator. N.B.: the granularity in the presented limit values is reduced with respect to the published result.

Expected exclusion limits at 95% CL on $\mu = \sigma/\sigma_{th}$ in the $m_{med}-m_{DM}$ plane assuming a pseudoscalar mediator. N.B.: the granularity in the presented limit values is reduced with respect to the published result.

Observed exclusion contour at 95% CL on $\mu = \sigma/\sigma_{th}$ in the $m_{med}-m_{DM}$ plane assuming a pseudoscalar mediator.

Expected exclusion contour at 95% CL on $\mu = \sigma/\sigma_{th}$ in the $m_{med}-m_{DM}$ plane assuming a pseudoscalar mediator.

Observed exclusion contour at 95% CL in the $g_{q}-m_{med}$ plane assuming a vector mediator.

Exclusion exclusion contour at 95% CL in the $g_{q}-m_{med}$ plane assuming a vector mediator.

Observed exclusion contour at 95% CL in the $g_{q}-m_{med}$ plane assuming an axial-vector mediator.

Exclusion exclusion contour at 95% CL in the $g_{q}-m_{med}$ plane assuming an axial-vector mediator.

Observed upper limits at 90% CL on $\sigma_{DM-nucleon}$ vs $m_{med}$ for vector mediator

Expected upper limits at 90% CL on $\sigma_{DM-nucleon}$ vs $m_{med}$ for vector mediator

Observed upper limits at 90% CL on $\sigma_{DM-nucleon}$ vs $m_{med}$ for axial-vector mediator

Expected upper limits at 90% CL on $\sigma_{DM-nucleon}$ vs $m_{med}$ for axial-vector mediator

Observed upper limits at 90% CL on velocity averaged DM annihilation cross section derived from those placed for pseudoscalar mediators.

Expected upper limits at 90% CL on velocity averaged DM annihilation cross section derived from those placed for pseudoscalar mediators.

Correlations between the predicted background yields in all the $p_{T}^{miss}$ bins of the monojet signal region.

Correlations between the predicted background yields in all the $p_{T}^{miss}$ bins of the mono-V signal region.