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The discovery of the Higgs boson has led to new possible signatures for heavy resonance searches at the LHC. Since then, search channels including at least one Higgs boson plus another particle have formed an important part of the program of new physics searches. In this report, the status of these searches by the CMS Collaboration is reviewed. Searches are discussed for resonances decaying to two Higgs bosons, a Higgs and a vector boson, or a Higgs boson and another new resonance, with proton-proton collision data collected at $\sqrt{s}$ = 13 TeV in the years 2016-2018. A combination of the results of these searches is presented together with constraints on different beyond-the-standard model scenarios, including scenarios with extended Higgs sectors, heavy vector bosons and extra dimensions. Studies are shown for the first time by CMS on the validity of the narrow-width approximation in searches for the resonant production of a pair of Higgs bosons. The potential for a discovery at the High Luminosity LHC is also discussed.
Upper limits on σB for a spin-0 resonance X obtained from the combination of the individual channels. The 68 and 95% CL intervals on the expected upper limits are shown as colored bands.
Upper limits on σB for a spin-2 resonance G obtained from the combination of the individual channels. The 68 and 95% CL intervals on the expected upper limits are shown as colored bands.
Upper limits at 95% CL on $\sigma$B(pp→X→Y(bb)H) for combination as a function of m$_Y$.
Upper limits at 95% CL on $\sigma$B(pp→X→Y(bb)H) for combination as a function of m$_Y$.
Expected upper limits at 95% CL on the X → HH cross section as a function of mX from the combination of the three channels bbγγ, bbττ, and bbbb for an integrated luminosity of 3000 fb−1 with different assumptions on the systematic uncertainties.
Expected upper limits on the X → YH cross section times B(Y → bb) for mX ≤ 1000 GeV at 95 % CL as a function of m$_X$ and m$_Y$ from the combination of all considered channels projected to an integrated luminosity of 3000 fb$^{-1}$. Systematic uncertainties according to the ”S2” scenario are assumed.
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. $M(\text{t}\bar{\text{t}})$.
Charmonium production in p – A collisions is a unique tool for the study of the interaction of bound c c states in nuclear matter. It can provide details on the basic features of the resonance formation mechanism and, in particular, on its non-perturbative aspects. In this Letter, we present an experimental study of charmonia and Drell–Yan production in proton–nucleus collisions at 450 GeV/ c . The results are analyzed in the framework of the Glauber model and lead to the values of the nuclear absorption cross-section σ abs pA for J / ψ and ψ ′. Then, we compare the J / ψ absorption in proton–nucleus and sulphur–uranium interactions, using NA38 data. We obtain that, for the J / ψ , σ abs pA and σ abs SU are compatible, showing that no sizeable additional suppression mechanism is present in S–U collisions, and confirming that the anomalous J / ψ suppression only sets in for Pb–Pb interactions.
The J/PSI production cross section times the branching ratio to MU+ MU- pernucleon-nucleon collision for the differential nuclear targets.
The PSI(3685) production cross section times the branching ratio to MU+ MU-per nucleon-nucleon collision for the differential nuclear targets.
The Drell Yan cross section, divided by the mass number A, and multiplied by the isospin correction factors in the mass interval 2.9 to 4.5 GeV.
Ratio of charmonium to Drell Yan cross section. The third column shows the J/PSI ratio corrected for contamination from PSI(3685) decays.
Ratio between the PSI(3685) and J/PSI cross section.
A partial-wave analysis has been performed of the diffractively produced low-mass ( K ̄ 0 π − π 0 ) system in the reaction K − p → ( K ̄ 0 π − π 0 ) p at 10 and 16 GeV/ c . Thus information complementary to that derived from the K − p → (K − π + π − )p) channel is obtained. The presence of the K ϱ decay mode, besides the dominant K ∗ (890)π mode, for the state J P = 1 + , is confirmed. It is also confirmed that for this 1 + state the assumption of factorization of the amplitude into “production” and “decay” does not hold: the two decay modes K ∗ π and K ϱ have different polarisation properties (helicity is approximately conserved in the t -channel for the first, in the s -channel for the second). The assumption that the ( K ̄ 0 π − π 0 ) system has isospin I = 1 2 has been tested and found to hold. From the cross sections for the various J P states, assuming I = 1 2 , the cross sections for the (K − π + π − ) system are predicted and compared with the experimental ones. In general, agreement is found.
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