Abstract
This chapter describes the event selection criteria, the data samples and the modeling of the signal and background samples used in the analysis.
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Notes
- 1.
\(\mathop m\nolimits _\mathrm{{T}}^\mathrm{{W}}= \sqrt{2 p^\ell _{\mathrm T} E_{\mathrm {T}}^{\mathrm {miss}}(1-\cos \Delta \phi )}\), where \(p^\ell _{\mathrm T}\) is the transverse momentum (energy) of the muon (electron) and \(\Delta \phi \) is the azimuthal angle separation between the lepton and the direction of the missing transverse momentum.
- 2.
The flavor of the jet is defined by looking at partons with \(p_\mathrm{{T}}> 5GeV\) within \(\Delta R < 0.3\) around the jet direction. If a b-quark is found, the jet is labeled as “b”. If no b-quarks are found, c-quarks are considered and if found, the jet is labeled as “c”. The remaining jets are labeled as “light”.
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Tsiskaridze, S. (2017). Event Samples and Preselection. In: Search for Flavor-Changing Neutral Current Top Quark Decays t → Hq, with H → bb̅ , in pp Collisions at √s = 8 TeV with the ATLAS Detector. Springer Theses. Springer, Cham. https://doi.org/10.1007/978-3-319-63414-2_5
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