Journal of High Energy Physics · 2013 · 409 citations · 111 references
Natural SciencesPhysicsNuclear PhysicsParticle PhysicsQuantum MechanicsCollider PhysicsHiggs PhysicsMonte Carlo MethodsMonte Carlo SimulationQuantum ChromodynamicsStrong InteractionCorrelation FunctionsJet PhysicsJet SubstructureTop Quark Physics
Energy correlation functions use particle energies and pairwise angles within a jet, with (N+1)-point correlators sensitive to N‑prong substructure. The paper demonstrates that generalized energy correlation functions serve as a powerful probe of jet substructure. The authors illustrate the method with three Monte Carlo case studies using 2‑, 3‑, and 4‑point correlators for quark/gluon discrimination, boosted W/Z/Higgs identification, and boosted top quark identification. The study finds that these correlation functions obviate explicit subjet identification, better probe soft and collinear features, and that 2‑point correlators are especially powerful for quark/gluon discrimination, while the advantage for boosted 2‑prong resonances varies with resonance mass.
We show how generalized energy correlation functions can be used as a powerful probe of jet substructure. These correlation functions are based on the energies and pair-wise angles of particles within a jet, with (N+1)-point correlators sensitive to N-prong substructure. Unlike many previous jet substructure methods, these correlation functions do not require the explicit identification of subjet regions. In addition, the correlation functions are better probes of certain soft and collinear features that are masked by other methods. We present three Monte Carlo case studies to illustrate the utility of these observables: 2-point correlators for quark/gluon discrimination, 3-point correlators for boosted W/Z/Higgs boson identification, and 4-point correlators for boosted top quark identification. For quark/gluon discrimination, the 2-point correlator is particularly powerful, as can be understood via a next-to-leading logarithmic calculation. For boosted 2-prong resonances the benefit depends on the mass of the resonance.
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