Abstract

Abstract This paper presents measurements of the polarization of W bosons in top quark decays, derived from $ t\overline t $ events with missing transverse momentum, one charged lepton and at least four jets, or two charged leptons and at least two jets. Data from pp collisions at a centre-of-mass energy of 7 TeV were collected with the ATLAS experiment at the LHC and correspond to an integrated luminosity of 1.04 fb−1. The measured fractions of longitudinally, left- and right-handed polarization are F 0 = 0.67 ± 0.07, F L = 0.32 ± 0.04 and F R = 0.01 ± 0.05, in agreement with the Standard Model predictions. As the polarization of the W bosons in top quark decays is sensitive to the Wtb vertex Lorentz structure and couplings, the measurements were used to set limits on anomalous contributions to the Wtb couplings.

Highlights

  • A quark-antiquark pair or into a charged lepton and a neutrino

  • The uncertainty on the normalization of the small background contributions from single top quark and diboson production was estimated to be about 10% and 5%, respectively. The former estimate was based on the difference between the predictions from Monte Carlo (MC)@NLO and MCFM [49], whereas the latter comes from scale and parton distribution functions (PDFs) uncertainties evaluated with MCFM

  • A measurement of the polarization of the W bosons in top quark decays was presented, based on 1.04 fb−1 of data collected with the ATLAS detector in 2011

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Summary

Data and simulation samples

The ATLAS detector [14] at the LHC covers nearly the entire solid angle around the collision point. A three-level trigger system, designed to reduce the event rate from 40 MHz to about 200 Hz, is used to select events of interest

Data sample
Signal and background modelling
Physics object definition
Single-lepton channels
Dilepton channels
Measurement strategies
Measurement using the template method
Measurement using the angular asymmetries
Sources of systematic uncertainty
Detector modelling
Results
Combination
Constraints on the W tb vertex structure
Conclusions

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