Showing 3 of 943 results
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. $M(\text{t}\bar{\text{t}})$.
The production of $\Upsilon$(2S) and $\Upsilon$(3S) mesons in lead-lead (PbPb) and proton-proton (pp) collisions is studied in their dimuon decay channel using the CMS detector at the LHC. The $\Upsilon$(3S) meson is observed for the first time in PbPb collisions, with a significance above five standard deviations. The ratios of yields measured in PbPb and pp collisions are reported for both the $\Upsilon$(2S) and $\Upsilon$(3S) mesons, as functions of transverse momentum and PbPb collision centrality. These ratios, when appropriately scaled, are significantly less than unity, indicating a suppression of $\Upsilon$ yields in PbPb collisions. This suppression increases from peripheral to central PbPb collisions. Furthermore, the suppression is stronger for $\Upsilon$(3S) mesons compared to $\Upsilon$(2S) mesons, extending the pattern of sequential suppression of quarkonium states in nuclear collisions previously seen for the $\psi$/J, $\psi$(2S), $\Upsilon$(1S), and $\Upsilon$(2S) mesons.
Measured $R_\text{AA}$ for the $\Upsilon(2S)$ state as functions of PbPb collision centrality, integrated over the full kinematic range $p_\text{T}$ < 30 GeV/c and |y| < 2.4. The global uncertainty "PP MB" represents the pp luminosity and PbPb $N_\text{MB}$ combined uncertainties, whereas the global uncertainty "PP 2S" corresponds to the uncertainty on the $\Upsilon(2S)$ pp yields.
Measured $R_\text{AA}$ for the $\Upsilon(3S)$ state as functions of PbPb collision centrality, integrated over the full kinematic range $p_\text{T}$ < 30 GeV/c and |y| < 2.4. The global uncertainty "PP MB" represents the pp luminosity and PbPb $N_\text{MB}$ combined uncertainties, whereas the global uncertainty "PP 3S" corresponds to the uncertainty on the $\Upsilon(3S)$ pp yields.
Measured $R_\text{AA}$ for the$\Upsilon(2S)$ state in the 0–90% centrality interval, integrated over the full kinematic range $p_\text{T}$ < 30 GeV/c and |y| < 2.4. The global uncertainty "PP MB" represents the pp luminosity and PbPb $N_\text{MB}$ combined uncertainties, whereas the global uncertainty "PP 2S" corresponds to the uncertainty on the $\Upsilon(2S)$ pp yields.
Measured $R_\text{AA}$ for the $\Upsilon(3S)$ state in the 0–90% centrality interval, integrated over the full kinematic range $p_\text{T}$ < 30 GeV/c and |y| < 2.4. The global uncertainty "PP MB" represents the pp luminosity and PbPb $N_\text{MB}$ combined uncertainties, whereas the global uncertainty "PP 3S" corresponds to the uncertainty on the$\Upsilon(3S)$ pp yields.
Measured $R_\text{AA}$ for the $\Upsilon(2S)$ state as functions of transverse momentum $p_\text{T}$, integrated over the rapidity range of |y| < 2.4 and the 0–90% centrality interval. The global uncertainty combines the uncertainties of $T_\text{AA}$ , pp luminosity, and PbPb $N_\text{MB}$.
Measured $R_\text{AA}$ for the $\Upsilon(3S)$ state as functions of transverse momentum $p_\text{T}$, integrated over the rapidity range of |y| < 2.4 and the 0–90% centrality interval. The global uncertainty combines the uncertainties of $T_\text{AA}$ , pp luminosity, and PbPb $N_\text{MB}$.
The double ratios of $\Upsilon(3S)$ /$\Upsilon(2S)$ as functions of PbPb collision centrality, integrated over the full kinematic range $p_\text{T}$ < 30 GeV/c and |y| < 2.4. The global uncertainty represents the combined systematic and statistical uncertainties from pp data.
The double ratios of $\Upsilon(3S)$ /$\Upsilon(2S)$ in the 0–90% centrality interval, integrated over the full kinematic range $p_\text{T}$ < 30 GeV/c and |y| < 2.4. The global uncertainty represents the combined systematic and statistical uncertainties from pp data.
The double ratios of $\Upsilon(3S)$ /$\Upsilon(2S)$ as functions of transverse momentum $p_\text{T}$, integrated over the rapidity range of |y| < 2.4 and the 0–90% centrality interval.
Yields for $\Upsilon(2S)$ mesons in PbPb collisions in centrality $0--90\%$ and $|y| < 2.4$, corrected for acceptance and efficiency, and normalized by the nuclear thickness function $\langle T_{AA} \rangle$ and the number of minimum bias events $N_{MB}$. The numbers are in units of pb$/GeV/c$.
Yields for $\Upsilon(2S)$ mesons in PbPb collisions in $p_\text{T} < 30GeV/c$ and $|y| < 2.4$, corrected for acceptance and efficiency, and normalized by the nuclear thickness function $\langle T_{AA} \rangle$ and the number of minimum bias events $N_{MB}$. The numbers are in units of pb$/GeV/c$.
Yields for $\Upsilon(3S)$ mesons in PbPb collisions in centrality $0--90\%$ and $|y| < 2.4$, corrected for acceptance and efficiency, and normalized by the nuclear thickness function $\langle T_{AA} \rangle$ and the number of minimum bias events $N_{MB}$. The numbers are in units of pb$/GeV/c$.
Yields for $\Upsilon(3S)$ mesons in PbPb collisions in $p_\text{T} < 30GeV/c$ and $|y| < 2.4$, corrected for acceptance and efficiency, and normalized by the nuclear thickness function $\langle T_{AA} \rangle$ and the number of minimum bias events $N_{MB}$. The numbers are in units of pb$/GeV/c$.
Yields for $\Upsilon(1S)$ mesons in PbPb collisions in $p_\text{T} < 30GeV/c$ and $|y| < 2.4$, corrected for acceptance and efficiency, and normalized by the nuclear thickness function $\langle T_{AA} \rangle$ and the number of minimum bias events $N_{MB}$. The numbers are in units of pb$/GeV/c$. The values and global integrated luminosity uncertainty are quoted from data taken from CMS in 2018 LHC PbPb run.
None
No description provided.
No description provided.
No description provided.
No description provided.
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.
About HEPData Submitting to HEPData HEPData File Formats HEPData Coordinators HEPData Terms of Use HEPData Cookie Policy
Status
Email
Forum
Twitter
GitHub
Copyright ~1975-Present, HEPData | Powered by Invenio, funded by STFC, hosted and originally developed at CERN, supported and further developed at IPPP Durham.