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Infrared structure of e+e−→2 jets at NNLO

2004/03/31 by A. Gehrmann–De Ridder, A. Gehrmann-De Ridder, T. Gehrmann +1 · 189 citations
Mathematics · Physics and Astronomy · #Algorithm #Annihilation #Factorization #Gluon #Hadron #High-Energy Particle Collisions Research #Infrared #Jet (fluid) #Mathematics #Observable #Particle physics #Particle physics theoretical and experimental studies #Parton #Phase space #Physics #Quantum Chromodynamics and Particle Interactions #Quantum chromodynamics #Quantum mechanics #hep-ph

paper · pdf · doi:10.1016/j.nuclphysb.2004.05.017

published in Nuclear Physics B 691(1-2), 195-222 (Elsevier BV) · 21 pages, LaTeX, misprints in formulae corrected, minor changes to text

arxiv created 2004/04/06 · openalex publication_date 2004/05/30 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05

Abstract

The production of two jets is the simplest exclusive quantum chromodynamics process in electron-positron annihilation. Using this process, we examine the structure of next-to-next-to-leading order (NNLO) corrections to jet production observables. We derive a subtraction formalism including double real radiation at tree level and single real radiation at one loop. For two-jet production, these subtraction terms coincide with the full matrix elements, thus highlighting the phase space structure of the subtraction procedure. We then analytically compute the infrared singularities arising from each partonic channel. For the purely virtual (two-parton) NNLO corrections, these take the well known form predicted by Catani's infrared factorization formula. We demonstrate that individual terms in the infrared factorization formula can be identified with infrared singular terms from three- and four-parton final states, leaving only single poles and a contribution from the one-loop soft gluon current, which subsequently cancels between the three- and four-parton final states. Summing over all different final states, we observe an explicit cancellation of all infrared poles and recover the known two-loop correction to the hadronic R-ratio.

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