Jet substructure has emerged to play a central role at the Large Hadron Collider (LHC),
where it has provided numerous innovative new ways to search for new physics and to …

A golden age for heavy-quarkonium physics dawned a decade ago, initiated by the
confluence of exciting advances in quantum chromodynamics (QCD) and an explosion of …

We review the physics basis, main features and use of general-purpose Monte Carlo event
generators for the simulation of proton–proton collisions at the Large Hadron Collider …

A bstract We present a subtraction method utilizing the N-jettiness observable, TN, to
perform QCD calculations for arbitrary processes at next-to-next-to-leading order (NNLO) …

Jet vetoes are essential in many analyses at the LHC and Tevatron. Typical signals have a
specific num<? format?> ber of hard jets or leptons, while backgrounds have additional jets …

We give a factorization formula for the e+ e-thrust distribution d σ/d τ with τ= 1-T based on
the soft-collinear effective theory. The result is applicable for all τ, ie in the peak, tail, and far …

We study proton-(anti) proton collisions at the LHC or Tevatron in the presence of
experimental restrictions on the hadronic final state and for generic parton momentum …

A bstract Observables which discriminate boosted topologies from massive QCD jets are of
great importance for the success of the jet substructure program at the Large Hadron …

Precision predictions for phenomenologically interesting observables such as the\(t\bar {t}\)
invariant mass distribution and forward-backward asymmetry in top-quark pair production at …

Starting from a factorization theorem in Soft-Collinear Effective Theory, the thrust distribution
in e+ e− collisions is calculated including resummation of the next-to-next-to-next-to leading …