Abstract

A search for new particles decaying into a pair of top quarks is performed using proton-proton collision data recorded with the ATLAS detector at the Large Hadron Collider at a center-of-mass energy of $\sqrt{s} = $13 TeV corresponding to an integrated luminosity of 36.1 fb$^{-1}$. Events consistent with top-quark pair production and the fully hadronic decay mode of the top quarks are selected by requiring multiple high transverse momentum jets including those containing $b$-hadrons. Two analysis techniques, exploiting dedicated top-quark pair reconstruction in different kinematic regimes, are used to optimize the search sensitivity to new hypothetical particles over a wide mass range. The invariant mass distribution of the two reconstructed top-quark candidates is examined for resonant production of new particles with various spins and decay widths. No significant deviation from the Standard Model prediction is observed and limits are set on the production cross-section times branching fraction for new hypothetical $Z'$ bosons, dark-matter mediators, Kaluza-Klein gravitons and Kaluza-Klein gluons. By comparing with the predicted production cross-sections, the $Z'$ boson in the topcolor-assisted-technicolor model is excluded for masses up to 3.1$-$3.6 TeV, the dark-matter mediators in a simplified framework are excluded in the mass ranges from 0.8 TeV to 0.9 TeV and from 2.0 TeV to 2.2 TeV, and the Kaluza-Klein gluon is excluded for masses up to 3.4 TeV, depending on the decay widths of the particles.

Highlights

  • ESTIMATIONThe main Standard Model (SM) backgrounds in both the resolved and boosted analyses are from SM production of tt pairs and multijet processes

  • The ATLAS detector at the LHC is a multipurpose, forward-backward symmetric detector2 with nearly full solid angle coverage, as described in Refs. [26,27,28]. It consists of an inner tracking detector (ID) surrounded by a thin superconducting solenoid, a calorimeter system composed of electromagnetic (EM) and hadronic calorimeters, and a muon spectrometer

  • Events containing leptons are included in the complementary search targeting the lepton-plus-jets topology [19] but are rejected in the analyses presented here

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Summary

INTRODUCTION

A cTenhteeLr-aorfg-me HasasdernoenrCgyololifdperffisffi(L1⁄4H1C3),TceuVrr,ehnatlsytohpeeproatteinngtiaatl to discover phenomena beyond the Standard Model (SM) at the TeV scale. The ATLAS search at 13 TeV [19], using data equivalent to 36.1 fb−1, exploits the lepton-plus-jets topology, where a high-pT electron or muon and large missing transverse momentum are required, and excludes masses below 3.0 (3.8) TeV for the new Z0TC2 boson with an intrinsic decay width of Γ 1⁄4 1% (3%) in the topcolor-assisted-technicolor model [2,3]. The Kaluza-Klein (KK) excitation of the graviton GKK predicted in the specific “bulk” RS model [22,23] decaying into tt (see details in Sec. II) was searched for by the ATLAS Collaboration and the mass range from 0.45 to 0.65 TeV is excluded assuming k=M Pl 1⁄4 1, where k is the cpurffivffiffiaffiffiture of the warped extra dimension and M Pl 1⁄4 MPl= 8π is the reduced Planck mass.

SIGNAL MODELS
ATLAS DETECTOR
DATA AND SIMULATION
Object reconstruction and event preselection
Top-quark pair reconstruction
Event categorization
BACKGROUND
All SRs Kaluza-Klein graviton
SYSTEMATIC UNCERTAINTIES
Experimental uncertainties in simulated samples
Background modeling uncertainties
VIII. STATISTICAL ANALYSIS
RESULTS
CONCLUSION
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