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A search for new long-lived particles decaying to leptons using proton-proton collision data produced by the CERN LHC at $\sqrt{s}$ = 13 TeV is presented. Events are selected with two leptons (an electron and a muon, two electrons, or two muons) that both have transverse impact parameter values between 0.01 and 10 cm and are not required to form a common vertex. Data used for the analysis were collected with the CMS detector in 2016, 2017, and 2018, and correspond to an integrated luminosity of 118 (113) fb$^{-1}$ in the ee channel (e$\mu$ and $\mu\mu$ channels). The search is designed to be sensitive to a wide range of models with displaced e$\mu$, ee, and $\mu\mu$ final states. The results constrain several well-motivated models involving new long-lived particles that decay to displaced leptons. For some areas of the available phase space, these are the most stringent constraints to date.
The distribution of electron $|d_0|$ for the events in data and signal that pass the e$\mu$ preselection. In all of the histograms, the last bin includes the overflow. The electron $|d_0|$ distributions have a longer tail than those of muons because the muon $|d_0|$ values are measured more precisely.
The distribution of muon $|d_0|$ for the events in data and signal that pass the e$\mu$ preselection. In all of the histograms, the last bin includes the overflow. The electron $|d_0|$ distributions have a longer tail than those of muons because the muon $|d_0|$ values are measured more precisely.
Two-dimensional distribution of $|d_{0}^{a}|$ vs $|d_{0}^{b}|$, for simulated background events passing the e$\mu$ preselection with 2018 conditions. In each $|d_{0}^{a}|$-$|d_{0}^{b}|$ bin, the number of events divided by the bin area is plotted. The inclusive signal region covers the region between 100 $\mu$m and 10 cm in each $|d_{0}|$ variable shown.
Two-dimensional distributions of the leading electron vs the leading muon $|d_{0}|$, for the events that pass the e$\mu$ preselection. Data events and $\tilde{t} \to b\ell$ signal events with a $\tilde{t}$ mass of 700 GeV and a proper decay length of 10 mm that correspond to 2018 data-taking conditions are shown. In each $|d_{0}|$-$|d_{0}|$ bin, the number of events divided by the bin area is plotted. The inclusive signal region covers the region between 100 $\mu$m and 10 cm in each $|d_{0}|$ variable shown.
Two-dimensional distributions of the leading vs the subleading electron $|d_0|$, for the events that pass the ee preselection. Data events and $\tilde{t} \to b\ell$ signal events with a $\tilde{t}$ mass of 700 GeV and a proper decay length of 10 mm that correspond to 2018 data-taking conditions are shown. In each $|d_{0}|$-$|d_{0}|$ bin, the number of events divided by the bin area is plotted. The inclusive signal region covers the region between 100 $\mu$m and 10 cm in each $|d_{0}|$ variable shown.
Two-dimensional distributions of the leading vs the subleading muon $|d_{0}|$, for the events that pass the $\mu\mu$ preselection. Data events and $\tilde{t} \to b\ell$ signal events with a $\tilde{t}$ mass of 700 GeV and a proper decay length of 10 mm that correspond to 2018 data-taking conditions are shown. In each $|d_{0}|$-$|d_{0}|$ bin, the number of events divided by the bin area is plotted. The inclusive signal region covers the region between 100 $\mu$m and 10 cm in each $|d_{0}|$ variable shown.
The number of observed and estimated background events in each channel and SR, with a representative signal overlaid. For each background estimate and signal yield, the total uncertainty (statistical plus systematic) is given. The distributions shown correspond to the events before the final maximum likelihood fit to the data.
The number of observed and estimated background events in each channel and SR in 2016, with a representative signal overlaid. For each background estimate and signal yield, the total uncertainty is given. The distributions shown correspond to the events before the final maximum likelihood fit to the data.
The number of observed and estimated background events in each channel and SR in 2017 and 2018, with a representative signal overlaid. For each background estimate and signal yield, the total uncertainty is given. The distributions shown correspond to the events before the final maximum likelihood fit to the data.
The observed 95% CL upper limits on the long-lived top squark production cross section, in the $c\tau_0$ -- mass plane, for the three channels combined. The $\tilde{t} \to b\ell $ process is shown. These limits assume $\mathcal{B}(\tilde{t} \to b\ell)$ is 100%, and each lepton has an equal probability of being an electron, a muon, or a tau lepton. The area to the left of the black curve represents the observed exclusion region, and the dashed red lines indicate the expected limits and their 68% confidence intervals.
The observed 95% CL upper limits on the long-lived top squark production cross section, in the $c\tau_0$ -- mass plane, for the three channels combined. The $\tilde{t} \to d\ell$ process is shown. These limits assume $\mathcal{B}(\tilde{t} \to d\ell)$ is 100%, and each lepton has an equal probability of being an electron, a muon, or a tau lepton. The area to the left of the black curve represents the observed exclusion region, and the dashed red lines indicate the expected limits and their 68% confidence intervals.
The observed 95% CL upper limits on the long-lived top squark production cross section, in the $c\tau_0$ -- mass plane, for the three channels combined. The $\tilde{t} \to b\ell $ process is shown. These limits assume $\mathcal{B}(\tilde{t} \to b\ell)$ is 100%, and each lepton has an equal probability of being an electron, a muon, or a tau lepton. The area to the left of the black curve represents the observed exclusion region, and the dashed red lines indicate the expected limits and their 68% confidence intervals.
The observed 95% CL upper limits on the long-lived top squark production cross section, in the $c\tau_0$ -- mass plane, for the three channels combined. The $\tilde{t} \to d\ell$ process is shown. These limits assume $\mathcal{B}(\tilde{t} \to d\ell)$ is 100%, and each lepton has an equal probability of being an electron, a muon, or a tau lepton. The area to the left of the black curve represents the observed exclusion region, and the dashed red lines indicate the expected limits and their 68% confidence intervals.
The 95% CL upper limits on the long-lived top squark proper decay length ($c\tau_0$) as a function of its mass, for the e$\mu$, ee, and $\mu\mu$ channels, and their combination. The $\tilde{t} \to b\ell $ process is shown. These limits assume $\mathcal{B}(\tilde{t} \to b\ell)$ is 100%, and each lepton has an equal probability of being an electron, a muon, or a tau lepton.
The 95% CL upper limits on the long-lived top squark proper decay length ($c\tau_0$) as a function of its mass, for the e$\mu$, ee, and $\mu\mu$ channels, and their combination. The $\tilde{t} \to d\ell$ process is shown. These limits assume $\mathcal{B}(\tilde{t} \to d\ell)$ is 100%, and each lepton has an equal probability of being an electron, a muon, or a tau lepton.
The 95% CL constraints on the long-lived slepton $c\tau_{0}$ and mass. The $\tilde{\tau}$ and co-NLSP limits are shown for the three channels combined, while the $\tilde{e}$ and $\tilde{\mu}$ NLSP limits are shown for the ee and $\mu\mu$ channels, respectively. These limits assume that the superpartners of the left- and right-handed leptons are degenerate in mass and $\mathcal{B}(\tilde{\ell} \to \ell\tilde{G})$ is 100%. The area to the left of the solid curves represents the observed exclusion region, and the dashed lines indicate the expected limits.
The observed 95% CL upper limits on the long-lived slepton production cross section, in the $c\tau_0$ -- mass plane. The co-NLSP limits are shown for the three channels combined. These limits assume that the superpartners of the left- and right-handed leptons are degenerate in mass and $\mathcal{B}(\tilde{\ell} \to \ell\tilde{G})$ is 100%. The area to the left of the black curve represents the observed exclusion region, and the dashed red lines indicate the expected limits and their 68% confidence intervals.
