Abstract

We consider double $gg\rightarrow g$ production in the presence of a bias on the unintegrated gluon distribution of the colliding hadron or nuclei. Such bias could be due to the selection of configurations with a greater number of gluons or higher mean transverse momentum squared or, more generally, due to a modified spectral shape of the gluon distribution in the hadrons. Hence, we consider reweighted functional averages over the stochastic ensemble of small-x gluons. We evaluate explicitly the double inclusive gluon transverse momentum spectrum in high-energy collisions, and their azimuthal correlations, for a few simple examples of biases.

Highlights

  • Observables in particle collision experiments are often evaluated in biased event ensembles

  • One may consider a class of events with greater than average multiplicity of produced particles, or events with high transverse energy deposition in a particular rapidity window, and so on

  • DNi d2 kdy refers to the transverse momentum distribution of particles in event i, and dNmb d2 kdy is the average over all events

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Summary

INTRODUCTION

Observables in particle collision experiments are often evaluated in biased event ensembles. We relate expectation values in biased ensembles in high-energy collisions to reweighted averages over the field configurations of small-x gluons in the colliding particles. That our approach allows us to compute expectation values in an ensemble defined by a functional bias on the gluon distribution Xðk⃗ Þ, rather than an ensemble defined with a bias on gluon number, mean transverse momentum, etc. We recompute the so-called “glasma graphs” for a biased gluon distribution different from its expectation value XsðkÞ in the unbiased small-x ensemble. These diagrams for high-pT double gluon production have originally been introduced in Refs. II, we write the two gluon inclusive distribution at high

TWO GLUON INCLUSIVE DISTRIBUTION IN A BIASED ENSEMBLE
SPECIFIC ENSEMBLES
E Þ2bΘðQ2
Transverse momentum dependent boost of the gluon density
E Þ2 : ð65Þ
SUMMARY AND CONCLUSION
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