2020
DOI: 10.1007/jhep03(2020)184
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Measuring the top energy asymmetry at the LHC: QCD and SMEFT interpretations

Abstract: The energy asymmetry in top-antitop-jet production is an observable of the top charge asymmetry designed for the LHC. We perform a realistic analysis in the boosted kinematic regime, including effects of the parton shower, hadronization and expected experimental uncertainties. Our predictions at particle level show that the energy asymmetry in the Standard Model can be measured with a significance of 3σ during Run 3, and with more than 5σ significance at the HL-LHC. Beyond the Standard Model the energy asymmet… Show more

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Cited by 10 publications
(14 citation statements)
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“…This allows us to distinguish between the two flavor contractions A and A by combining symmetric and antisymmetric top-antitop observables [43,78]. Kinematic distributions with boosted tops and/or an additional jet in the final state are also sensitive to the relative impact of color-singlet and color-octet coefficients [43,79,80].…”
Section: Four-quark Operatorsmentioning
confidence: 99%
“…This allows us to distinguish between the two flavor contractions A and A by combining symmetric and antisymmetric top-antitop observables [43,78]. Kinematic distributions with boosted tops and/or an additional jet in the final state are also sensitive to the relative impact of color-singlet and color-octet coefficients [43,79,80].…”
Section: Four-quark Operatorsmentioning
confidence: 99%
“…Moreover, it is expected that another LHC experiment, the LHCb, will be able to observe a non-zero tt charge asymmetry at the high-luminosity LHC [121]. Additionally, there is a possibility to measure different types of asymmetries, such as energy asymmetry between the top and antitop quarks [122].…”
Section: Discussion and Outlookmentioning
confidence: 99%
“…To provide a constraint on these additional degrees of freedom, the inclusive pp → t t cross-section measurement from the Tevatron experiments [65] and the pp → t t cross-section at 13 TeV [66] are included in this extended fit. In order to perform a competitive global fit on these additional degrees of freedom we should include more observables, like differential measurements of pp → t t, the t t charge asymmetry [67] or the top energy asymmetry [68]. The purpose of this analysis is just to see the degradation of our limits due to extending the basis, not to find a competitive constraint on C tG and/or the four-fermion operators.…”
Section: Limitations Of the Basismentioning
confidence: 99%