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Measurements of top-quark pair differential cross-sections in the e μ channel in pp collisions at √ s = 13 TeV using the ATLAS detector M. Aaboud, G. Aad, B. Abbott [et.al.]

Contributor(s): Aaboud, M | Abbott, B | Chelkov, G. A | Aad, G | Vaniachine, AMaterial type: ArticleArticleSubject(s): ATLAS, детектор | верхние кварки | протон-протонные столкновенияGenre/Form: статьи в журналах Online resources: Click here to access online In: The European physical journal C Vol. 77, № 5. P. 292 (1-30)Abstract: This article presents measurements of tt¯tt¯ differential cross-sections in a fiducial phase-space region, using an integrated luminosity of 3.2 fb−1−1 of proton–proton data at a centre-of-mass energy of s√=13s=13 TeV recorded by the ATLAS experiment at the LHC in 2015. Differential cross-sections are measured as a function of the transverse momentum and absolute rapidity of the top quark, and of the transverse momentum, absolute rapidity and invariant mass of the tt¯tt¯ system. The tt¯tt¯ events are selected by requiring one electron and one muon of opposite electric charge, and at least two jets, one of which must be tagged as containing a b-hadron. The measured differential cross-sections are compared to predictions of next-to-leading order generators matched to parton showers and the measurements are found to be consistent with all models within the experimental uncertainties with the exception of the Powheg-Box++ Herwig++ predictions, which differ significantly from the data in both the transverse momentum of the top quark and the mass of the tt¯tt¯ system.
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This article presents measurements of tt¯tt¯ differential cross-sections in a fiducial phase-space region, using an integrated luminosity of 3.2 fb−1−1 of proton–proton data at a centre-of-mass energy of s√=13s=13 TeV recorded by the ATLAS experiment at the LHC in 2015. Differential cross-sections are measured as a function of the transverse momentum and absolute rapidity of the top quark, and of the transverse momentum, absolute rapidity and invariant mass of the tt¯tt¯ system. The tt¯tt¯ events are selected by requiring one electron and one muon of opposite electric charge, and at least two jets, one of which must be tagged as containing a b-hadron. The measured differential cross-sections are compared to predictions of next-to-leading order generators matched to parton showers and the measurements are found to be consistent with all models within the experimental uncertainties with the exception of the Powheg-Box++ Herwig++ predictions, which differ significantly from the data in both the transverse momentum of the top quark and the mass of the tt¯tt¯ system.

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