Abstract

Searches for the Higgs boson decays H→ee and H→eμ are performed using data corresponding to an integrated luminosity of 139fb−1 collected with the ATLAS detector in pp collisions at s=13 TeV at the LHC. No significant signals are observed, in agreement with the Standard Model expectation. For a Higgs boson mass of 125 GeV, the observed (expected) upper limit at the 95% confidence level on the branching fraction B(H→ee) is 3.6×10−4 (3.5×10−4) and on B(H→eμ) is 6.2×10−5 (5.9×10−5). These results represent improvements by factors of about five and six on the previous best limits on B(H→ee) and B(H→eμ) respectively.

Highlights

  • The discovery of a heavy scalar particle by ATLAS and CMS [1, 2] provided experimental confirmation of the Englert–Brout–Higgs mechanism [3,4,5,6,7,8], which spontaneously breaks electroweak (EW)gauge symmetry and generates mass terms for the W and Z gauge bosons

  • The observed dielectron mass spectra are divided into 200 mee bins in each of the seven categories and signal yields are obtained in a simultaneous maximum-likelihood fit

  • The Higgs boson production cross sections are assumed to be as predicted in the Standard Model

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Summary

Introduction

The discovery of a heavy scalar particle by ATLAS and CMS [1, 2] provided experimental confirmation of the Englert–Brout–Higgs mechanism [3,4,5,6,7,8], which spontaneously breaks electroweak (EW). This Letter presents the first ATLAS searches for H → ee and for the lepton-flavour-violating decay H → eμ using the full Run. 2 datase√t of proton–proton ergy of s = 13 TeV, with (pp) collisions an integrated at a centre-of-mass enluminosity of 139 fb−1. There are strong indirect constraints on the off-diagonal Yeμ coupling, the strongest derived from limits on the branching fraction of μ → eγ and the electric dipole moment of the electron [19]. These indirect constraints assume SM values for the as yet unmeasured Yee and Yμμ. The production of top quarks, dibosons (mainly through W W → eνeμνμ), W +jets and multijet events, with jets misidentified as leptons, are more important than in the ee search

ATLAS detector
Simulated event samples
Event selection
Signal and background parameterisation
Systematic uncertainties
Results
Conclusion
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