Abstract

A search for new phenomena is presented in final states with two leptons and one or no b-tagged jets. The event selection requires the two leptons to have opposite charge, the same flavor (electrons or muons), and a large invariant mass. The analysis is based on the full run-2 proton-proton collision dataset recorded at a center-of-mass energy of sqrt[s]=13 TeV by the ATLAS experiment at the LHC, corresponding to an integrated luminosity of 139 fb^{-1}. No significant deviation from the expected background is observed in the data. Inspired by the B-meson decay anomalies, a four-fermion contact interaction between two quarks (b, s) and two leptons (ee or μμ) is used as a benchmark signal model, which is characterized by the energy scale and coupling, Λ and g_{*}, respectively. Contact interactions with Λ/g_{*} lower than 2.0 (2.4)TeV are excluded for electrons (muons) at the 95%confidence level, still far below the value that is favored by the B-meson decay anomalies. Model-independent limits are set as a function of the minimum dilepton invariant mass, which allow the results to be reinterpreted in various signal scenarios.

Highlights

  • Lepton flavor universality (LFU) is one of the fundamental predictions of the standard model (SM)

  • The POWHEG-BOX [v1] Monte Carlo (MC) generator [25,26,27,28] was used to simulate at next-to-leading order (NLO) in QCD the inclusive hard-scattering Z=γà → lþl− sample, denoted as Z=γà þ jets, using the CT10 parton distribution function (PDF) set [29]

  • The effect of multiple interactions in the same and neighboring bunch crossings was modeled by overlaying simulated inelastic pp events generated by PYTHIA [8.186] [56] with the A3 tune [57] and the NNPDF2.3lo PDF set [58]

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Summary

Introduction

Lepton flavor universality (LFU) is one of the fundamental predictions of the standard model (SM). The POWHEG-BOX [v1] MC generator [25,26,27,28] was used to simulate at next-to-leading order (NLO) in QCD the inclusive hard-scattering Z=γà → lþl− sample, denoted as Z=γà þ jets, using the CT10 parton distribution function (PDF) set [29].

Results
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