Showing 10 of 701 results
Measurements of differential and double-differential cross sections of top quark pair ($\text{t}\overline{\text{t}}$) production are presented in the lepton+jets channels with a single electron or muon and jets in the final state. The analysis combines for the first time signatures of top quarks with low transverse momentum $p_\text{T}$, where the top quark decay products can be identified as separated jets and isolated leptons, and with high $p_\text{T}$, where the decay products are collimated and overlap. The measurements are based on proton-proton collision data at $\sqrt{s} = $ 13 TeV collected by the CMS experiment at the LHC, corresponding to an integrated luminosity of 137 fb$^{-1}$. The cross sections are presented at the parton and particle levels, where the latter minimizes extrapolations based on theoretical assumptions. Most of the measured differential cross sections are well described by standard model predictions with the exception of some double-differential distributions. The inclusive $\text{t}\overline{\text{t}}$ production cross section is measured to be $\sigma_{\text{t}\overline{\text{t}}} = $ 791 $\pm$ 25 pb, which constitutes the most precise measurement in the lepton+jets channel to date.
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A measurement is presented of differential cross sections for $t$-channel single top quark and antiquark production in proton-proton collisions at a centre-of-mass energy of 13 TeV by the CMS experiment at the LHC. From a data set corresponding to an integrated luminosity of 35.9 fb$^{-1}$, events containing one muon or electron and two or three jets are analysed. The cross section is measured as a function of the top quark transverse momentum ($p_\mathrm{T}$), rapidity, and polarisation angle, the charged lepton $p_\mathrm{T}$ and rapidity, and the $p_\mathrm{T}$ of the W boson from the top quark decay. In addition, the charge ratio is measured differentially as a function of the top quark, charged lepton, and W boson kinematic observables. The results are found to be in agreement with standard model predictions using various next-to-leading-order event generators and sets of parton distribution functions. Additionally, the spin asymmetry, sensitive to the top quark polarisation, is determined from the differential distribution of the polarisation angle at parton level to be 0.440 $\pm$ 0.070, in agreement with the standard model prediction.
A measurement is presented of differential cross sections for the Higgs boson (H) production in pp collisions at sqrt(s) = 8 TeV. The analysis exploits the H to gamma gamma decay in data corresponding to an integrated luminosity of 19.7 inverse femtobarns collected by the CMS experiment at the LHC. The cross section is measured as a function of the kinematic properties of the diphoton system and of the associated jets. Results corrected for detector effects are compared with predictions at next-to-leading order and next-to-next-to-leading order in perturbative quantum chromodynamics, as well as with predictions beyond the standard model. For isolated photons with pseudorapidities abs(eta) < 2.5, and with the photon of largest and next-to-largest transverse momentum (pt[gamma]) divided by the diphoton mass m[gamma-gamma] satisfying the respective conditions of pt[gamma] / m[gamma-gamma] > 1/3 and > 1/4, the total fiducial cross section is 32 +/- 10 fb.
Values of the pp $\to$ H $\to \gamma\gamma$ differential cross sections as a function of kinematic observables as measured in data and as predicted in SM simulations. For each observable the fit to $m_{\gamma\gamma}$ is performed simultaneously in all the bins. Since the signal mass is profiled for each observable, the best fit $\hat{m}_{\rm{H}}$ varies from observable to observable.
Values of the pp $\to$ H $\to \gamma\gamma$ differential cross sections as a function of $p_{\rm{T}}^{\gamma\gamma}$ as measured in data. For each observable the fit to $m_{\gamma\gamma}$ is performed simultaneously in all the bins. Since the signal mass is profiled for each observable, the best fit $\hat{m}_{\rm{H}}$ varies from observable to observable.
Values of the pp $\to$ H $\to \gamma\gamma$ differential cross sections as a function of |$\cos\theta^{\ast}$| as measured in data. For each observable the fit to $m_{\gamma\gamma}$ is performed simultaneously in all the bins. Since the signal mass is profiled for each observable, the best fit $\hat{m}_{\rm{H}}$ varies from observable to observable.
Values of the pp $\to$ H $\to \gamma\gamma$ differential cross sections as a function of $\Delta \phi^{\gamma\gamma}$ as measured in data. For each observable the fit to $m_{\gamma\gamma}$ is performed simultaneously in all the bins. Since the signal mass is profiled for each observable, the best fit $\hat{m}_{\rm{H}}$ varies from observable to observable.
Values of the pp $\to$ H $\to \gamma\gamma$ differential cross sections as a function of ||$y^{\gamma\gamma}$|| as measured in data. For each observable the fit to $m_{\gamma\gamma}$ is performed simultaneously in all the bins. Since the signal mass is profiled for each observable, the best fit $\hat{m}_{\rm{H}}$ varies from observable to observable.
Values of the pp $\to$ H $\to \gamma\gamma$ differential cross sections as a function of $N_\rm{jets}$ as measured in data. For each observable the fit to $m_{\gamma\gamma}$ is performed simultaneously in all the bins. Since the signal mass is profiled for each observable, the best fit $\hat{m}_{\rm{H}}$ varies from observable to observable.
Values of the pp $\to$ H $\to \gamma\gamma$ differential cross sections as a function of $p_\rm{T}^\rm{j1}$ as measured in data. For each observable the fit to $m_{\gamma\gamma}$ is performed simultaneously in all the bins. Since the signal mass is profiled for each observable, the best fit $\hat{m}_{\rm{H}}$ varies from observable to observable.
Values of the pp $\to$ H $\to \gamma\gamma$ differential cross sections as a function of |$y^{\gamma\gamma}-y^{\rm{j1}}$| as measured in data. For each observable the fit to $m_{\gamma\gamma}$ is performed simultaneously in all the bins. Since the signal mass is profiled for each observable, the best fit $\hat{m}_{\rm{H}}$ varies from observable to observable.