The observed 95% CL upper limits on the long-lived slepton production cross section, in the $c\tau_0$ -- mass plane. The co-NLSP limits are shown for the three channels combined. These limits assume that the superpartners of the left- and right-handed leptons are degenerate in mass and $\mathcal{B}(\tilde{\ell} \to \ell\tilde{G})$ is 100%. The area to the left of the black curve represents the observed exclusion region, and the dashed red lines indicate the expected limits and their 68% confidence intervals.
The 95% CL upper limits on the $\mathrm{H} \to \mathrm{S}\mathrm{S}, \mathrm{S} \to \ell^{+}\ell^{-}$ branching fraction as a function of $c\tau_0$, for a Higgs boson with a mass of 125 GeV and a long-lived scalar with a mass of 30 GeV or 50 GeV, for the three channels combined. These limits assume that $\mathcal{B}(H \to SS)=100\%$ and each S has a 50% probability of decaying to two electrons or two muons. The area above the solid (dashed) curve represents the observed (expected) exclusion region.
The 95% CL upper limits on the product of the cross section and branching fraction $\mathrm{H} \to \mathrm{S}\mathrm{S}, \mathrm{S} \to \ell^{+}\ell^{-}$ as a function of $c\tau_0$, for a 300 GeV Higgs boson and several long-lived scalar masses, for the three channels combined. These limits assume that $\mathcal{B}(H \to SS)=100\%$ and each S has a 50% probability of decaying to two electrons or two muons. The area above the solid (dashed) curves represents the observed (expected) exclusion region.
The 95% CL upper limits on the product of the cross section and branching fraction $\mathrm{H} \to \mathrm{S}\mathrm{S}, \mathrm{S} \to \ell^{+}\ell^{-}$ as a function of $c\tau_0$, for a 400 GeV Higgs boson and several long-lived scalar masses, for the three channels combined. These limits assume that $\mathcal{B}(H \to SS)=100\%$ and each S has a 50% probability of decaying to two electrons or two muons. The area above the solid (dashed) curves represents the observed (expected) exclusion region.
The 95% CL upper limits on the product of the cross section and branching fraction $\mathrm{H} \to \mathrm{S}\mathrm{S}, \mathrm{S} \to \ell^{+}\ell^{-}$ as a function of $c\tau_0$, for a 600 GeV Higgs boson and several long-lived scalar masses, for the three channels combined. These limits assume that $\mathcal{B}(H \to SS)=100\%$ and each S has a 50% probability of decaying to two electrons or two muons. The area above the solid (dashed) curves represents the observed (expected) exclusion region.
The 95% CL upper limits on the product of the cross section and branching fraction $\mathrm{H} \to \mathrm{S}\mathrm{S}, \mathrm{S} \to \ell^{+}\ell^{-}$ as a function of $c\tau_0$, for a 800 GeV Higgs boson and several long-lived scalar masses, for the three channels combined. These limits assume that $\mathcal{B}(H \to SS)=100\%$ and each S has a 50% probability of decaying to two electrons or two muons. The area above the solid (dashed) curves represents the observed (expected) exclusion region.
The 95% CL upper limits on the product of the cross section and branching fraction $\mathrm{H} \to \mathrm{S}\mathrm{S}, \mathrm{S} \to \ell^{+}\ell^{-}$ as a function of $c\tau_0$, for a 1000 GeV Higgs boson and several long-lived scalar masses, for the three channels combined. These limits assume that $\mathcal{B}(H \to SS)=100\%$ and each S has a 50% probability of decaying to two electrons or two muons. The area above the solid (dashed) curves represents the observed (expected) exclusion region.
The 95% CL upper limits on the $\mathrm{H} \to \mathrm{S}\mathrm{S} \to 4\ell$ branching fraction as a function of $c\tau_0$, for a Higgs boson with a mass of 125 GeV and a long-lived scalar with a mass of 30 GeV or 50 GeV, for the ee channel only. These limits assume that $\mathcal{B}(H \to SS)=100\%$ and each S has a 50% probability of decaying to two electrons. The area above the solid (dashed) curve represents the observed (expected) exclusion region. The curves are not smooth because very few ee channel events pass the preselection for the Higgs boson and scalar masses shown in this figure.
The 95% CL upper limits on the product of the cross section and branching fraction $\mathrm{H} \to \mathrm{S}\mathrm{S} \to 4\ell$ as a function of $c\tau_0$, for a 600 GeV Higgs boson and several long-lived scalar masses, for the ee channel only. These limits assume that $\mathcal{B}(H \to SS)=100\%$ and each S has a 50% probability of decaying to two electrons. The area above the solid (dashed) curves represents the observed (expected) exclusion region.
The 95% CL upper limits on the product of the cross section and branching fraction $\mathrm{H} \to \mathrm{S}\mathrm{S} \to 4\ell$ as a function of $c\tau_0$, for a 1000 GeV Higgs boson and several long-lived scalar masses, for the ee channel only. These limits assume that $\mathcal{B}(H \to SS)=100\%$ and each S has a 50% probability of decaying to two electrons. The area above the solid (dashed) curves represents the observed (expected) exclusion region.
The 95% CL upper limits on the $\mathrm{H} \to \mathrm{S}\mathrm{S} \to 4\ell$ branching fraction as a function of $c\tau_0$, for a Higgs boson with a mass of 125 GeV and a long-lived scalar with a mass of 30 GeV or 50 GeV, for the $\mu\mu$ channel only. These limits assume that $\mathcal{B}(H \to SS)=100\%$ and each S has a 50% probability of decaying to two muons. The area above the solid (dashed) curve represents the observed (expected) exclusion region.
The 95% CL upper limits on the product of the cross section and branching fraction $\mathrm{H} \to \mathrm{S}\mathrm{S} \to 4\ell$ as a function of $c\tau_0$, for a 600 GeV Higgs boson and several long-lived scalar masses, for the $\mu\mu$ channel only. These limits assume that $\mathcal{B}(H \to SS)=100\%$ and each S has a 50% probability of decaying to two muons. The area above the solid (dashed) curves represents the observed (expected) exclusion region.
The 95% CL upper limits on the product of the cross section and branching fraction $\mathrm{H} \to \mathrm{S}\mathrm{S} \to 4\ell$ as a function of $c\tau_0$, for a 1000 GeV Higgs boson and several long-lived scalar masses, for the $\mu\mu$ channel only. These limits assume that $\mathcal{B}(H \to SS)=100\%$ and each S has a 50% probability of decaying to two muons. The area above the solid (dashed) curves represents the observed (expected) exclusion region.
Collinear (small-angle) and large-angle, as well as soft and hard radiations are investigated in three-jet and Z + two-jet events collected in proton-proton collisions at the LHC. The normalized production cross sections are measured as a function of the ratio of transverse momenta of two jets and their angular separation. The measurements in the three-jet and Z + two-jet events are based on data collected at a center-of-mass energy of 8 TeV, corresponding to an integrated luminosity of 19.8 fb$^{-1}$. The Z + two-jet events are reconstructed in the dimuon decay channel of the Z boson. The three-jet measurement is extended to include $\sqrt{s} =$ 13 TeV data corresponding to an integrated luminosity of 2.3 fb$^{-1}$. The results are compared to predictions from event generators that include parton showers, multiple parton interactions, and hadronization. The collinear and soft regions are in general well described by parton showers, whereas the regions of large angular separation are often best described by calculations using higher-order matrix elements.
