Abstract

AbstractThe results of a search for pair production of supersymmetric partners of the Standard Model third-generation quarks are reported. This search uses 20.1 fb−1ofppcollisions at$ \sqrt{s}=8 $TeV collected by the ATLAS experiment at the Large Hadron Collider. The lightest bottom and top squarks ($ {{\widetilde{b}}_1} $and$ {{\widetilde{t}}_1} $respectively) are searched for in a final state with large missing transverse momentum and two jets identified as originating fromb-quarks. No excess of events above the expected level of Standard Model background is found. The results are used to set upper limits on the visible cross section for processes beyond the Standard Model. Exclusion limits at the 95 % confidence level on the masses of the third-generation squarks are derived in phenomenological supersymmetricR-parity-conserving models in which either the bottom or the top squark is the lightest squark. The$ {{\widetilde{b}}_1} $is assumed to decay via$ {{\widetilde{b}}_1}\to b_{{\chi 1}}^{{\sim 0}} $and the$ {{\widetilde{t}}_1} $via$ {{\widetilde{t}}_1}\to b_{{\chi 1}}^{{\sim \pm }} $, with undetectable products of the subsequent decay of the$ _{{\chi 1}}^{{\sim \pm }} $due to the small mass splitting between the$ _{{\chi 1}}^{{\sim \pm }} $and the$ _{{\chi 1}}^{{\sim 0}} $.

Highlights

  • Background estimateThe dominant SM background processes in the signal regions are the production of W or Z bosons in association with heavy-flavour jets and the production of top-quarks

  • The lightest bottom and top squarks ( ̃b1 and t1 respectively) are searched for in a final state with large missing transverse momentum and two jets identified as originating from b-quarks

  • The ATLAS detector [37] consists of inner tracking devices surrounded by a superconducting solenoid, electromagnetic and hadronic calorimeters and a muon spectrometer with a magnetic field produced by a set of toroids

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Summary

The ATLAS detector and data samples

The ATLAS detector [37] consists of inner tracking devices surrounded by a superconducting solenoid, electromagnetic and hadronic calorimeters and a muon spectrometer with a magnetic field produced by a set of toroids. The inner detector (ID), in combination with a superconducting solenoid magnet with a central field of 2 T, provides precision tracking and momentum measurement of charged particles in a pseudorapidity range |η| < 2.5 and allows efficient identification of jets originating from b-hadron decays using impact parameter measurements and reconstructed secondary decay vertices. The muon spectrometer has separate trigger and high-precision tracking chambers, the latter providing muon identification and momentum measurement for |η| < 2.7. After the application of beam, detector, and data-quality requirements, the total integrated luminosity considered is 20.1 fb−1. Events with final-state electrons or muons that satisfy single-lepton or dilepton triggers are used to define control regions in a total data sample of 20.3 fb−1. A requirement on the transverse momentum pT > 25 GeV is applied to the highest-pT electron or muon to ensure the trigger selection is fully efficient

Simulated event samples
Physics object reconstruction
Event selection
Background estimate
Systematic uncertainties
Results and interpretation
Conclusions
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