Values of the pp $\to$ H $\to \gamma\gamma$ differential cross sections as a function of $m_\rm{jj}$ as measured in data. For each observable the fit to $m_{\gamma\gamma}$ is performed simultaneously in all the bins. Since the signal mass is profiled for each observable, the best fit $\hat{m}_{\rm{H}}$ varies from observable to observable.
Values of the pp $\to$ H $\to \gamma\gamma$ differential cross sections as a function of $\Delta \eta^{\rm{jj}}$ as measured in data. For each observable the fit to $m_{\gamma\gamma}$ is performed simultaneously in all the bins. Since the signal mass is profiled for each observable, the best fit $\hat{m}_{\rm{H}}$ varies from observable to observable.
Values of the pp $\to$ H $\to \gamma\gamma$ differential cross sections as a function of $\Delta \phi^{\gamma\gamma,\rm{jj}}$ as measured in data. For each observable the fit to $m_{\gamma\gamma}$ is performed simultaneously in all the bins. Since the signal mass is profiled for each observable, the best fit $\hat{m}_{\rm{H}}$ varies from observable to observable.
Values of the pp $\to$ H $\to \gamma\gamma$ differential cross sections as a function of $\Delta \phi^{\rm{jj}}$ as measured in data. For each observable the fit to $m_{\gamma\gamma}$ is performed simultaneously in all the bins. Since the signal mass is profiled for each observable, the best fit $\hat{m}_{\rm{H}}$ varies from observable to observable.
Values of the pp $\to$ H $\to \gamma\gamma$ differential cross sections as a function of |$\eta^{\gamma\gamma}-(\eta^{\rm{j1}}+\eta^{\rm{j2}})/2$| as measured in data. For each observable the fit to $m_{\gamma\gamma}$ is performed simultaneously in all the bins. Since the signal mass is profiled for each observable, the best fit $\hat{m}_{\rm{H}}$ varies from observable to observable.
This Letter reports measurements of differential cross sections for the production of two Z bosons in association with jets in proton-proton collisions at $\sqrt{s} =$ 8 and 13 TeV. The analysis is based on data samples collected at the LHC with the CMS detector, corresponding to integrated luminosities of 19.7 and 35.9 fb$^{-1}$ at 8 and 13 TeV, respectively. The measurements are performed in the leptonic decay modes ZZ $\to\ell^+ \ell^- \ell'^+ \ell'^-$, where $\ell,\ell' =$ e, $\mu$. The differential cross sections as a function of the jet multiplicity, the transverse momentum $p_\mathrm{T}$, and pseudorapidity of the $p_\mathrm{T}$-leading and subleading jets are presented. In addition, the differential cross sections as a function of variables sensitive to the vector boson scattering, such as the invariant mass of the two $p_\mathrm{T}$-leading jets and their pseudorapidity separation, are reported. The results are compared to theoretical predictions and found in good agreement within the theoretical and experimental uncertainties.
Data from Fig. 2 upper right panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ differential cross section at $\sqrt{s} = 13$ TeV as a function of the jet multiplicity with $|\eta_{j}| < 4.7$.
Data from Fig. 3 upper right panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 13$ TeV as a function of the jet multiplicity with $|\eta_{j}| < 4.7$.
Data from Fig. 2 lower right panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ differential cross section at $\sqrt{s} = 13$ TeV as a function of the jet multiplicity with $|\eta_{j}| < 2.4$.
Data from Fig. 3 lower right panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 13$ TeV as a function of the jet multiplicity with $|\eta_{j}| < 2.4$.
Data from Fig. 4 upper right panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 13$ TeV as a function of the p$_T$-leading jet transverse momentum with $|\eta_{j}| < 4.7$.
Data from Fig. 5 left panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 13$ TeV as a function of the p$_T$-leading jet transverse momentum with $|\eta_{j}| < 4.7$.
Data from Fig. 4 lower right panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 13$ TeV as a function of the p$_T$-leading jet $|\eta_{j}|$ with $|\eta_{j}| < 4.7$.
Data from Fig. 5 right panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 13$ TeV as a function of the p$_T$-subleading jet $|\eta_{j}|$ with $|\eta_{j}| < 4.7$.
Data from Fig. 6 left panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 13$ TeV as a function of the invariant mass of the two p$_T$ leading jets with $|\eta_{j}| < 4.7$.
Data from Fig. 6 right panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 13$ TeV as a function of the invariant of pseudorapidity separation of the two $p$_T$ leading jets with $|\eta_{j}| < 4.7$.
Data from Fig. 2 upper left. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ differential cross section at $\sqrt{s} = 8$ TeV as a function of the jet multiplicity with $|\eta| < 4.7$.
Data from Fig. 3 upper left panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 8$ TeV as a function of the jet multiplicity with $|\eta| < 4.7$.
Data from Fig. 2 lower left panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ differential cross section at $\sqrt{s} = 8$ TeV as a function of the jet multiplicity with $|\eta| < 2.4$.
Data from Fig. 3 lower left panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 8$ TeV as a function of the jet multiplicity with $|\eta| < 2.4$.
Data from Fig. 4 upper left panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 8$ TeV as a function of the p$_T$-leading jet transverse momentum with $|\eta| < 4.7$.
Data from Fig. 4 lower left panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 8$ TeV as a function of the p$_T$-leading jet transverse $\eta$ with $|\eta| < 4.7$.
The production of a Z boson, decaying to two charged leptons, in association with jets in proton-proton collisions at a centre-of-mass energy of 13 TeV is measured. Data recorded with the CMS detector at the LHC are used that correspond to an integrated luminosity of 2.19 fb$^{-1}$. The cross section is measured as a function of the jet multiplicity and its dependence on the transverse momentum of the Z boson, the jet kinematic variables (transverse momentum and rapidity), the scalar sum of the jet momenta, which quantifies the hadronic activity, and the balance in transverse momentum between the reconstructed jet recoil and the Z boson. The measurements are compared with predictions from four different calculations. The first two merge matrix elements with different parton multiplicities in the final state and parton showering, one of which includes one-loop corrections. The third is a fixed-order calculation with next-to-next-to-leading order accuracy for the process with a Z boson and one parton in the final state. The fourth combines the fully differential next-to-next-to-leading order calculation with next-to-next-to-leading logarithm resummation and parton showering.