Three-jet events $p_{\mathrm{T}3}/p_{\mathrm{T}2}$ for small-angle radiation ($\Delta R_{23}$ < 1.0)
Three-jet events $p_{\mathrm{T}3}/p_{\mathrm{T}2}$ for small-angle radiation ($\Delta R_{23}$ < 1.0)
Three-jet events $p_{\mathrm{T}3}/p_{\mathrm{T}2}$ for large-angle radiation ($\Delta R_{23}$ > 1.0)
Three-jet events $p_{\mathrm{T}3}/p_{\mathrm{T}2}$ for large-angle radiation ($\Delta R_{23}$ > 1.0)
Three-jet events $\Delta R_{23}$ for soft radiation ($p_{\mathrm{T}3}/p_{\mathrm{T}2}$ < 0.3)
Three-jet events $\Delta R_{23}$ for soft radiation ($p_{\mathrm{T}3}/p_{\mathrm{T}2}$ < 0.3)
Three-jet events $\Delta R_{23}$ for hard radiation ($p_{\mathrm{T}3}/p_{\mathrm{T}2}$ > 0.6)
Three-jet events $\Delta R_{23}$ for hard radiation ($p_{\mathrm{T}3}/p_{\mathrm{T}2}$ > 0.6)
Three-jet events $p_{\mathrm{T}3}/p_{\mathrm{T}2}$ for small-angle radiation ($\Delta R_{23}$ < 1.0)
Three-jet events $p_{\mathrm{T}3}/p_{\mathrm{T}2}$ for small-angle radiation ($\Delta R_{23}$ < 1.0)
Three-jet events $p_{\mathrm{T}3}/p_{\mathrm{T}2}$ for large-angle radiation ($\Delta R_{23}$ > 1.0)
Three-jet events $p_{\mathrm{T}3}/p_{\mathrm{T}2}$ for large-angle radiation ($\Delta R_{23}$ > 1.0)
Three-jet events $\Delta R_{23}$ for soft radiation ($p_{\mathrm{T}3}/p_{\mathrm{T}2}$ < 0.3)
Three-jet events $\Delta R_{23}$ for soft radiation ($p_{\mathrm{T}3}/p_{\mathrm{T}2}$ < 0.3)
Three-jet events $\Delta R_{23}$ for hard radiation ($p_{\mathrm{T}3}/p_{\mathrm{T}2}$ > 0.6)
Three-jet events $\Delta R_{23}$ for hard radiation ($p_{\mathrm{T}3}/p_{\mathrm{T}2}$ > 0.6)
Z + two-jet events $p_{\mathrm{T}3}/p_{\mathrm{T}2}$ for small-angle radiation ($\Delta R_{23}$ < 1.0)
Z + two-jet events $p_{\mathrm{T}3}/p_{\mathrm{T}2}$ for small-angle radiation ($\Delta R_{23}$ < 1.0)
Z + two-jet events $p_{\mathrm{T}3}/p_{\mathrm{T}2}$ for large-angle radiation ($\Delta R_{23}$ > 1.0)
Z + two-jet events $p_{\mathrm{T}3}/p_{\mathrm{T}2}$ for large-angle radiation ($\Delta R_{23}$ > 1.0)
Z + two-jet events $\Delta R_{23}$ for soft radiation ($p_{\mathrm{T}3}/p_{\mathrm{T}2}$ < 0.3)
Z + two-jet events $\Delta R_{23}$ for soft radiation ($p_{\mathrm{T}3}/p_{\mathrm{T}2}$ < 0.3)
Z + two-jet events $\Delta R_{23}$ for hard radiation ($p_{\mathrm{T}3}/p_{\mathrm{T}2}$ > 0.6)
Z + two-jet events $\Delta R_{23}$ for hard radiation ($p_{\mathrm{T}3}/p_{\mathrm{T}2}$ > 0.6)
Double-parton scattering is investigated using events with a Z boson and jets. The Z boson is reconstructed using only the dimuon channel. The measurements are performed with proton-proton collision data recorded by the CMS experiment at the LHC at $\sqrt{s} =$ 13 TeV, corresponding to an integrated luminosity of 35.9 fb$^{-1}$ collected in the year 2016. Differential cross sections of Z + $\geq$ 1 jet and Z + $\geq$ 2 jets are measured with transverse momentum of the jets above 20 GeV and pseudorapidity $|\eta|$$\lt$ 2.4. Several distributions with sensitivity to double-parton scattering effects are measured as functions of the angle and the transverse momentum imbalance between the Z boson and the jets. The measured distributions are compared with predictions from several event generators with different hadronization models and different parameter settings for multiparton interactions. The measured distributions show a dependence on the hadronization and multiparton interaction simulation parameters, and are important input for future improvements of the simulations.
Differential cross sections as function of Delta Phi between Z boson and the leading jet for Z+ ≥ 1 jet events.
Differential cross sections as function of transverse momentum imbalance between Z boson and the leading jet for Z+ ≥ 1 jet events.
Differential cross sections as function of Delta Phi between Z boson and dijet for Z+ ≥ 2 jets events.
Differential cross sections as function of transverse momentum imbalance between Z boson and dijet for Z+ ≥ 2 jets events.
Differential cross sections as function of transverse momentum imbalance between leading and subleading jet for Z+ ≥ 2 jets events.
Area normalized distribution as function of Delta Phi between Z boson and the leading jet for Z+ ≥ 1 jet events.
Area normalized distribution as function of transverse momentum imbalance between Z boson and the leading jet for Z+ ≥ 1 jet events.
Area normalized distribution as function of Delta Phi between Z boson and dijet for Z+ ≥ 2 jets events.
Area normalized distribution as function of transverse momentum imbalance between Z boson and dijet for Z+ ≥ 2 jets events.
Area normalized distribution as function of transverse momentum imbalance between leading and subleading jet for Z+ ≥ 2 jets events
Response matrix for Delta Phi between Z boson and the leading jet for Z+ ≥ 1 jet events.
Response matrix for transverse momentum imbalance between Z boson and the leading jet for Z+ ≥ 1 jet events.
Response matrix for Delta Phi between Z boson and dijet for Z+ ≥ 2 jets events.
Response matrix for transverse momentum imbalance between Z boson and dijet for Z+ ≥ 2 jets events.
Response matrix for transverse momentum imbalance between the leading jet and subleading jet for Z+ ≥ 2 jets events.
Correlation matrix for Delta Phi between Z boson and the leading jet for Z+ ≥ 1 jet events (for absolute differential cross section measurements).
Correlation matrix for transverse momentum imbalance between Z boson and the leading jet for Z+ ≥ 1 jet events (for absolute differential cross section measurements).
Correlation matrix for Delta Phi between Z boson and dijet for Z+ ≥ 2 jets events (for absolute differential cross section measurements).
Correlation matrix for transverse momentum imbalance between Z boson and dijet for Z+ ≥ 2 jets events (for absolute differential cross section measurements).
Correlation matrix for transverse momentum imbalance between the leading jet and subleading jet for Z+ ≥ 2 jets events (for absolute differential cross section measurements).
Correlation matrix for Delta Phi between Z boson and the leading jet for Z+ ≥ 1 jet events (for normalized differential cross section measurements).
Correlation matrix for transverse momentum imbalance between Z boson and the leading jet for Z+ ≥ 1 jet events (for normalized differential cross section measurements).
Correlation matrix for Delta Phi between Z boson and dijet for Z+ ≥ 2 jets events (for normalized differential cross section measurements).
Correlation matrix for transverse momentum imbalance between Z boson and dijet for Z+ ≥ 2 jets events (for normalized differential cross section measurements).
