6533b820fe1ef96bd127a4d4

RESEARCH PRODUCT

Dipole picture and the nonrelativistic expansion

Miguel Angel Escobedo EspinosaTuomas LappiTuomas Lappi

subject

QuarkParticle physicselectron-ion collisionsPhotonNuclear TheoryQC1-999High Energy Physics::LatticeFOS: Physical scienceshiukkasfysiikka114 Physical sciences01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)Light cone0103 physical sciences010306 general physicsWave functionNuclear ExperimentPhysics010308 nuclear & particles physicsPhysicsHigh Energy Physics::PhenomenologyQuarkoniumDeep inelastic scatteringrelativistic heavy-ion collionsGluonHigh Energy Physics - PhenomenologyDipoleHeavy ionHigh Energy Physics::Experimentydinfysiikka

description

We study exclusive quarkonium production in the dipole picture at next-to-leading order (NLO) accuracy, using the non-relativistic expansion for the quarkonium wavefunction. This process offers one of the best ways to obtain information about gluon distributions at small $x$, in ultraperipheral heavy ion collisions and in deep inelastic scattering. The quarkonium light cone wave functions needed in the dipole picture have typically been available only at tree level, either in phenomenological models or in the nonrelativistic limit. In this paper, we discuss the compatibility of the dipole approach and the non-relativistic expansion and compute NLO relativistic corrections to the quarkonium light-cone wave function in light-cone gauge. Using these corrections we recover results for the NLO decay width of quarkonium to $e^{+}e^{-}$ and we check that the non-relativistic expansion is consistent with ERBL evolution and with B-JIMWLK evolution of the target. The results presented here will allow computing the exclusive quarkonium production rate at NLO once the one loop photon wave function with massive quarks, currently under investigation, is known.

http://urn.fi/URN:NBN:fi:jyu-202003022242