Measurements of inclusive isolated-photon and photon+jet production in proton-proton collisions at $\sqrt{s} =$ 13 TeV are presented. The analysis uses data collected by the CMS experiment in 2015, corresponding to an integrated luminosity of 2.26 fb$^{-1}$. The cross section for inclusive isolated photon production is measured as a function of the photon transverse energy in a fiducial region. The cross section for photon+jet production is measured as a function of the photon transverse energy in the same fiducial region with identical photon requirements and with the highest transverse momentum jet. All measurements are in agreement with predictions from next-to-leading-order perturbative QCD.
Double differential cross sections for isolated-photon production in photon rapidity bins. The cross section values are presented per photon transverse energy and rapidity unit.
Tripple differential cross sections for photon+jet production in photon and jet rapidity bins. The cross section values are presented per photon transverse energy, photon rapidity, and jet rapidity unit.
A measurement is presented of the production of Z bosons that decay into two electrons or muons in association with jets, in proton-proton collisions at a centre-of-mass energy of 13 TeV. The data were recorded by the CMS Collaboration at the LHC with an integrated luminosity of 35.9 fb$^{-1}$. The differential cross sections are measured as a function of the transverse momentum ($p_\mathrm{T}$) of the Z boson and the transverse momentum and rapidities of the five jets with largest $p_\mathrm{T}$. The jet multiplicity distribution is measured for up to eight jets. The hadronic activity in the events is estimated using the scalar sum of the $p_\mathrm{T}$ of all the jets. All measurements are unfolded to the stable particle-level and compared with predictions from various Monte Carlo event generators, as well as with expectations at leading and next-to-leading orders in perturbative quantum chromodynamics.
A measurement of differential cross sections for the production of a pair of isolated photons in proton-proton collisions at sqrt(s) = 7 TeV is presented. The data sample corresponds to an integrated luminosity of 5.0 inverse femtobarns collected with the CMS detector. A data-driven isolation template method is used to extract the prompt diphoton yield. The measured cross section for two isolated photons, with transverse energy above 40 and 25 GeV respectively, in the pseudorapidity range abs(eta) < 2.5, abs(eta) not in [1.44,1.57] and with an angular separation Delta R > 0.45, is 17.2 +/- 0.2 (stat.) +/- 1.9 (syst.) +/- 0.4 (lum.) pb. Differential cross sections are measured as a function of the diphoton invariant mass, the diphoton transverse momentum, the azimuthal angle difference between the two photons, and the cosine of the polar angle in the Collins-Soper reference frame of the diphoton system. The results are compared to theoretical predictions at leading, next-to-leading, and next-to-next-to-leading order in quantum chromodynamics.
Values of D(SIG)/DM(GAMMA GAMMA) for the data. The error given on each value is the total uncertainty.
Values of D(SIG)/DPT(GAMMA GAMMA) for the data. The error given on each value is the total uncertainty.
Values of D(SIG)/DDELTA(PHI(GAMMA GAMMA)) (pb/rad) for the data. The error given on each value is the total uncertainty.
Values of D(SIG)/DABS(COS(THETA)) for the data. The error given on each value is the total uncertainty.
Differential and double-differential cross sections for the production of top quark pairs in proton-proton collisions at $\sqrt{s} =$ 13 TeV are measured as a function of kinematic variables of the top quarks and the top quark-antiquark ($\mathrm{t}\overline{\mathrm{t}}$) system. In addition, kinematic variables and multiplicities of jets associated with the $\mathrm{t}\overline{\mathrm{t}}$ production are measured. This analysis is based on data collected by the CMS experiment at the LHC in 2016 corresponding to an integrated luminosity of 35.8 fb$^{-1}$. The measurements are performed in the lepton+jets decay channels with a single muon or electron and jets in the final state. The differential cross sections are presented at the particle level, within a phase space close to the experimental acceptance, and at the parton level in the full phase space. The results are compared to several standard model predictions that use different methods and approximations. The kinematic variables of the top quarks and the $\mathrm{t}\overline{\mathrm{t}}$ system are reasonably described in general, though none predict all the measured distributions. In particular, the transverse momentum distribution of the top quarks is more steeply falling than predicted. The kinematic distributions and multiplicities of jets are adequately modeled by certain combinations of next-to-leading-order calculations and parton shower models.
Absolute cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$.
Covariance matrix of absolute cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$.
Covariance matrix of absolute cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at particle level as a function of $|y(\text{t}_\text{h})|$.
Absolute cross section at particle level as a function of $|y(\text{t}_\text{h})|$.
Covariance matrix of absolute cross section at particle level as a function of $|y(\text{t}_\text{h})|$.
Covariance matrix of absolute cross section at particle level as a function of $|y(\text{t}_\text{h})|$.
Absolute cross section at particle level as a function of $p_\text{T}(\text{t}_\text{l})$.
Absolute cross section at particle level as a function of $p_\text{T}(\text{t}_\text{l})$.
Covariance matrix of absolute cross section at particle level as a function of $p_\text{T}(\text{t}_\text{l})$.
Covariance matrix of absolute cross section at particle level as a function of $p_\text{T}(\text{t}_\text{l})$.
Absolute cross section at particle level as a function of $|y(\text{t}_\text{l})|$.
Absolute cross section at particle level as a function of $|y(\text{t}_\text{l})|$.
Covariance matrix of absolute cross section at particle level as a function of $|y(\text{t}_\text{l})|$.
Covariance matrix of absolute cross section at particle level as a function of $|y(\text{t}_\text{l})|$.
