Abstract

For any factorisation proof, a crucial step is a demonstration of the cancellation of so-called Glauber gluons. We summarise a recent paper in which we demonstrated this cancellation for double Drell–Yan production (the double parton scattering process in which a pair of electroweak gauge bosons is produced), both for the integrated cross section and for the cross section differential in the boson transverse momenta.

Highlights

  • In order to make predictions at the LHC one relies on factorisation formulae that separate the short distance/high-scale dynamics of interest from the low-scale nonperturbative physics

  • Factorisation has been rigorously proven for Drell–Yan production, for the total cross section and cross section differential in the pT of the colour singlet system [8,12,13,14]

  • For the analogous process in double parton scattering, namely double Drell–Yan production, a factorisation formula was written down long ago for the total cross section [21,22] based on the analysis of the lowest-order Feynman diagrams

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Summary

Introduction

In order to make predictions at the LHC one relies on factorisation formulae that separate the short distance/high-scale dynamics of interest from the low-scale nonperturbative physics. Factorisation has been rigorously proven for Drell–Yan production (or, more generally, colour-singlet production), for the total cross section and cross section differential in the pT of the colour singlet system [8,12,13,14]. These factorisation formulae are correct at leading power—i.e. up to corrections of order Λ2QC D/Q2, with Q the hard scale of the process. Serious attempts to rigorously justify these formulae have only begun in recent years [7,15,16,20]

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Glauber Cancellation for One-Gluon Exchange
Glauber Gluon Cancellation at All orders
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