Measurement of the top quark pair production cross section in dilepton final states containing one τ lepton in pp collisions at s$$ \sqrt{s} $$ = 13 TeV
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Author(s)
Sirunyan, A. M
Tumasyan, A.
Adam, W.
Ambrogi, F.
Bergauer, T.
Brandstetter, J.
Dragicevic, M.
Erö, J.
Escalante Del Valle, A.
Flechl, M.
Date Issued
February 28, 2020
Publisher
Springer Berlin Heidelberg
Citation
Journal of High Energy Physics. 2020 Feb 28;2020(2):191
Version
Final published version
Abstract
Abstract
The cross section of top quark pair production is measured in the tt¯→ℓνℓτhντbb¯$$ \mathrm{t}\overline{\mathrm{t}}\to \left(\ell {\nu}_{\ell}\right)\left({\uptau}_{\mathrm{h}}{\nu}_{\uptau}\right)\mathrm{b}\overline{\mathrm{b}} $$ final state, where τh refers to the hadronic decays of the τ lepton, and ℓ is either an electron or a muon. The data sample corresponds to an integrated luminosity of 35.9 fb−1 collected in proton-proton collisions at s$$ \sqrt{s} $$ = 13 TeV with the CMS detector. The measured cross section is σtt¯$$ {\sigma}_{\mathrm{t}\overline{\mathrm{t}}} $$ = 781 ± 7 (stat) ± 62 (syst) ± 20 (lumi) pb, and the ratio of the partial width Γ(t → τντb) to the total decay width of the top quark is measured to be 0.1050 ± 0.0009 (stat) ± 0.0071 (syst). This is the first measurement of the tt¯$$ \mathrm{t}\overline{\mathrm{t}} $$ production cross section in proton-proton collisions at s$$ \sqrt{s} $$ = 13 TeV that explicitly includes τ leptons. The ratio of the cross sections in the ℓτh and ℓℓ final states yields a value Rℓτh/ll$$ {R}_{\ell {\uptau}_{\mathrm{h}}/\mathcal{ll}} $$ = 0.973 ± 0.009 (stat) ± 0.066 (syst), consistent with lepton universality.
MIT Department
Massachusetts Institute of Technology. Department of Physics
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DOI of Published Version
https://doi.org/10.1007/JHEP02(2020)191