Absolute cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$.
Covariance matrix of absolute cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$.
Covariance matrix of absolute cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of $p_\text{T}(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of $p_\text{T}(\text{t}\bar{\text{t}})$.
Covariance matrix of absolute cross section at particle level as a function of $p_\text{T}(\text{t}\bar{\text{t}})$.
Covariance matrix of absolute cross section at particle level as a function of $p_\text{T}(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of $|y(\text{t}\bar{\text{t}})|$.
Absolute cross section at particle level as a function of $|y(\text{t}\bar{\text{t}})|$.
Covariance matrix of absolute cross section at particle level as a function of $|y(\text{t}\bar{\text{t}})|$.
Covariance matrix of absolute cross section at particle level as a function of $|y(\text{t}\bar{\text{t}})|$.
Absolute cross section at particle level as a function of Additional jets.
Absolute cross section at particle level as a function of Additional jets.
Covariance matrix of absolute cross section at particle level as a function of Additional jets.
Covariance matrix of absolute cross section at particle level as a function of Additional jets.
Absolute cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.
Covariance matrix of absolute cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.
Covariance matrix of absolute cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.
Covariance matrix of absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.
Covariance matrix of absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.
Covariance matrix of absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.
Covariance matrix of absolute cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Covariance matrix of absolute cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Covariance matrix of absolute cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Absolute cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Absolute cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Absolute cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Absolute cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Absolute cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Absolute cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Absolute cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Covariance matrix of absolute cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Covariance matrix of absolute cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Absolute cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Covariance matrix of absolute cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Covariance matrix of absolute cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Absolute cross section at particle level as a function of $p_\text{T}(b_\text{l})$.
Absolute cross section at particle level as a function of $p_\text{T}(b_\text{l})$.
Absolute cross section at particle level as a function of $p_\text{T}(b_\text{h})$.
Absolute cross section at particle level as a function of $p_\text{T}(b_\text{h})$.
Absolute cross section at particle level as a function of $p_\text{T}(j_\text{W1})$.
Absolute cross section at particle level as a function of $p_\text{T}(j_\text{W1})$.
Absolute cross section at particle level as a function of $p_\text{T}(j_\text{W2})$.
Absolute cross section at particle level as a function of $p_\text{T}(j_\text{W2})$.
Absolute cross section at particle level as a function of $p_\text{T}(j_\text{1})$.
Absolute cross section at particle level as a function of $p_\text{T}(j_\text{1})$.
Absolute cross section at particle level as a function of $p_\text{T}(j_\text{2})$.
Absolute cross section at particle level as a function of $p_\text{T}(j_\text{2})$.
Absolute cross section at particle level as a function of $p_\text{T}(j_\text{3})$.
Absolute cross section at particle level as a function of $p_\text{T}(j_\text{3})$.
Absolute cross section at particle level as a function of $p_\text{T}(j_\text{4})$.
Absolute cross section at particle level as a function of $p_\text{T}(j_\text{4})$.
Covariance matrix of absolute cross section at particle level as a function of Jet type vs. $p_\text{T}(\mathrm{jet})$.
Covariance matrix of absolute cross section at particle level as a function of Jet type vs. $p_\text{T}(\mathrm{jet})$.
Absolute cross section at particle level as a function of $|\eta(b_\text{l})|$.
Absolute cross section at particle level as a function of $|\eta(b_\text{l})|$.
Absolute cross section at particle level as a function of $|\eta(b_\text{h})|$.
Absolute cross section at particle level as a function of $|\eta(b_\text{h})|$.
Absolute cross section at particle level as a function of $|\eta(j_\text{W1})|$.
Absolute cross section at particle level as a function of $|\eta(j_\text{W1})|$.
Absolute cross section at particle level as a function of $|\eta(j_\text{W2})|$.
Absolute cross section at particle level as a function of $|\eta(j_\text{W2})|$.
Absolute cross section at particle level as a function of $|\eta(j_\text{1})|$.
Absolute cross section at particle level as a function of $|\eta(j_\text{1})|$.
Absolute cross section at particle level as a function of $|\eta(j_\text{2})|$.
Absolute cross section at particle level as a function of $|\eta(j_\text{2})|$.
Absolute cross section at particle level as a function of $|\eta(j_\text{3})|$.
Absolute cross section at particle level as a function of $|\eta(j_\text{3})|$.
Absolute cross section at particle level as a function of $|\eta(j_\text{4})|$.
Absolute cross section at particle level as a function of $|\eta(j_\text{4})|$.
Covariance matrix of absolute cross section at particle level as a function of Jet type vs. $|\eta(\text{jet})|$.
Covariance matrix of absolute cross section at particle level as a function of Jet type vs. $|\eta(\text{jet})|$.
Absolute cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(b_\text{l})$.
Absolute cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(b_\text{l})$.
Absolute cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(b_\text{h})$.
Absolute cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(b_\text{h})$.
Absolute cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{W1})$.
Absolute cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{W1})$.
Absolute cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{W2})$.
Absolute cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{W2})$.
Absolute cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{1})$.
Absolute cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{1})$.
Absolute cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{2})$.
Absolute cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{2})$.
Absolute cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{3})$.
Absolute cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{3})$.
Absolute cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{4})$.
Absolute cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{4})$.
Covariance matrix of absolute cross section at particle level as a function of Jet type vs. $\Delta R_{\text{j}_\text{t}}$.
Covariance matrix of absolute cross section at particle level as a function of Jet type vs. $\Delta R_{\text{j}_\text{t}}$.
Absolute cross section at particle level as a function of $\Delta R_\text{t}(b_\text{l})$.
Absolute cross section at particle level as a function of $\Delta R_\text{t}(b_\text{l})$.
Absolute cross section at particle level as a function of $\Delta R_\text{t}(b_\text{h})$.
Absolute cross section at particle level as a function of $\Delta R_\text{t}(b_\text{h})$.
