Abstract

This Letter presents direct searches for lepton flavour violation in Higgs boson decays, H→eτ and H→μτ, performed with the ATLAS detector at the LHC. The searches are based on a data sample of proton–proton collisions at a centre-of-mass energy s=13 TeV, corresponding to an integrated luminosity of 36.1 fb−1. No significant excess is observed above the expected background from Standard Model processes. The observed (median expected) 95% confidence-level upper limits on the lepton-flavour-violating branching ratios are 0.47% (0.34−0.10+0.13%) and 0.28% (0.37−0.10+0.14%) for H→eτ and H→μτ, respectively.

Highlights

  • The search for processes beyond the Standard Model (SM) is one of the main goals of the Large Hadron Collider (LHC) programme at CERN

  • The measured values are obtained by the fit to data, while the expected values are determined by the fit to a background-only sample

  • These limits are more stringent by a factor of 2 (5) than the corresponding√limits for the H → eτ (H → μτ ) decay determined by ATLAS at s = 8 TeV

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Summary

Introduction

The search for processes beyond the Standard Model (SM) is one of the main goals of the Large Hadron Collider (LHC) programme at CERN. A possible sign of such processes is lepton flavour violation (LFV) in decays of the Higgs boson [1,2]. The dataset corresponds to an integrated luminosity of 36.1 fb−1. (1.43%) on the H → eτ (H → μτ ) branching ratio√(B) with a 95% confidence level (CL) using Run 1 data collected at s = 8 TeV, corresponding to an integrated luminosity of 20.3 fb−1. √ing ratios of 0.61% s = 13 TeV, with and 0.25%, respectively, using data collected an integrated luminosity of 35.9 fb−1 [16]. The dilepton final state τ only considers pairs of different-flavour leptons. It consists of an inner tracking detector covering the range |η| < 2.5, surrounded by a superconducting solenoid providing a 2 T axial magnetic field, high-granularity electromagnetic (|η| < 3.2) and hadronic calorimeters (|η| < 4.9), and a muon spectrometer (MS) which covers the range |η| < 2.7 and includes fast trigger chambers (|η| < 2.4) and superconducting toroidal magnets

Simulation samples
Object reconstruction
Event selection and categorization
Background modelling
Systematic uncertainties
Statistical analysis
Results
Conclusions
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