Parton-shower effects in polarized deep inelastic scattering
arXiv:2404.07702 · doi:10.1007/JHEP07(2024)177
Abstract
We present a Monte-Carlo program for the simulation of polarized deep inelastic scattering at next-to-leading order in QCD matched to parton shower programs building on an existing implementation of the unpolarized case in the POWHEG BOX package. We discuss extensions of the POWHEG BOX framework necessary to account for polarized initial states and validate the code by detailed comparisons to existing fixed-order results. We then use the new tool to make predictions for the upcoming Electron Ion Collider. We find that parton-shower effects do have an impact on experimentally accessible distributions and improve the agreement with the next-to-next-to-leading order results.
26 pages, 8 figures; v2: published version
References in corpus (15)
- PYTHIA 6.4 Physics and Manual
- An Introduction to PYTHIA 8.2
- Matching NLO QCD computations with Parton Shower simulations: the POWHEG method
- Event generation with SHERPA 1.1
- Tuning PYTHIA 8.1: the Monash 2013 Tune
- A first unbiased global determination of polarized PDFs and their uncertainties
- Evidence for polarization of gluons in the proton
- The Three-Loop Splitting Functions in QCD: The Helicity-Dependent Case
- Vector boson plus one jet production in POWHEG
- The three-loop unpolarized and polarized non-singlet anomalous dimensions from off shell operator matrix elements
- Towards the NNLO evolution of polarised parton distributions
- How well do we know the gluon polarization in the proton?
- Jet production in Polarized DIS at NNLO
- A POWHEG generator for deep inelastic scattering
- Next-to-leading order QCD corrections to hadron+jet production in pp collisions at RHIC
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