0000000001205695

AUTHOR

G. Beuf

showing 3 related works from this author

Massive quarks in NLO dipole factorization for DIS : Longitudinal photon

2021

In this work, we will present the first complete calculation of the one-loop longitudinal photon-to-quark-antiquark light cone wave function, with massive quarks. The quark masses are renormalized in the pole mass scheme. The result is used to calculate the next-to-leading order correction to the high energy Deep Inelastic Scattering longitudinal structure function on a dense target in the dipole factorization framework. For massless quarks the next-to-leading order correction was already known to be sizeable, and our result makes it possible to evaluate it also for massive quarks.

QuarkParticle physicsPhotonNuclear TheoryHigh Energy Physics::LatticeNuclear TheoryQUANTUM ELECTRODYNAMICSFOS: Physical scienceshiukkasfysiikka01 natural sciences114 Physical sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)FactorizationLight coneINFINITE-MOMENTUM0103 physical sciencesSCATTERINGPICTURE010306 general physicsWave functionPhysics010308 nuclear & particles physicskvarkitLIGHT-FRONT QCDHigh Energy Physics::PhenomenologyDeep inelastic scatteringINVARIANCEMassless particleDipoleHigh Energy Physics - PhenomenologykvanttiväridynamiikkaHigh Energy Physics::ExperimentBK EVOLUTION
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Diffractive deep inelastic scattering at NLO in the dipole picture: The qq¯g contribution

2022

Physical Review D
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Diffractive deep inelastic scattering at NLO in the dipole picture: The qq¯g contribution

2022

We calculate the contribution from the qq¯g state production to the diffractive cross sections in deep inelastic scattering at high energy. The obtained cross section is finite by itself and a part of the full next-to-leading order result for the diffractive structure functions. We perform the calculation in exact kinematics in the eikonal limit, and show that the previously known high-Q2 and large MX2 results for the structure functions can be extracted from our results in the appropriate limits. We furthermore discuss the steps required to obtain the full next-to-leading order results for the structure functions.

sirontahiukkasfysiikka114 Physical sciencesPhysical Review
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