Absolute cross section at particle level as a function of $\Delta R_\text{t}(j_\text{W1})$.
Absolute cross section at particle level as a function of $\Delta R_\text{t}(j_\text{W1})$.
Absolute cross section at particle level as a function of $\Delta R_\text{t}(j_\text{W2})$.
Absolute cross section at particle level as a function of $\Delta R_\text{t}(j_\text{W2})$.
Absolute cross section at particle level as a function of $\Delta R_\text{t}(j_\text{1})$.
Absolute cross section at particle level as a function of $\Delta R_\text{t}(j_\text{1})$.
Absolute cross section at particle level as a function of $\Delta R_\text{t}(j_\text{2})$.
Absolute cross section at particle level as a function of $\Delta R_\text{t}(j_\text{2})$.
Absolute cross section at particle level as a function of $\Delta R_\text{t}(j_\text{3})$.
Absolute cross section at particle level as a function of $\Delta R_\text{t}(j_\text{3})$.
Absolute cross section at particle level as a function of $\Delta R_\text{t}(j_\text{4})$.
Absolute cross section at particle level as a function of $\Delta R_\text{t}(j_\text{4})$.
Covariance matrix of absolute cross section at particle level as a function of Jet type vs. $\Delta R_\text{t}$.
Covariance matrix of absolute cross section at particle level as a function of Jet type vs. $\Delta R_\text{t}$.
Normalized cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$.
Covariance matrix of normalized cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$.
Covariance matrix of normalized cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at particle level as a function of $|y(\text{t}_\text{h})|$.
Normalized cross section at particle level as a function of $|y(\text{t}_\text{h})|$.
Covariance matrix of normalized cross section at particle level as a function of $|y(\text{t}_\text{h})|$.
Covariance matrix of normalized cross section at particle level as a function of $|y(\text{t}_\text{h})|$.
Normalized cross section at particle level as a function of $p_\text{T}(\text{t}_\text{l})$.
Normalized cross section at particle level as a function of $p_\text{T}(\text{t}_\text{l})$.
Covariance matrix of normalized cross section at particle level as a function of $p_\text{T}(\text{t}_\text{l})$.
Covariance matrix of normalized cross section at particle level as a function of $p_\text{T}(\text{t}_\text{l})$.
Normalized cross section at particle level as a function of $|y(\text{t}_\text{l})|$.
Normalized cross section at particle level as a function of $|y(\text{t}_\text{l})|$.
Covariance matrix of normalized cross section at particle level as a function of $|y(\text{t}_\text{l})|$.
Covariance matrix of normalized cross section at particle level as a function of $|y(\text{t}_\text{l})|$.
Normalized cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$.
Covariance matrix of normalized cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$.
Covariance matrix of normalized cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of $p_\text{T}(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of $p_\text{T}(\text{t}\bar{\text{t}})$.
Covariance matrix of normalized cross section at particle level as a function of $p_\text{T}(\text{t}\bar{\text{t}})$.
Covariance matrix of normalized cross section at particle level as a function of $p_\text{T}(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of $|y(\text{t}\bar{\text{t}})|$.
Normalized cross section at particle level as a function of $|y(\text{t}\bar{\text{t}})|$.
Covariance matrix of normalized cross section at particle level as a function of $|y(\text{t}\bar{\text{t}})|$.
Covariance matrix of normalized cross section at particle level as a function of $|y(\text{t}\bar{\text{t}})|$.
Normalized cross section at particle level as a function of Additional jets.
Normalized cross section at particle level as a function of Additional jets.
Covariance matrix of normalized cross section at particle level as a function of Additional jets.
Covariance matrix of normalized cross section at particle level as a function of Additional jets.
Normalized cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.
Covariance matrix of normalized cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.
Covariance matrix of normalized cross section at particle level as a function of Additional jets vs. $M(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.
Covariance matrix of normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.
Covariance matrix of normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.
Covariance matrix of normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.
Covariance matrix of normalized cross section at particle level as a function of Additional jets vs. $p_\text{T}(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Covariance matrix of normalized cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Covariance matrix of normalized cross section at particle level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Normalized cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Normalized cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Normalized cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Normalized cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Normalized cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Normalized cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Normalized cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Covariance matrix of normalized cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Covariance matrix of normalized cross section at particle level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Normalized cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Covariance matrix of normalized cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Covariance matrix of normalized cross section at particle level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Normalized cross section at particle level as a function of $p_\text{T}(b_\text{l})$.
Normalized cross section at particle level as a function of $p_\text{T}(b_\text{l})$.
Normalized cross section at particle level as a function of $p_\text{T}(b_\text{h})$.
Normalized cross section at particle level as a function of $p_\text{T}(b_\text{h})$.
Normalized cross section at particle level as a function of $p_\text{T}(j_\text{W1})$.
Normalized cross section at particle level as a function of $p_\text{T}(j_\text{W1})$.
Normalized cross section at particle level as a function of $p_\text{T}(j_\text{W2})$.
Normalized cross section at particle level as a function of $p_\text{T}(j_\text{W2})$.
Normalized cross section at particle level as a function of $p_\text{T}(j_\text{1})$.
Normalized cross section at particle level as a function of $p_\text{T}(j_\text{1})$.
Normalized cross section at particle level as a function of $p_\text{T}(j_\text{2})$.
Normalized cross section at particle level as a function of $p_\text{T}(j_\text{2})$.
Normalized cross section at particle level as a function of $p_\text{T}(j_\text{3})$.
Normalized cross section at particle level as a function of $p_\text{T}(j_\text{3})$.
Normalized cross section at particle level as a function of $p_\text{T}(j_\text{4})$.
Normalized cross section at particle level as a function of $p_\text{T}(j_\text{4})$.
Covariance matrix of normalized cross section at particle level as a function of Jet type vs. $p_\text{T}(\mathrm{jet})$.
