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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. 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. 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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Correspondence to Shota Tsiskaridze .

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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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