Abstract

A search for flavour-changing neutral-current processes in top-quark decays is presented. Data collected with the ATLAS detector from proton-proton collisions at the Large Hadron Collider at a centre-of-mass energy of sqrt{s}=13 TeV, corresponding to an integrated luminosity of 36.1 fb−1, are analysed. The search is performed using top-quark pair events, with one top quark decaying through the t → qZ (q = u, c) flavour-changing neutral-current channel, and the other through the dominant Standard Model mode t → bW. Only Z boson decays into charged leptons and leptonic W boson decays are considered as signal. Consequently, the final-state topology is characterized by the presence of three isolated charged leptons (electrons or muons), at least two jets, one of the jets originating from a b-quark, and missing transverse momentum from the undetected neutrino. The data are consistent with Standard Model background contributions, and at 95% confidence level the search sets observed (expected) upper limits of 1.7 × 10−4 (2.4 × 10−4) on the t → uZ branching ratio and 2.4 × 10−4 (3.2 × 10−4) on the t → cZ branching ratio, constituting the most stringent limits to date.

Highlights

  • Background estimation and control regionsThe main sources of background events containing three prompt leptons are: diboson production, ttZ, and tZ processes

  • Z boson decays into charged leptons and leptonic W boson decays are considered as signal

  • A simultaneous fit to the signal region (SR) and all control regions (CRs) defined in table 4 is used to search for a signal from FCNC decays of the top quark

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Summary

ATLAS detector and data samples

The ATLAS experiment [23] is a multi-purpose particle physics detector consisting of several subdetector systems, which almost fully cover the solid angle around the interaction point. It is composed of an inner tracking system close to the interaction point and immersed in a 2 T axial magnetic field produced by a thin superconducting solenoid. The first level is implemented with custom hardware and uses a subset of detector information to reduce the event rate. Triggers with different transverse-momentum thresholds are used to increase the overall efficiency. At high pT the isolation requirements incur small efficiency losses which are recovered by higher-threshold triggers (peT > 60 GeV, peT > 120 GeV, or pμT > 50 GeV for 2015 data and peT > 60 GeV, peT > 140 GeV, or pμT > 50 GeV for 2016 data) without isolation requirements

Signal and background simulation samples
Object reconstruction
Event selection and reconstruction
Background estimation and control regions
Systematic uncertainties
Results
Conclusions
Full Text
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