Correlation matrix for transverse momentum imbalance between the leading jet and subleading jet for Z+ ≥ 2 jets events (for normalized differential cross section measurements).
A search for invisible decays of the Higgs boson produced via vector boson fusion (VBF) has been performed with 101 fb$^{-1}$ of proton-proton collisions delivered by the LHC at $\sqrt{s} =$ 13 TeV and collected by the CMS detector in 2017 and 2018. The sensitivity to the VBF production mechanism is enhanced by constructing two analysis categories, one based on missing transverse momentum, and a second based on the properties of jets. In addition to control regions with Z and W boson candidate events, a highly populated control region, based on the production of a photon in association with jets, is used to constrain the dominant irreducible background from the invisible decay of a Z boson produced in association with jets. The results of this search are combined with all previous measurements in the VBF topology, based on data collected in 2012 (at $\sqrt{s} =$ 8 TeV), 2015, and 2016, corresponding to integrated luminosities of 19.7, 2.3, and 36.3 fb$^{-1}$, respectively. The observed (expected) upper limit on the invisible branching fraction of the Higgs boson is found to be 0.18 (0.10) at the 95% confidence level, assuming the standard model production cross section. The results are also interpreted in the context of Higgs-portal models.
Observed and expected 95% CL upper limits on ${{(\sigma_{\text{H}}/\sigma_{\text{H}}^{\mathrm{SM}}) \times {{\mathcal{B}(\text{H} \to \text{inv})}}}}$ for all three years of data taking, as well as their combination, assuming a SM Higgs boson with a mass of 125.38GeV.
The 90% CL upper limits on the spin-independent DM-nucleon scattering cross section in Higgs-portal models, assuming a scalar or fermion DM candidate.
Expected event yields in each $m_{jj}$ bin for the different background processes in the SR of the MTR category, in the 2017 and 2018 samples. The background yields and the corresponding uncertainties are obtained after performing a combined fit across all of the CRs and SR. The expected signal contributions for a Higgs boson, produced in the non-VBF and VBF modes, decaying to invisible particles with a branching fraction of $\mathcal{B}(\text{H} \to \text{inv}) = 1$, and the observed event yields are also reported.
Expected event yields in each $m_{jj}$ bin for the different background processes in the SR of the VTR category, in the 2017 and 2018 samples. The background yields and the corresponding uncertainties are obtained after performing a combined fit across all of the CRs and SR. The expected signal contributions for a Higgs boson, produced in the non-VBF and VBF modes, decaying to invisible particles with a branching fraction of $\mathcal{B}(\text{H} \to \text{inv}) = 1$, and the observed event yields are also reported.
Event yields for the postfit background model from the background-only and signal-plus-background fits, as well as the observed event yields for MTR, 2017, signal region. All signal and control regions from the 2017 and 2018 data sets are included in the fit.
Event yields for the postfit background model from the background-only and signal-plus-background fits, as well as the observed event yields for MTR, 2017, dimuon region. All signal and control regions from the 2017 and 2018 data sets are included in the fit.
Event yields for the postfit background model from the background-only and signal-plus-background fits, as well as the observed event yields for MTR, 2018, signal region. All signal and control regions from the 2017 and 2018 data sets are included in the fit.
Event yields for the postfit background model from the background-only and signal-plus-background fits, as well as the observed event yields for MTR, 2018, dimuon region. All signal and control regions from the 2017 and 2018 data sets are included in the fit.
Event yields for the postfit background model from the background-only and signal-plus-background fits, as well as the observed event yields for VTR, 2017, signal region. All signal and control regions from the 2017 and 2018 data sets are included in the fit.
Event yields for the postfit background model from the background-only and signal-plus-background fits, as well as the observed event yields for VTR, 2017, dimuon region. All signal and control regions from the 2017 and 2018 data sets are included in the fit.
Event yields for the postfit background model from the background-only and signal-plus-background fits, as well as the observed event yields for VTR, 2018, signal region. All signal and control regions from the 2017 and 2018 data sets are included in the fit.
Event yields for the postfit background model from the background-only and signal-plus-background fits, as well as the observed event yields for VTR, 2018, single electron region. All signal and control regions from the 2017 and 2018 data sets are included in the fit.
Event yields for the postfit background model from the background-only and signal-plus-background fits, as well as the observed event yields for VTR, 2018, dielectron region. All signal and control regions from the 2017 and 2018 data sets are included in the fit.
Event yields for the postfit background model from the background-only and signal-plus-background fits, as well as the observed event yields for VTR, 2018, dimuon region. All signal and control regions from the 2017 and 2018 data sets are included in the fit.
Event yields for the postfit background model from the background-only and signal-plus-background fits, as well as the observed event yields for MTR, 2017, photon region. All signal and control regions from the 2017 and 2018 data sets are included in the fit.
Event yields for the postfit background model from the background-only and signal-plus-background fits, as well as the observed event yields for MTR, 2018, photon region. All signal and control regions from the 2017 and 2018 data sets are included in the fit.
Event yields for the postfit background model from the background-only and signal-plus-background fits, as well as the observed event yields for MTR, 2017, single electron region. All signal and control regions from the 2017 and 2018 data sets are included in the fit.
Event yields for the postfit background model from the background-only and signal-plus-background fits, as well as the observed event yields for MTR, 2017, single muon region. All signal and control regions from the 2017 and 2018 data sets are included in the fit.
Event yields for the postfit background model from the background-only and signal-plus-background fits, as well as the observed event yields for MTR, 2017, dielectron region. All signal and control regions from the 2017 and 2018 data sets are included in the fit.
Event yields for the postfit background model from the background-only and signal-plus-background fits, as well as the observed event yields for MTR, 2018, single electron region. All signal and control regions from the 2017 and 2018 data sets are included in the fit.
Event yields for the postfit background model from the background-only and signal-plus-background fits, as well as the observed event yields for MTR, 2018, single muon region. All signal and control regions from the 2017 and 2018 data sets are included in the fit.
Event yields for the postfit background model from the background-only and signal-plus-background fits, as well as the observed event yields for MTR, 2018, dielectron region. All signal and control regions from the 2017 and 2018 data sets are included in the fit.
Event yields for the postfit background model from the background-only and signal-plus-background fits, as well as the observed event yields for VTR, 2017, single electron region. All signal and control regions from the 2017 and 2018 data sets are included in the fit.
Event yields for the postfit background model from the background-only and signal-plus-background fits, as well as the observed event yields for VTR, 2017, single muon region. All signal and control regions from the 2017 and 2018 data sets are included in the fit.
Event yields for the postfit background model from the background-only and signal-plus-background fits, as well as the observed event yields for VTR, 2017, dielectron region. All signal and control regions from the 2017 and 2018 data sets are included in the fit.
Event yields for the postfit background model from the background-only and signal-plus-background fits, as well as the observed event yields for VTR, 2018, single muon region. All signal and control regions from the 2017 and 2018 data sets are included in the fit.
Trigger efficiency measured as a function of $p_{T}^{miss}$ in data for the 2017 and 2018 samples for the MTR category. The efficiency is measured in a phase space with at least two jets in which the leading (trailing) jet has $p_{T}>80~\text{GeV}$ ($>40~\text{GeV}$). The two jets are required to form a system with $m_{jj}>200~\text{GeV}$ and $\Delta\Phi_{jj}<1.5$.
