Abstract

Measurements are presented of differential cross-sections for top quark pair production in pp collisions at sqrt(s) = 7 TeV relative to the total inclusive top quark pair production cross-section. A data sample of 2.05/fb recorded by the ATLAS detector at the Large Hadron Collider is used. Relative differential cross-sections are derived as a function of the invariant mass, the transverse momentum and the rapidity of the top quark pair system. Events are selected in the lepton (electron or muon) + jets channel. The background-subtracted differential distributions are corrected for detector effects, normalized to the total inclusive top quark pair production cross-section and compared to theoretical predictions. The measurement uncertainties range typically between 10% and 20% and are generally dominated by systematic effects. No significant deviations from the Standard Model expectations are observed.

Highlights

  • The top quark [1, 2] is the most massive known fundamental constituent of matter

  • This paper focuses on three observables of the ttsystem: the invariant mass, the transverse momentum and the rapidity

  • The multijet background with misidentified and non-prompt leptons in both the e + jets and μ + jets channels is evaluated with a matrix method, which relies on defining loose and tight lepton samples [3, 45] and measuring the fractions of real and fake loose leptons that are selected as tight leptons

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Summary

Introduction

The top quark [1, 2] is the most massive known fundamental constituent of matter. Its unexplained large mass suggests an important connection to the electroweak symmetry breaking mechanism. The main expected backgrounds in the lepton + jets channel are W + jets which can give rise to the same final state as the ttsignal, and fake leptons. They are both estimated using auxiliary measurements. The multijet background with misidentified and non-prompt leptons (referred to collectively as fake leptons) in both the e + jets and μ + jets channels is evaluated with a matrix method, which relies on defining loose and tight lepton samples [3, 45] and measuring the fractions of real (εreal) and fake (εfake) loose leptons that are selected as tight leptons. Contributions from W + jets and Z + jets backgrounds are subtracted in the control regions using Monte Carlo simulation

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