Abstract

We present the evaluation of the complete set of NLO corrections to three-jet production at the LHC. To this end we consider all contributions of mathcal{{O}}(alpha _s^nalpha ^m) with n+m=3 and n+m=4. This includes in particular also subleading Born contributions of electroweak origin, as well as electroweak virtual and QED real-radiative corrections. As an application we present results for the three- over two-jet ratio R_{32}. While the impact of non-QCD corrections on the total cross section is rather small, they can exceed -10% for high jet transverse momenta. The R_{32} observable turns out to be very stable against electroweak corrections, receiving absolute corrections below 5% even in the high-p_T region.

Highlights

  • Jet-production processes make up the most abundant final states in hadron–hadron collisions, as carried out at the Large Hadron Collider (LHC)

  • We present the evaluation of the complete set of next-to-leading order (NLO) corrections to three-jet production at the LHC

  • While the latter represents a novel result from our full NLO three-jet calculation, the first is obtained from a dijet computation with identical parameter settings, scale choices and parton density functions (PDFs)

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Summary

Introduction

Jet-production processes make up the most abundant final states in hadron–hadron collisions, as carried out at the Large Hadron Collider (LHC). For hadro-production the next-to-leading order (NLO) QCD corrections are known to up to five-jet final states [1–5]. A first evaluation of the full set of NLO corrections, of QCD and EW origin, for the three-jet inclusive cross section has been quoted in [11].

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