Trigger efficiency measured as a function of $p_{T}^{miss}$ in data for the 2017 and 2018 samples for the MTR category. The efficiency is measured in a phase space with at least two jets in which the leading (trailing) jet has $p_{T}>140~\text{GeV}$ ($>70~\text{GeV}$). The two jets are required to form a system with $m_{jj}>900~\text{GeV}$ and $\Delta\Phi_{jj}<1.8$.
The transverse momentum ($p_\mathrm{T}$) distributions of $\Lambda$, $\Xi^-$, and $\Omega^-$ baryons, their antiparticles, and K$^0_\mathrm{S}$ mesons are measured in proton-proton (pp) and proton-lead (pPb) collisions at a nucleon-nucleon center-of-mass energy of 5.02 TeV over a broad rapidity range. The data, corresponding to integrated luminosities of 40.2 nb$^{-1}$ and 15.6 $\mu$b$^{-1}$ for pp and pPb collisions, respectively, were collected by the CMS experiment. The nuclear modification factor $R_\mathrm{pPb}$, defined as the ratio of the particle yield in pPb collisions and a scaled pp reference, is measured for each particle. A strong dependence on particle species is observed in the $p_\mathrm{T}$ range from 2 to 7 GeV, where $R_\mathrm{pPb}$ for K$^0_\mathrm{S}$ is consistent with unity, while an enhancement ordered by strangeness content and/or particle mass is observed for the three baryons. In pPb collisions, the strange hadron production is asymmetric about the nucleon-nucleon center-of-mass rapidity. Enhancements, which depend on the particle type, are observed in the direction of the Pb beam. The results are compared to predictions from EPOS LHC, which includes parametrized radial flow. The model is in qualitative agreement with the $R_\mathrm{pPb}$ data, but fails to describe the dependence on particle species in the yield asymmetries measured away from mid-rapidity in pPb collisions.
Invariant $p_{T}$-differential spectra of ${K_{0}}^{S}$ in p+p and p+Pb at $\sqrt{s}$=5.02 TeV in various |$y_{CM}$| ranges
Invariant $p_{T}$-differential spectra of ${K_{0}}^{S}$ in p+p and p+Pb at $\sqrt{s}$=5.02 TeV in various $y_{CM}$ ranges
Invariant $p_{T}$-differential spectra of $\Lambda + \bar{\Lambda}$ in p+p and p+Pb at $\sqrt{s}$=5.02 TeV in various |$y_{CM}$| ranges
Invariant $p_{T}$-differential spectra of $\Lambda + \bar{\Lambda}$ in p+p and p+Pb at $\sqrt{s}$=5.02 TeV in various $y_{CM}$ ranges
Invariant $p_{T}$-differential spectra of $\Xi- + \bar{\Xi+}$ in p+p and p+Pb at $\sqrt{s}$=5.02 TeV in various |$y_{CM}$| ranges
Invariant $p_{T}$-differential spectra of $\Xi- + \bar{\Xi+}$ in p+p and p+Pb at $\sqrt{s}$=5.02 TeV in various $y_{CM}$ ranges
Invariant $p_{T}$-differential spectra of $\Omega- + \bar{\Omega+}$ in p+p and p+Pb at $\sqrt{s}$=5.02 TeV in |$y_{CM}$| < 1.8
Invariant $p_{T}$-differential spectra of $\Omega- + \bar{\Omega+}$ in p+p and p+Pb at $\sqrt{s}$=5.02 TeV in |$y_{CM}$| < 1.8
$R_{pPb}$ in p+Pb at $\sqrt{s}$=5.02 TeV in |$y_{CM}$| < 1.8
$R_{pPb}$ in p+Pb at $\sqrt{s}$=5.02 TeV in |$y_{CM}$| < 1.8
$R_{pPb}$ in p+Pb at $\sqrt{s}$=5.02 TeV in -1.8 < $y_{CM}$ < 0
$R_{pPb}$ in p+Pb at $\sqrt{s}$=5.02 TeV in |$y_{CM}$| < 1.8
$R_{pPb}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 0 < $y_{CM}$ < 1.8
$R_{pPb}$ in p+Pb at $\sqrt{s}$=5.02 TeV in |$y_{CM}$| < 1.8
Invariant $p_{T}$-differential spectra of ${K_{0}}^{S}$ in p+Pb at $\sqrt{s}$=5.02 TeV in various $y_{CM}$ ranges
$R_{pPb}$ in p+Pb at $\sqrt{s}$=5.02 TeV in |$y_{CM}$| < 1.8
Invariant $p_{T}$-differential spectra of $\Lambda + \bar{\Lambda}$ in p+Pb at $\sqrt{s}$=5.02 TeV in various $y_{CM}$ ranges
$R_{pPb}$ in p+Pb at $\sqrt{s}$=5.02 TeV in -1.8 < $y_{CM}$ < 0
$Y_{asym}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 0.3 < $y_{CM}$ < 0.8
$R_{pPb}$ in p+Pb at $\sqrt{s}$=5.02 TeV in -1.8 < $y_{CM}$ < 0
$Y_{asym}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 0.8 < $y_{CM}$ < 1.3
$R_{pPb}$ in p+Pb at $\sqrt{s}$=5.02 TeV in -1.8 < $y_{CM}$ < 0
$Y_{asym}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 1.3 < $y_{CM}$ < 1.8
$R_{pPb}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 0 < $y_{CM}$ < 1.8
$R_{pPb}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 0 < $y_{CM}$ < 1.8
$R_{pPb}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 0 < $y_{CM}$ < 1.8
Invariant $p_{T}$-differential spectra of ${K_{0}}^{S}$ in p+Pb at $\sqrt{s}$=5.02 TeV in various $y_{CM}$ ranges
Invariant $p_{T}$-differential spectra of $\Lambda + \bar{\Lambda}$ in p+Pb at $\sqrt{s}$=5.02 TeV in various $y_{CM}$ ranges
$Y_{asym}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 0.3 < |$y_{CM}$| < 0.8
$Y_{asym}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 0.3 < |$y_{CM}$| < 0.8
$Y_{asym}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 0.3 < |$y_{CM}$| < 0.8
$Y_{asym}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 0.8 < |$y_{CM}$| < 1.3
$Y_{asym}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 0.8 < |$y_{CM}$| < 1.3
$Y_{asym}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 0.8 < |$y_{CM}$| < 1.3
$Y_{asym}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 1.3 < |$y_{CM}$| < 1.8
$Y_{asym}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 1.3 < |$y_{CM}$| < 1.8
$Y_{asym}$ in p+Pb at $\sqrt{s}$=5.02 TeV in 1.3 < |$y_{CM}$| < 1.8
Protons consist of three valence quarks, two up-quarks and one down-quark, held together by gluons and a sea of quark-antiquark pairs. Collectively, quarks and gluons are referred to as partons. In a proton-proton collision, typically only one parton of each proton undergoes a hard scattering - referred to as single-parton scattering - leaving the remainder of each proton only slightly disturbed. Here, we report the study of double- and triple-parton scatterings through the simultaneous production of three J/$\psi$ mesons, which consist of a charm quark-antiquark pair, in proton-proton collisions recorded with the CMS experiment at the Large Hadron Collider. We observed this process - reconstructed through the decays of J/$\psi$ mesons into pairs of oppositely charged muons - with a statistical significance above five standard deviations. We measured the inclusive fiducial cross section to be 272 $^{+141}_{-104}$ (stat) $\pm$ 17 (syst) fb, and compared it to theoretical expectations for triple-J/$\psi$ meson production in single-, double- and triple-parton scattering scenarios. Assuming factorization of multiple hard-scattering probabilities in terms of single-parton scattering cross sections, double- and triple-parton scattering are the dominant contributions for the measured process.