Covariance matrix of normalized cross section at particle level as a function of Jet type vs. $p_\text{T}(\mathrm{jet})$.
Normalized cross section at particle level as a function of $|\eta(b_\text{l})|$.
Normalized cross section at particle level as a function of $|\eta(b_\text{l})|$.
Normalized cross section at particle level as a function of $|\eta(b_\text{h})|$.
Normalized cross section at particle level as a function of $|\eta(b_\text{h})|$.
Normalized cross section at particle level as a function of $|\eta(j_\text{W1})|$.
Normalized cross section at particle level as a function of $|\eta(j_\text{W1})|$.
Normalized cross section at particle level as a function of $|\eta(j_\text{W2})|$.
Normalized cross section at particle level as a function of $|\eta(j_\text{W2})|$.
Normalized cross section at particle level as a function of $|\eta(j_\text{1})|$.
Normalized cross section at particle level as a function of $|\eta(j_\text{1})|$.
Normalized cross section at particle level as a function of $|\eta(j_\text{2})|$.
Normalized cross section at particle level as a function of $|\eta(j_\text{2})|$.
Normalized cross section at particle level as a function of $|\eta(j_\text{3})|$.
Normalized cross section at particle level as a function of $|\eta(j_\text{3})|$.
Normalized cross section at particle level as a function of $|\eta(j_\text{4})|$.
Normalized cross section at particle level as a function of $|\eta(j_\text{4})|$.
Covariance matrix of normalized cross section at particle level as a function of Jet type vs. $|\eta(\text{jet})|$.
Covariance matrix of normalized cross section at particle level as a function of Jet type vs. $|\eta(\text{jet})|$.
Normalized cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(b_\text{l})$.
Normalized cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(b_\text{l})$.
Normalized cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(b_\text{h})$.
Normalized cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(b_\text{h})$.
Normalized cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{W1})$.
Normalized cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{W1})$.
Normalized cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{W2})$.
Normalized cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{W2})$.
Normalized cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{1})$.
Normalized cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{1})$.
Normalized cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{2})$.
Normalized cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{2})$.
Normalized cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{3})$.
Normalized cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{3})$.
Normalized cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{4})$.
Normalized cross section at particle level as a function of $\Delta R_{\text{j}_\text{t}}(j_\text{4})$.
Covariance matrix of normalized cross section at particle level as a function of Jet type vs. $\Delta R_{\text{j}_\text{t}}$.
Covariance matrix of normalized cross section at particle level as a function of Jet type vs. $\Delta R_{\text{j}_\text{t}}$.
Normalized cross section at particle level as a function of $\Delta R_\text{t}(b_\text{l})$.
Normalized cross section at particle level as a function of $\Delta R_\text{t}(b_\text{l})$.
Normalized cross section at particle level as a function of $\Delta R_\text{t}(b_\text{h})$.
Normalized cross section at particle level as a function of $\Delta R_\text{t}(b_\text{h})$.
Normalized cross section at particle level as a function of $\Delta R_\text{t}(j_\text{W1})$.
Normalized cross section at particle level as a function of $\Delta R_\text{t}(j_\text{W1})$.
Normalized cross section at particle level as a function of $\Delta R_\text{t}(j_\text{W2})$.
Normalized cross section at particle level as a function of $\Delta R_\text{t}(j_\text{W2})$.
Normalized cross section at particle level as a function of $\Delta R_\text{t}(j_\text{1})$.
Normalized cross section at particle level as a function of $\Delta R_\text{t}(j_\text{1})$.
Normalized cross section at particle level as a function of $\Delta R_\text{t}(j_\text{2})$.
Normalized cross section at particle level as a function of $\Delta R_\text{t}(j_\text{2})$.
Normalized cross section at particle level as a function of $\Delta R_\text{t}(j_\text{3})$.
Normalized cross section at particle level as a function of $\Delta R_\text{t}(j_\text{3})$.
Normalized cross section at particle level as a function of $\Delta R_\text{t}(j_\text{4})$.
Normalized cross section at particle level as a function of $\Delta R_\text{t}(j_\text{4})$.
Covariance matrix of normalized cross section at particle level as a function of Jet type vs. $\Delta R_\text{t}$.
Covariance matrix of normalized cross section at particle level as a function of Jet type vs. $\Delta R_\text{t}$.
gap fraction at particle level.
gap fraction at particle level.
Covariance matrix of gap fraction at particle level.
Covariance matrix of gap fraction at particle level.
gap fraction at particle level.
gap fraction at particle level.
Covariance matrix of gap fraction at particle level.
Covariance matrix of gap fraction at particle level.
jet multiplicities for $p_{T}(jet) > 30.0$ GeV.
jet multiplicities for $p_{T}(jet) > 30.0$ GeV.
jet multiplicities for $p_{T}(jet) > 50.0$ GeV.
jet multiplicities for $p_{T}(jet) > 50.0$ GeV.
jet multiplicities for $p_{T}(jet) > 75.0$ GeV.
jet multiplicities for $p_{T}(jet) > 75.0$ GeV.
jet multiplicities for $p_{T}(jet) > 100.0$ GeV.
jet multiplicities for $p_{T}(jet) > 100.0$ GeV.
Covariance matrix of jet multiplicities with different pT(jet) thresholds.
Covariance matrix of jet multiplicities with different pT(jet) thresholds.
Absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{high})$.
Absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{high})$.
Covariance matrix of absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{high})$.
Covariance matrix of absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{high})$.
Absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{low})$.
Absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{low})$.
Covariance matrix of absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{low})$.
Covariance matrix of absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{low})$.
Absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$.
Covariance matrix of absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$.
Covariance matrix of absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at the parton level as a function of $|y(\text{t}_\text{h})|$.
Absolute cross section at the parton level as a function of $|y(\text{t}_\text{h})|$.
Covariance matrix of absolute cross section at the parton level as a function of $|y(\text{t}_\text{h})|$.
