Abstract

A search is presented for the production of new heavy quarks that decay to a $Z$ boson and a third-generation Standard Model quark. In the case of a new charge +2/3 quark ($T$), the decay targeted is $T \rightarrow Zt$, while the decay targeted for a new charge -1/3 quark ($B$) is $B \rightarrow Zb$. The search is performed with a dataset corresponding to 20.3 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}=8$ TeV recorded in 2012 with the ATLAS detector at the CERN Large Hadron Collider. Selected events contain a high transverse momentum $Z$ boson candidate reconstructed from a pair of oppositely charged same-flavor leptons (electrons or muons), and are analyzed in two channels defined by the absence or presence of a third lepton. Hadronic jets, in particular those with properties consistent with the decay of a $b$-hadron, are also required to be present in selected events. Different requirements are made on the jet activity in the event in order to enhance the sensitivity to either heavy quark pair production mediated by the strong interaction, or single production mediated by the electroweak interaction. No significant excess of events above the Standard Model expectation is observed, and lower limits are derived on the mass of vector-like $T$ and $B$ quarks under various branching ratio hypotheses, as well as upper limits on the magnitude of electroweak coupling parameters.

Highlights

  • Background modelingThe SM backgrounds in this analysis are predicted primarily with simulated samples normalized to next-to-leading order, or higher, cross-section calculations

  • A search is presented for the production of new heavy quarks that decay to a Z boson and a third-generation Standard Model quark

  • Different requirements are made on the jet activity in the event in order to enhance the sensitivity to either heavy quark pair production mediated by the strong interaction, or single production mediated by the electroweak interaction

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Summary

ATLAS detector

The ATLAS detector [24] identifies and measures the momentum and energy of particles created in proton-proton (pp) collisions at the LHC It has a cylindrical geometry, approximate 4π solid angle coverage, and consists of particle-tracking detectors, electromagnetic and hadronic calorimeters, and a muon spectrometer. At small radii transverse to the beamline, the inner tracking system utilizes fine-granularity pixel and microstrip detectors designed to provide precision track impact parameter and secondary vertex measurements. These silicon-based detectors cover the pseudorapidity range |η| < 2.5.1 A gas-filled strawtube tracker complements the silicon tracker at larger radii. Liquid-argon calorimetry with copper absorbers is employed in the hadronic end-cap calorimeters, which cover the region 1.5 < |η| < 3.2. The first-level trigger system is implemented in custom electronics, using a subset of the detector information to reduce the event rate to a design value of 75 kHz, while the second and third levels use software algorithms running on PC farms to yield a recorded event rate of approximately 400 Hz

Reconstruction of physics objects
Data sample and event preselection
Heavy quark pair production and vector-like quark decay modes
Electroweak single production
Background modeling
Search strategies
Comparison of the data to the predictions
Dilepton channel analysis targeting the pair-production hypotheses
Trilepton channel analysis targeting the pair-production hypotheses
ATLAS 7 6 5 4 3 2 1
Modified selection criteria to target the single-production hypotheses
35 ATLAS 30 25 20
Systematic uncertainties
10 Results
10.1 Limits on the pair-production hypotheses
10.2 Limits on the single-production hypotheses
11 Conclusions
Full Text
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