Kinematic properties of each one of the three \JPsi mesons selected in the 5? 6? signal events.
Dimuon invariant mass ($m$), proper decay-length ($L$), transverse momentum ($p_{T}$), rapidity ($y$), and azimuthal angle ($\phi$) of each of the three $J/\psi$ candidates measured in the six triple-$J/\psi$ events passing our selection criteria.
DPS effective cross section
Measured DPS effective cross section
pp -> J/psi J/psi J/psi X cross section
$pp \rightarrow J/\psi J/\psi J/\psi X~$ fiducial cross section
Evidence is reported for electroweak (EW) vector boson scattering in the decay channel $\ell\nu$qq of two weak vector bosons WV (V = W or Z), produced in association with two parton jets. The search uses a data set of proton-proton collisions at 13 TeV collected with the CMS detector during 2016-2018 with an integrated luminosity of 138 fb$^{-1}$. Events are selected requiring one lepton (electron or muon), moderate missing transverse momentum, two jets with a large pseudorapidity separation and a large dijet invariant mass, and a signature consistent with the hadronic decay of a W/Z boson. The cross section is computed in a fiducial phase space defined at parton level requiring all parton transverse momenta $p_\mathrm{T}$$\gt$ 10 GeV and at least one pair of outgoing partons with invariant mass $m_\mathrm{qq}$$\gt$ 100 GeV. The measured and expected EW WV production cross sections are 1.90 $^{+0.53}_{-0.46}$ pb and 2.23 $^{+0.08}_{-0.11}$ (scale) $\pm$ 0.05 (PDF) pb, respectively, where PDF is the parton distribution function. The observed EW signal strength is $m_\mathrm{EW}$ = 0.85 $\pm$ 0.12 (stat) $^{+0.19}_{-0.17}$ (syst), corresponding to a signal significance of 4.4 standard deviations with 5.1 expected, and it is measured keeping the quantum chromodynamics (QCD) associated diboson production fixed to the standard model prediction. This is the first evidence of vector boson scattering in the $\ell\nu$qq decay channel at LHC. The simultaneous measurement of the EW and QCD associated diboson production agrees with the standard model prediction.
Expected and observed cross sections for EW and EW+QCD WV production in association with 2 jets. Two separate maximum likelihood fits are performed: the measurement of the purely EW signal strength μ_EW keeping the QCD WV production contribution fixed to the SM prediction μQCD = 1; the measurement of the signal strength considering as signal the EW and QCD WV processes together.
Invariant mass of the pair of the VBS tag jets in the resolved category. The last bin contains overflow events.
Invariant mass of the pair of the VBS tag jets in the boosted category. The last bin contains overflow events.
Simultaneous EW and QCD WV signal strength fit.
Measurements of Higgs boson production, where the Higgs boson decays into a pair of $\tau$ leptons, are presented, using a sample of proton-proton collisions collected with the CMS experiment at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 fb$^{-1}$. Three analyses are presented. Two are targeting Higgs boson production via gluon fusion and vector boson fusion: a neural network based analysis and an analysis based on an event categorization optimized on the ratio of signal over background events. These are complemented by an analysis targeting vector boson associated Higgs boson production. Results are presented in the form of signal strengths relative to the standard model predictions and products of cross sections and branching fraction to $\tau$ leptons, in up to 16 different kinematic regions. For the simultaneous measurements of the neural network based analysis and the analysis targeting vector boson associated Higgs boson production signal strengths are found to be 0.82 $\pm$ 0.11 for inclusive Higgs boson production, 0.67 $\pm$ 0.19 (0.81 $\pm$ 0.17) for the production mainly via gluon fusion (vector boson fusion), and 1.79 $\pm$ 0.45 for vector boson associated Higgs boson production.
Measurements of the signal strengths for inclusive H production ($\mu_{\text{incl}}$) and the ggH ($\mu_{\text{ggH}}$), qqH ($\mu_{\text{qqH}}$), and VH ($\mu_{\text{VH}}$) STXS stage-0 processes, for the combination of the NN- and VH-analyses. Central values maximizing the likelihood and a split of uncertainties are provided with each result.
Measurements of the signal strengths for inclusive H production ($\mu_{\text{incl}}$) and the ggH ($\mu_{\text{ggH}}$), qqH ($\mu_{\text{qqH}}$), and VH ($\mu_{\text{VH}}$) STXS stage-0 processes, for the combination of the CB- and VH-analyses. Central values maximizing the likelihood and a split of uncertainties are provided with each result.
Measurements of the signal strengths $\mu_{\text{s}}$ in the STXS stage-1.2 bins for the ggH, qqH, and VH processes, for the combination of the NN- and VH-analyses. Central values and a split of uncertainties are also provided with each result.
Measurements of the signal strengths $\mu_{\text{s}}$ in the STXS stage-1.2 bins for the ggH, qqH, and VH processes, for the combination of the CB- and VH-analyses. Central values and a split of uncertainties are also provided with each result.
Correlation matrix of the POIs of the measured STXS stage-1.2 signal strengths for the combination of the NN- an VH-analyses.
Correlation matrix of the POIs of the measured STXS stage-1.2 signal strengths for the combination of the CB- an VH-analyses.
Cross section measurements in the STXS stage-0 bins for the combination of the NN- and VH-analyses. Central values and combined statistical and systematic uncertainties are given for each measurement.
Cross section measurements in the STXS stage-1.2 bins for the combination of the NN- and VH-analyses. Central values and combined statistical and systematic uncertainties are given for each measurement.
Cross section measurements in the STXS stage-0 bins for the combination of the CB- and VH-analyses. Central values and combined statistical and systematic uncertainties are given for each measurement.
Cross section measurements in the STXS stage-1.2 bins for the combination of the CB- and VH-analyses. Central values and combined statistical and systematic uncertainties are given for each measurement.
The measurement of the charge asymmetry in top quark pair events with highly Lorentz-boosted top quarks decaying to a single lepton and jets is presented. The analysis is performed using proton-proton collisions at $\sqrt{s}$ = 13 TeV with the CMS detector at the LHC and corresponding to an integrated luminosity of 138 fb$^{-1}$. The selection is optimized for top quarks produced with large Lorentz boosts, resulting in nonisolated leptons and overlapping jets. The top quark charge asymmetry is measured for events with a $\mathrm{t\bar{t}}$ invariant mass larger than 750 GeV and corrected for detector and acceptance effects using a binned maximum likelihood fit. The measured top quark charge asymmetry of (0.42 $_{-0.69}^{+0.64}$)% is in good agreement with the standard model prediction at next-to-next-to-leading order in quantum chromodynamic perturbation theory with next-to-leading-order electroweak corrections. The result is also presented for two invariant mass ranges, 750-900 and $\gt$ 900 GeV.