Covariance matrix of absolute cross section at the parton level as a function of $|y(\text{t}_\text{h})|$.
Absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{l})$.
Absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{l})$.
Covariance matrix of absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{l})$.
Covariance matrix of absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{l})$.
Absolute cross section at the parton level as a function of $|y(\text{t}_\text{l})|$.
Absolute cross section at the parton level as a function of $|y(\text{t}_\text{l})|$.
Covariance matrix of absolute cross section at the parton level as a function of $|y(\text{t}_\text{l})|$.
Covariance matrix of absolute cross section at the parton level as a function of $|y(\text{t}_\text{l})|$.
Absolute cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$.
Absolute cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$.
Covariance matrix of absolute cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$.
Covariance matrix of absolute cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$.
Absolute cross section at the parton level as a function of $p_\text{T}(\text{t}\bar{\text{t}})$.
Absolute cross section at the parton level as a function of $p_\text{T}(\text{t}\bar{\text{t}})$.
Covariance matrix of absolute cross section at the parton level as a function of $p_\text{T}(\text{t}\bar{\text{t}})$.
Covariance matrix of absolute cross section at the parton level as a function of $p_\text{T}(\text{t}\bar{\text{t}})$.
Absolute cross section at the parton level as a function of $|y(\text{t}\bar{\text{t}})|$.
Absolute cross section at the parton level as a function of $|y(\text{t}\bar{\text{t}})|$.
Covariance matrix of absolute cross section at the parton level as a function of $|y(\text{t}\bar{\text{t}})|$.
Covariance matrix of absolute cross section at the parton level as a function of $|y(\text{t}\bar{\text{t}})|$.
Absolute cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Covariance matrix of absolute cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Covariance matrix of absolute cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Absolute cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Absolute cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Absolute cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Absolute cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Absolute cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Absolute cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Absolute cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Absolute cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Covariance matrix of absolute cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Covariance matrix of absolute cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Covariance matrix of absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Covariance matrix of absolute cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{high})$.
Normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{high})$.
Covariance matrix of normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{high})$.
Covariance matrix of normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{high})$.
Normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{low})$.
Normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{low})$.
Covariance matrix of normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{low})$.
Covariance matrix of normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{low})$.
Normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$.
Covariance matrix of normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$.
Covariance matrix of normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at the parton level as a function of $|y(\text{t}_\text{h})|$.
Normalized cross section at the parton level as a function of $|y(\text{t}_\text{h})|$.
Covariance matrix of normalized cross section at the parton level as a function of $|y(\text{t}_\text{h})|$.
Covariance matrix of normalized cross section at the parton level as a function of $|y(\text{t}_\text{h})|$.
Normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{l})$.
Normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{l})$.
Covariance matrix of normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{l})$.
Covariance matrix of normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{l})$.
Normalized cross section at the parton level as a function of $|y(\text{t}_\text{l})|$.
Normalized cross section at the parton level as a function of $|y(\text{t}_\text{l})|$.
Covariance matrix of normalized cross section at the parton level as a function of $|y(\text{t}_\text{l})|$.
Covariance matrix of normalized cross section at the parton level as a function of $|y(\text{t}_\text{l})|$.
Normalized cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$.
Normalized cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$.
Covariance matrix of normalized cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$.
Covariance matrix of normalized cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$.
Normalized cross section at the parton level as a function of $p_\text{T}(\text{t}\bar{\text{t}})$.
Normalized cross section at the parton level as a function of $p_\text{T}(\text{t}\bar{\text{t}})$.
Covariance matrix of normalized cross section at the parton level as a function of $p_\text{T}(\text{t}\bar{\text{t}})$.
Covariance matrix of normalized cross section at the parton level as a function of $p_\text{T}(\text{t}\bar{\text{t}})$.
Normalized cross section at the parton level as a function of $|y(\text{t}\bar{\text{t}})|$.
Normalized cross section at the parton level as a function of $|y(\text{t}\bar{\text{t}})|$.
Covariance matrix of normalized cross section at the parton level as a function of $|y(\text{t}\bar{\text{t}})|$.
Covariance matrix of normalized cross section at the parton level as a function of $|y(\text{t}\bar{\text{t}})|$.
Normalized cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Covariance matrix of normalized cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Covariance matrix of normalized cross section at the parton level as a function of $|y(\text{t}_\text{h})|$ vs. $p_\text{T}(\text{t}_\text{h})$.
Normalized cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Normalized cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Normalized cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Normalized cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Normalized cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Normalized cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Normalized cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Normalized cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Covariance matrix of normalized cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Covariance matrix of normalized cross section at the parton level as a function of $M(\text{t}\bar{\text{t}})$ vs. $|y(\text{t}\bar{\text{t}})|$.
Normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Covariance matrix of normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Covariance matrix of normalized cross section at the parton level as a function of $p_\text{T}(\text{t}_\text{h})$ vs. $M(\text{t}\bar{\text{t}})$.
Differential and double-differential cross sections for the production of top quark pairs in proton-proton collisions at 13 TeV are measured as a function of jet multiplicity and of kinematic variables of the top quarks and the top quark-antiquark system. This analysis is based on data collected by the CMS experiment at the LHC corresponding to an integrated luminosity of 2.3 inverse femtobarns. The measurements are performed in the lepton+jets decay channels with a single muon or electron in the final state. The differential cross sections are presented at particle level, within a phase space close to the experimental acceptance, and at parton level in the full phase space. The results are compared to several standard model predictions.
Absolute cross section at particle level.
Covariance matrix of absolute cross section at particle level.
Absolute cross section at particle level.
Covariance matrix of absolute cross section at particle level.
Absolute cross section at particle level.
Covariance matrix of absolute cross section at particle level.
Absolute cross section at particle level.
Covariance matrix of absolute cross section at particle level.
Absolute cross section at particle level.
