The cross sections for the production of single top quarks and antiquarks in the $t$ channel, and their ratio, are measured in proton-proton collisions at a center-of-mass energy of $13~\mathrm{TeV}$. The full data set recorded in 2016 by the CMS detector at the LHC is analyzed, corresponding to an integrated luminosity of $35.9~\mathrm{fb}^{-1}$. Events with one muon or electron and two jets are selected, where one of the two jets is identified as originating from a bottom quark. A multivariate discriminator exploiting several kinematic variables is applied to separate signal from background events. The ratio $R_{t\mathrm{\text{-}ch.}}$ of the cross sections is measured to be $1.65 \pm0.02\,\text{(stat)} \pm0.04\,\text{(syst)}$. The total cross section for the production of single top quarks or antiquarks is measured to be $219.0 \pm1.5\,\text{(stat)} \pm33.0\,\text{(syst)} \,\mathrm{pb}$ and the absolute value of the CKM matrix element $V_{\mathrm{tb}}$ is determined to be $1.00 \pm0.05\,\text{(exp)} \pm0.02 \,\text{(theo)}$. All results are in agreement with the standard model predictions.
The measured cross section of top quark production in $t$-channel. The first uncertainty is the statistical, the second is due to profiled systematic sources, the third is due to the sources describing signal modelling (externalized), and the last due to the integrated luminosity (externalized).
The measured cross section of top antiquark production in $t$-channel. The first uncertainty is the statistical, the second is due to profiled systematic sources, the third is due to the sources describing signal modelling (externalized), and the last due to the integrated luminosity (externalized).
The measured inclusive cross section of production of the top quarks and antiquarks in $t$-channel. The first uncertainty is the statistical, the second is due to profiled systematic sources, the third is due to the sources describing signal modelling (externalized), and the last due to the integrated luminosity (externalized).
A measurement is presented of the associated production of a single top quark and a W boson in proton-proton collisions at $\sqrt{s}=$ 13 TeV by the CMS Collaboration at the CERN LHC. The data collected corresponds to an integrated luminosity of 35.9 fb$^{-1}$. The measurement is performed using events with one electron and one muon in the final state along with at least one jet originated from a bottom quark. A multivariate discriminant, exploiting the kinematic properties of the events, is used to separate the signal from the dominant $\mathrm{t\overline{t}}$ background. The measured cross section of 63.1 $\pm$ 1.8 (stat) $\pm$ 6.4 (syst) $\pm$ 2.1 (lumi) pb is in agreement with the standard model expectation.
The measured total cross sections based on the $\rm{e}^\pm \mu^\mp$ decay channel. The first uncertainty is the statistical, the second is the systematic, and the last due to the integrated luminosity.
Summary of the individual contributions to the uncertainty in the $\sigma_{tW}$ measurement.
A measurement of the top quark mass is performed using a data sample enriched with single top quark events produced in the $t$ channel. The study is based on proton-proton collision data, corresponding to an integrated luminosity of 35.9 fb$^{-1}$, recorded at $\sqrt{s}$ = 13 TeV by the CMS experiment at the LHC in 2016. Candidate events are selected by requiring an isolated high-momentum lepton (muon or electron) and exactly two jets, of which one is identified as originating from a bottom quark. Multivariate discriminants are designed to separate the signal from the background. Optimized thresholds are placed on the discriminant outputs to obtain an event sample with high signal purity. The top quark mass is found to be 172.13 $^{+0.76}_{-0.77}$ GeV, where the uncertainty includes both the statistical and systematic components, reaching sub-GeV precision for the first time in this event topology. The masses of the top quark and antiquark are also determined separately using the lepton charge in the final state, from which the mass ratio and difference are determined to be 0.9952 $^{+0.0079}_{-0.0104}$ and 0.83 $^{+1.79}_{-1.35}$ GeV, respectively. The results are consistent with $CPT$ invariance.
The top quark mass measured inclusive of lepton flavor and charge. The uncertainties are given in two parts, the first is the combination of statistical (stat) and profiled systematic (prof) uncertainties and the second is the externalized systematic (ext) uncertainties.
Top quark mass measured inclusive of lepton flavor and for positively charged lepton.
Top quark mass measured inclusive of lepton flavor and for negatively charged lepton.