Comparison between data and MC simulation for kinematic distributions based on events in the signal candidate sample for the distance between the lepton and the closest AK4 jet. The vertical bars on the points show the statistical uncertainty in the data. The shaded bands represent the total uncertainty in the MC predictions. The lower panels give the ratio of the data to the sum of the MC
Comparison between data and MC simulation for kinematic distributions based on events in the signal candidate sample for the number of AK4 jets. The vertical bars on the points show the statistical uncertainty in the data. The shaded bands represent the total uncertainty in the MC predictions. The lower panels give the ratio of the data to the sum of the MC
Comparison between data and MC simulation for kinematic distributions based on events in the signal candidate sample for the reconstruced mass of the top quark pairs. The vertical bars on the points show the statistical uncertainty in the data. The shaded bands represent the total uncertainty in the MC predictions. The lower panels give the ratio of the data to the sum of the MC
Comparison between data and MC simulation for kinematic distributions based on events in the signal candidate sample for \Delta|y|. The vertical bars on the points show the statistical uncertainty in the data. The shaded bands represent the total uncertainty in the MC predictions. The lower panels give the ratio of the data to the sum of the MC
Comparison between data and MC simulation for \Delta|y| for each of the 12 analysis channels for the low mass region prior to maximum likelihood fit. The vertical bars on the points show the statistical uncertainty in the data. The shaded bands represent the total uncertainty in the MC predictions. The lower panels give the ratio of the data to the sum of the MC
Comparison between data and MC simulation for \Delta|y| for each of the 12 analysis channels for the low mass region after the maximum likelihood fit. The vertical bars on the points show the statistical uncertainty in the data. The shaded bands represent the total uncertainty in the MC predictions. The lower panels give the ratio of the data to the sum of the MC
Comparison between data and MC simulation for \Delta|y| for each of the 12 analysis channels for the high mass region prior to the maximum likelihood fit. The vertical bars on the points show the statistical uncertainty in the data. The shaded bands represent the total uncertainty in the MC predictions. The lower panels give the ratio of the data to the sum of the MC
Comparison between data and MC simulation for \Delta|y| for each of the 12 analysis channels for the high mass region after the maximum likelihood fit. The vertical bars on the points show the statistical uncertainty in the data. The shaded bands represent the total uncertainty in the MC predictions. The lower panels give the ratio of the data to the sum of the MC
Measured A_{C}^{fid} in different mass regions after combining the two lepton channels. The vertical bars on the points show the statistical uncertainty in the data
Measured A_{C} in the full phase space in different mass regions after combining the two lepton channels. The vertical bars on the points show the statistical uncertainty in the data
The +/- standard deviation (\sigma) impacts of the nuisance parameters corresponding to the systematic uncertainties in the full phase space A_{C} measurement for mttbar > 750GeV. The red and blue bars show the effect on the unfolded AC values for up and down variations of the systematic uncertainty. The MC statistical uncertainties are omitted here.
Measurements of jet substructure describing the composition of quark- and gluon-initiated jets are presented. Proton-proton (pp) collision data at $\sqrt{s}$ =13 TeV collected with the CMS detector are used, corresponding to an integrated luminosity of 35.9 fb$^{-1}$. Generalized angularities are measured that characterize the jet substructure and distinguish quark- and gluon-initiated jets. These observables are sensitive to the distributions of transverse momenta and angular distances within a jet. The analysis is performed using a data sample of dijet events enriched in gluon-initiated jets, and, for the first time, a Z+jet event sample enriched in quark-initiated jets. The observables are measured in bins of jet transverse momentum, and as a function of the jet radius parameter. Each measurement is repeated applying a "soft drop" grooming procedure that removes soft and large angle radiation from the jet. Using these measurements, the ability of various models to describe jet substructure is assessed, showing a clear need for improvements in Monte Carlo generators.
Mean of ungroomed LHA for AK4 jets as a function of PT in the central dijet region.
Mean of ungroomed LHA for AK4 jets as a function of PT in the forward dijet region.
Mean of ungroomed LHA (charged-only) for AK4 jets as a function of PT in the central dijet region.
Mean of ungroomed LHA (charged-only) for AK4 jets as a function of PT in the forward dijet region.
Mean of ungroomed multiplicity (charged-only) for AK4 jets as a function of PT in the Z+jet region.
Mean of ungroomed multiplicity (charged-only) for AK4 jets as a function of PT in the central dijet region.
Mean of ungroomed multiplicity (charged-only) for AK4 jets as a function of PT in the forward dijet region.
Mean of ungroomed pTD2 (charged-only) for AK4 jets as a function of PT in the Z+jet region.
Mean of ungroomed pTD2 (charged-only) for AK4 jets as a function of PT in the central dijet region.
Mean of ungroomed thrust (charged-only) for AK4 jets as a function of PT in the Z+jet region.
Mean of ungroomed thrust (charged-only) for AK4 jets as a function of PT in the forward dijet region.
Mean of ungroomed width (charged-only) for AK4 jets as a function of PT in the Z+jet region.
Mean of ungroomed width (charged-only) for AK4 jets as a function of PT in the central dijet region.
Mean of ungroomed width (charged-only) for AK4 jets as a function of PT in the forward dijet region.
Mean of ungroomed multiplicity for AK4 jets as a function of PT in the Z+jet region.
Mean of ungroomed multiplicity for AK4 jets as a function of PT in the central dijet region.
Mean of ungroomed pTD2 for AK4 jets as a function of PT in the Z+jet region.
Mean of ungroomed pTD2 for AK4 jets as a function of PT in the central dijet region.
Mean of ungroomed pTD2 for AK4 jets as a function of PT in the forward dijet region.
Mean of ungroomed thrust for AK4 jets as a function of PT in the Z+jet region.
Mean of ungroomed thrust for AK4 jets as a function of PT in the central dijet region.
Mean of ungroomed thrust for AK4 jets as a function of PT in the forward dijet region.
Mean of ungroomed width for AK4 jets as a function of PT in the Z+jet region.
Mean of ungroomed width for AK4 jets as a function of PT in the central dijet region.
Mean of ungroomed width for AK4 jets as a function of PT in the forward dijet region.
Mean of groomed LHA for AK4 jets as a function of PT in the Z+jet region.
Mean of groomed LHA for AK4 jets as a function of PT in the central dijet region.
Mean of groomed LHA for AK4 jets as a function of PT in the forward dijet region.
Mean of groomed LHA (charged-only) for AK4 jets as a function of PT in the Z+jet region.
Mean of groomed LHA (charged-only) for AK4 jets as a function of PT in the central dijet region.
Mean of groomed LHA (charged-only) for AK4 jets as a function of PT in the forward dijet region.
Mean of groomed multiplicity (charged-only) for AK4 jets as a function of PT in the central dijet region.
Mean of groomed multiplicity (charged-only) for AK4 jets as a function of PT in the forward dijet region.
Mean of groomed pTD2 (charged-only) for AK4 jets as a function of PT in the central dijet region.
Mean of groomed pTD2 (charged-only) for AK4 jets as a function of PT in the forward dijet region.
Mean of groomed thrust (charged-only) for AK4 jets as a function of PT in the central dijet region.
Mean of groomed thrust (charged-only) for AK4 jets as a function of PT in the forward dijet region.
Mean of groomed width (charged-only) for AK4 jets as a function of PT in the Z+jet region.
Mean of groomed width (charged-only) for AK4 jets as a function of PT in the central dijet region.
Mean of groomed width (charged-only) for AK4 jets as a function of PT in the forward dijet region.
Mean of groomed multiplicity for AK4 jets as a function of PT in the Z+jet region.
Mean of groomed multiplicity for AK4 jets as a function of PT in the central dijet region.
Mean of groomed multiplicity for AK4 jets as a function of PT in the forward dijet region.
Mean of groomed pTD2 for AK4 jets as a function of PT in the Z+jet region.
Mean of groomed pTD2 for AK4 jets as a function of PT in the central dijet region.
Mean of groomed pTD2 for AK4 jets as a function of PT in the forward dijet region.
Mean of groomed thrust for AK4 jets as a function of PT in the Z+jet region.
Mean of groomed thrust for AK4 jets as a function of PT in the central dijet region.
Mean of groomed thrust for AK4 jets as a function of PT in the forward dijet region.
Mean of groomed width for AK4 jets as a function of PT in the Z+jet region.
