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  • Measurement of $$\hbox {t}{...
    T. Bergauer; J. Erö; M. Spanring; E. A. De Wolf; A. Popov; P. David; P. Vischia; M. Shopova; Y. Wang; Z. Antunovic; M. Raidal; J. K. Heikkilä; S. Ganjour; V. Cherepanov; M. Gouzevitch; R. Fischer; T. Pook; A. Nehrkorn; O. Behnke; C. Kleinwort; M. Missiroli; G. Mittag; D. Pitzl; D. Gonzalez; S. Kudella; G. Karathanasis; P. Gianneios; K. Manitara; S. Bansal; S. B. Beri; R. B. Garg; T. Sarkar; P. K. Behera; R. Chudasama; T. Aziz; S. Chauhan; M. Felcini; L. Viliani; N. Cavallo; G. Galati; A. Boletti; T. Dorigo; A. T. Meneguzzo; G. Zumerle; C. Cecchi; R. Leonardi; M. Menichelli; C. Mariotti; D. C. Son; T. J. Kim; D. Gyun; I. C. Park; M. Górski; V. Kim; I. Smirnov; A. Pashenkov; J. M. Hernandez; A. Triossi; S. Sanchez Cruz; B. Chazin Quero; J. Duarte Campderros; A. Lopez Virto; M. Dobson; F. Moortgat; G. Petrucciani; M. Marionneau; G. Karapinar; E. Gülmez; Y. Komurcu; E. Olaiya; D. Petyt; M. Della Negra; T. Virdee; P. Kyberd; N. Pastika; Z. Mao; J. W. Gary; G. Karapostoli; J. G. Branson; M. Pieri; V. Sharma; S. Xie; J. Duarte; J. Hanlon; F. Ravera; D. Acosta; O. Evdokimov; J. Kunkle; T. Gunter; R. Goldouzian; L. Antonelli; A. Kalogeropoulos; S. Kwan; J. Salfeld-Nebgen; R. Demina; P. Tan; D. Sheffield; T. Kamon; Z. Wang; J. Sturdy

    The European physical journal. C, Particles and fields, 07/2020, Letnik: 80, Številka: 7
    Journal Article

    Abstract Normalised multi-differential cross sections for top quark pair ($$\hbox {t}{\bar{\hbox {t}}}$$ tt¯ ) production are measured in proton-proton collisions at a centre-of-mass energy of 13$$\,{\text {TeV}}$$ TeV using events containing two oppositely charged leptons. The analysed data were recorded with the CMS detector in 2016 and correspond to an integrated luminosity of $$35.9{\,{\text {fb}}^{-1}} $$ 35.9fb-1 . The double-differential $$\hbox {t}{\bar{\hbox {t}}}$$ tt¯ cross section is measured as a function of the kinematic properties of the top quark and of the $$\hbox {t}{\bar{\hbox {t}}}$$ tt¯ system at parton level in the full phase space. A triple-differential measurement is performed as a function of the invariant mass and rapidity of the $$\hbox {t}{\bar{\hbox {t}}}$$ tt¯ system and the multiplicity of additional jets at particle level. The data are compared to predictions of Monte Carlo event generators that complement next-to-leading-order (NLO) quantum chromodynamics (QCD) calculations with parton showers. Together with a fixed-order NLO QCD calculation, the triple-differential measurement is used to extract values of the strong coupling strength $$\alpha _{S}$$ αS and the top quark pole mass ($$m_{{\text {t}}}^{{\text {pole}}}$$ mtpole ) using several sets of parton distribution functions (PDFs). The measurement of $$m_{{\text {t}}}^{{\text {pole}}}$$ mtpole exploits the sensitivity of the $$\hbox {t}{\bar{\hbox {t}}}$$ tt¯ invariant mass distribution to $$m_{{\text {t}}}^{{\text {pole}}}$$ mtpole near the production threshold. Furthermore, a simultaneous fit of the PDFs, $$\alpha _{S}$$ αS , and $$m_{{\text {t}}}^{{\text {pole}}}$$ mtpole is performed at NLO, demonstrating that the new data have significant impact on the gluon PDF, and at the same time allow an accurate determination of $$\alpha _{S}$$ αS and $$m_{{\text {t}}}^{{\text {pole}}}$$ mtpole . The values $$\alpha _{S}(m_{{\text {Z}}}) = 0.1135{}^{+0.0021}_{-0.0017}$$ αS(mZ)=0.1135-0.0017+0.0021 and $$m_{{\text {t}}}^{{\text {pole}}} = 170.5 \pm 0.8 \,{\text {GeV}} $$ mtpole=170.5±0.8GeV are extracted, which account for experimental and theoretical uncertainties, the latter being estimated from NLO scale variations. Possible effects from Coulomb and soft-gluon resummation near the $$\hbox {t}{\bar{\hbox {t}}}$$ tt¯ production threshold are neglected in these parameter extractions. A rough estimate of these effects indicates an expected correction of $$m_{{\text {t}}}^{{\text {pole}}}$$ mtpole of the order of $$+1 \,{\text {GeV}} $$ +1GeV , which can be regarded as additional theoretical uncertainty in the current $$m_{{\text {t}}}^{{\text {pole}}}$$ mtpole extraction.