Covariance matrix of absolute cross section at particle level.
Absolute cross section at particle level.
Covariance matrix of absolute cross section at particle level.
Absolute cross section at particle level.
Covariance matrix of absolute cross section at particle level.
Absolute cross section at particle level.
Covariance matrix of absolute cross section at particle level.
Absolute cross section at particle level.
Absolute cross section at particle level.
Absolute cross section at particle level.
Absolute cross section at particle level.
Covariance matrix of absolute cross section at particle level.
Absolute cross section at particle level.
Absolute cross section at particle level.
Absolute cross section at particle level.
Absolute cross section at particle level.
Covariance matrix of absolute cross section at particle level.
Absolute cross section at particle level.
Absolute cross section at particle level.
Absolute cross section at particle level.
Absolute cross section at particle level.
Covariance matrix of absolute cross section at particle level.
Absolute cross section at particle level.
Absolute cross section at particle level.
Absolute cross section at particle level.
Absolute cross section at particle level.
Covariance matrix of absolute cross section at particle level.
Absolute cross section at particle level.
Absolute cross section at particle level.
Absolute cross section at particle level.
Absolute cross section at particle level.
Covariance matrix of absolute cross section at particle level.
Normalized cross section at particle level.
Covariance matrix of normalized cross section at particle level.
Normalized cross section at particle level.
Covariance matrix of normalized cross section at particle level.
Normalized cross section at particle level.
Covariance matrix of normalized cross section at particle level.
Normalized cross section at particle level.
Covariance matrix of normalized cross section at particle level.
Normalized cross section at particle level.
Covariance matrix of normalized cross section at particle level.
Normalized cross section at particle level.
Covariance matrix of normalized cross section at particle level.
Normalized cross section at particle level.
Covariance matrix of normalized cross section at particle level.
Normalized cross section at particle level.
Covariance matrix of normalized cross section at particle level.
Normalized cross section at particle level.
Normalized cross section at particle level.
Normalized cross section at particle level.
Normalized cross section at particle level.
Covariance matrix of normalized cross section at particle level.
Normalized cross section at particle level.
Normalized cross section at particle level.
Normalized cross section at particle level.
Normalized cross section at particle level.
Covariance matrix of normalized cross section at particle level.
Normalized cross section at particle level.
Normalized cross section at particle level.
Normalized cross section at particle level.
Normalized cross section at particle level.
Covariance matrix of normalized cross section at particle level.
Normalized cross section at particle level.
Normalized cross section at particle level.
Normalized cross section at particle level.
Normalized cross section at particle level.
Covariance matrix of normalized cross section at particle level.
Normalized cross section at particle level.
Normalized cross section at particle level.
Normalized cross section at particle level.
Normalized cross section at particle level.
Covariance matrix of normalized cross section at particle level.
Absolute cross section at parton level.
Covariance matrix of absolute cross section at parton level.
Absolute cross section at parton level.
Covariance matrix of absolute cross section at parton level.
Absolute cross section at parton level.
Covariance matrix of absolute cross section at parton level.
Absolute cross section at parton level.
Covariance matrix of absolute cross section at parton level.
Absolute cross section at parton level.
Covariance matrix of absolute cross section at parton level.
Absolute cross section at parton level.
Covariance matrix of absolute cross section at parton level.
Absolute cross section at parton level.
Covariance matrix of absolute cross section at parton level.
Absolute cross section at parton level.
Covariance matrix of absolute cross section at parton level.
Absolute cross section at parton level.
Absolute cross section at parton level.
Absolute cross section at parton level.
Absolute cross section at parton level.
Covariance matrix of absolute cross section at parton level.
Absolute cross section at parton level.
Absolute cross section at parton level.
Absolute cross section at parton level.
Absolute cross section at parton level.
Covariance matrix of absolute cross section at parton level.
Absolute cross section at parton level.
Absolute cross section at parton level.
Absolute cross section at parton level.
Absolute cross section at parton level.
Covariance matrix of absolute cross section at parton level.
Absolute cross section at parton level.
Absolute cross section at parton level.
Absolute cross section at parton level.
Absolute cross section at parton level.
Covariance matrix of absolute cross section at parton level.
Absolute cross section at parton level.
Absolute cross section at parton level.
Absolute cross section at parton level.
Absolute cross section at parton level.
Covariance matrix of absolute cross section at parton level.
Normalized cross section at parton level.
Covariance matrix of normalized cross section at parton level.
Normalized cross section at parton level.
Covariance matrix of normalized cross section at parton level.
Normalized cross section at parton level.
Covariance matrix of normalized cross section at parton level.
Normalized cross section at parton level.
Covariance matrix of normalized cross section at parton level.
Normalized cross section at parton level.
Covariance matrix of normalized cross section at parton level.
Normalized cross section at parton level.
Covariance matrix of normalized cross section at parton level.
Normalized cross section at parton level.
Covariance matrix of normalized cross section at parton level.
Normalized cross section at parton level.
Covariance matrix of normalized cross section at parton level.
Normalized cross section at parton level.
Normalized cross section at parton level.
Normalized cross section at parton level.
Normalized cross section at parton level.
Covariance matrix of normalized cross section at parton level.
Normalized cross section at parton level.
Normalized cross section at parton level.
Normalized cross section at parton level.
Normalized cross section at parton level.
Covariance matrix of normalized cross section at parton level.
Normalized cross section at parton level.
Normalized cross section at parton level.
Normalized cross section at parton level.
Normalized cross section at parton level.
Covariance matrix of normalized cross section at parton level.
Normalized cross section at parton level.
Normalized cross section at parton level.
Normalized cross section at parton level.
Normalized cross section at parton level.
Covariance matrix of normalized cross section at parton level.
Normalized cross section at parton level.
Normalized cross section at parton level.
Normalized cross section at parton level.
Normalized cross section at parton level.
Covariance matrix of normalized cross section at parton level.
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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