Mean of groomed width for AK4 jets as a function of PT in the central dijet region.
Mean of groomed width for AK4 jets as a function of PT in the forward dijet region.
Mean of ungroomed LHA for AK8 jets as a function of PT in the Z+jet region.
Mean of ungroomed LHA for AK8 jets as a function of PT in the central dijet region.
Mean of ungroomed LHA for AK8 jets as a function of PT in the forward dijet region.
Mean of ungroomed LHA (charged-only) for AK8 jets as a function of PT in the Z+jet region.
Mean of ungroomed LHA (charged-only) for AK8 jets as a function of PT in the central dijet region.
Mean of ungroomed LHA (charged-only) for AK8 jets as a function of PT in the forward dijet region.
Mean of ungroomed multiplicity (charged-only) for AK8 jets as a function of PT in the Z+jet region.
Mean of ungroomed multiplicity (charged-only) for AK8 jets as a function of PT in the central dijet region.
Mean of ungroomed multiplicity (charged-only) for AK8 jets as a function of PT in the forward dijet region.
Mean of ungroomed pTD2 (charged-only) for AK8 jets as a function of PT in the Z+jet region.
Mean of ungroomed pTD2 (charged-only) for AK8 jets as a function of PT in the central dijet region.
Mean of ungroomed pTD2 (charged-only) for AK8 jets as a function of PT in the forward dijet region.
Mean of ungroomed thrust (charged-only) for AK8 jets as a function of PT in the Z+jet region.
Mean of ungroomed thrust (charged-only) for AK8 jets as a function of PT in the central dijet region.
Mean of ungroomed thrust (charged-only) for AK8 jets as a function of PT in the forward dijet region.
Mean of ungroomed width (charged-only) for AK8 jets as a function of PT in the Z+jet region.
Mean of ungroomed width (charged-only) for AK8 jets as a function of PT in the central dijet region.
Mean of ungroomed width (charged-only) for AK8 jets as a function of PT in the forward dijet region.
Mean of ungroomed multiplicity for AK8 jets as a function of PT in the central dijet region.
Mean of ungroomed multiplicity for AK8 jets as a function of PT in the forward dijet region.
Mean of ungroomed pTD2 for AK8 jets as a function of PT in the Z+jet region.
Mean of ungroomed pTD2 for AK8 jets as a function of PT in the central dijet region.
Mean of ungroomed pTD2 for AK8 jets as a function of PT in the forward dijet region.
Mean of ungroomed thrust for AK8 jets as a function of PT in the Z+jet region.
Mean of ungroomed thrust for AK8 jets as a function of PT in the central dijet region.
Mean of ungroomed thrust for AK8 jets as a function of PT in the forward dijet region.
Mean of ungroomed width for AK8 jets as a function of PT in the Z+jet region.
Mean of ungroomed width for AK8 jets as a function of PT in the central dijet region.
Mean of ungroomed width for AK8 jets as a function of PT in the forward dijet region.
Mean of groomed LHA for AK8 jets as a function of PT in the Z+jet region.
Mean of groomed LHA for AK8 jets as a function of PT in the central dijet region.
Mean of groomed LHA for AK8 jets as a function of PT in the forward dijet region.
Mean of groomed LHA (charged-only) for AK8 jets as a function of PT in the Z+jet region.
Mean of groomed LHA (charged-only) for AK8 jets as a function of PT in the central dijet region.
Mean of groomed LHA (charged-only) for AK8 jets as a function of PT in the forward dijet region.
Mean of groomed multiplicity (charged-only) for AK8 jets as a function of PT in the Z+jet region.
Mean of groomed multiplicity (charged-only) for AK8 jets as a function of PT in the central dijet region.
Mean of groomed multiplicity (charged-only) for AK8 jets as a function of PT in the forward dijet region.
Mean of groomed pTD2 (charged-only) for AK8 jets as a function of PT in the Z+jet region.
Mean of groomed pTD2 (charged-only) for AK8 jets as a function of PT in the central dijet region.
Mean of groomed pTD2 (charged-only) for AK8 jets as a function of PT in the forward dijet region.
Mean of groomed thrust (charged-only) for AK8 jets as a function of PT in the Z+jet region.
Mean of groomed thrust (charged-only) for AK8 jets as a function of PT in the central dijet region.
Mean of groomed thrust (charged-only) for AK8 jets as a function of PT in the forward dijet region.
Mean of groomed width (charged-only) for AK8 jets as a function of PT in the Z+jet region.
Mean of groomed width (charged-only) for AK8 jets as a function of PT in the central dijet region.
Mean of groomed width (charged-only) for AK8 jets as a function of PT in the forward dijet region.
Mean of groomed multiplicity for AK8 jets as a function of PT in the central dijet region.
Mean of groomed multiplicity for AK8 jets as a function of PT in the forward dijet region.
Mean of groomed pTD2 for AK8 jets as a function of PT in the Z+jet region.
Mean of groomed pTD2 for AK8 jets as a function of PT in the central dijet region.
Mean of groomed pTD2 for AK8 jets as a function of PT in the forward dijet region.
Mean of groomed thrust for AK8 jets as a function of PT in the Z+jet region.
Mean of groomed thrust for AK8 jets as a function of PT in the central dijet region.
Mean of groomed thrust for AK8 jets as a function of PT in the forward dijet region.
Mean of groomed width for AK8 jets as a function of PT in the Z+jet region.
Mean of groomed width for AK8 jets as a function of PT in the central dijet region.
Mean of groomed width for AK8 jets as a function of PT in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 LHA (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 LHA (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 multiplicity in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 multiplicity in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 multiplicity in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 pTD2 in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 pTD2 in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 pTD2 in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 thrust in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 thrust in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 thrust in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 thrust in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of ungroomed AK4 width in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of ungroomed AK4 width in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of ungroomed AK4 width in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of ungroomed AK4 width in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 150 < PT < 186 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 LHA (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 LHA (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 88 < PT < 120 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 120 < PT < 150 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 186 < PT < 254 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 254 < PT < 326 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 326 < PT < 408 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 408 < PT < 481 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 481 < PT < 614 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 614 < PT < 800 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 800 < PT < 1000 GeV in the central dijet region.
Correlation matrix of the particle-level distributions of groomed AK4 multiplicity (charged-only) in 1000 < PT < 4000 GeV in the central dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 50 < PT < 65 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 65 < PT < 88 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 88 < PT < 120 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 120 < PT < 150 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 150 < PT < 186 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 186 < PT < 254 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 254 < PT < 326 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 326 < PT < 408 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 408 < PT < 481 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 481 < PT < 614 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 614 < PT < 800 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 800 < PT < 1000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 multiplicity (charged-only) in 1000 < PT < 4000 GeV in the forward dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 50 < PT < 65 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 65 < PT < 88 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 88 < PT < 120 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 120 < PT < 150 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 150 < PT < 186 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 186 < PT < 254 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 254 < PT < 326 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 326 < PT < 408 GeV in the Z+jet region.
Correlation matrix of the particle-level distributions of groomed AK4 pTD2 (charged-only) in 408 < PT < 1500 GeV in the Z+jet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 50 < PT < 65 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 65 < PT < 88 GeV in the central dijet region.
Particle-level distributions of groomed AK4 pTD2 (charged-only) in 88 < PT < 120 GeV in the central dijet region.
When you search on a word, e.g. 'collisions', we will automatically search across everything we store about a record. But, sometimes you may wish to be more specific. Here we show you how.
Guidance and examples on the query string syntax can be found in the Elasticsearch documentation.
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