Abstract

A search for the production of single-top-quarks in association with missing energy is performed in proton–proton collisions at a centre-of-mass energy of sqrt{s}=mathrm {8~TeV} with the ATLAS experiment at the large hadron collider using data collected in 2012, corresponding to an integrated luminosity of 20.3 fb^{-1}. In this search, the W boson from the top quark is required to decay into an electron or a muon and a neutrino. No deviation from the standard model prediction is observed, and upper limits are set on the production cross-section for resonant and non-resonant production of an invisible exotic state in association with a right-handed top quark. In the case of resonant production, for a spin-0 resonance with a mass of 500 GeV, an effective coupling strength above 0.15 is excluded at 95,% confidence level for the top quark and an invisible spin-1/2 state with mass between 0 and 100 GeV. In the case of non-resonant production, an effective coupling strength above 0.2 is excluded at 95,% confidence level for the top quark and an invisible spin-1 state with mass between 0 and 657 GeV.

Highlights

  • Many theories beyond the standard model (BSM) predict enhanced production of events with large missing energy in association with a single reconstructed object

  • This paper presents a search for singly produced top quarks in association with significant missing energy, corresponding to the associated production of one or several undetected neutral particles, and without any other reconstructed object

  • Processes involving top quarks are sensitive to BSM physics, due to the large mass of this standard model (SM) particle which is close to the electroweak symmetrybreaking scale. No such process is possible in the SM at tree level: the direct production of a top quark and a Z boson decaying into a pair of neutrinos, without any additional quark, is suppressed by the Glashow–Iliopoulos–Maiani mechanism [7]

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Summary

Introduction

Many theories beyond the standard model (BSM) predict enhanced production of events with large missing energy in association with a single reconstructed object Such events have been searched for at the large hadron collider (LHC), when the single object is either a photon [1,2], a jet [3,4], or a W or Z boson [5,6]. No such process is possible in the SM at tree level: the direct production of a top quark and a Z boson decaying into a pair of neutrinos, without any additional quark, is suppressed by the Glashow–Iliopoulos–Maiani mechanism [7].

Signal models
Data and Monte Carlo samples
Selection and background estimation
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Sample size
Systematic uncertainties
Object modelling
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Background normalisation
Results and interpretation
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Full Text
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