Abstract

The identification of hadronically decaying heavy states, such as vector bosons, the Higgs, or the top quark, produced with large transverse boosts has been and will continue to be a central focus of the jet physics program at the Large Hadron Collider (LHC). At a future hadron collider working at an order-of-magnitude larger energy than the LHC, these heavy states would be easily produced with transverse boosts of several TeV. At these energies, their decay products will be separated by angular scales comparable to individual calorimeter cells, making the current jet substructure identification techniques for hadronic decay modes not directly employable. In addition, at the high energy and luminosity projected at a future hadron collider, there will be numerous sources for contamination including initial- and final-state radiation, underlying event, or pile-up which must be mitigated. We propose a simple strategy to tag such “hyper-boosted” objects that defines jets with radii that scale inversely proportional to their transverse boost and combines the standard calorimetric information with charged track-based observables. By means of a fast detector simulation, we apply it to top quark identification and demonstrate that our method efficiently discriminates hadronically decaying top quarks from light QCD jets up to transverse boosts of 20 TeV. Our results open the way to tagging heavy objects with energies in the multi-TeV range at present and future hadron colliders.

Highlights

  • Scaling the jet radius inversely with pT decreases the amount of contamination radiation in the jet, though it does so at the cost of reducing the number of calorimeter cells in the detector that contribute to the jet

  • We summarize the results of this paper in figure 8, illustrating the potential discrimination power for identifying boosted top quarks at the detector of a future high energy proton collider modeled with Delphes

  • We show the hadronically-decaying top quark tagging efficiency as a function of jet pT at fixed mistag rate for jets produced from light quarks and gluons of 5% comparing our method using tracking versus using calorimetry exclusively

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Summary

Dynamic contamination removal

Contamination from initial state radiation (ISR), underlying event (UE) and pile-up is proportional to area of the jet. In addition for a coloured particle such as the top quark, for a fixed jet radius more perturbative QCD radiation is emitted as the pT increases and is collected by the jet algorithm. Such an effect degrades the accuracy of the jet mass reconstruction and the efficiency of tagging the boosted object. The typical angular size of a jet generated by a particle of mass m scales as m/pT , i.e., inversely proportional to the transverse momentum To mitigate all these effects we propose use of a jet radius that scales inversely with the jet pT. Appendices provide details of the Delphes fast detector simulation used throughout this paper and plots of top tagging results for a wide range of jet pT

Observables and methodology
Jet finding and definition
Track-based observables
Detailed studies at fixed pT
Mass distributions
Substructure observables
Conclusions
A Parametrised detector simulation
Tracking
Findings
Calorimetry

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