NNLO QCD predictions for Z-boson production in association with a charm jet within the LHCb fiducial region
arXiv:2302.12844 · doi:10.1140/epjc/s10052-023-11530-x
Abstract
We compute next-to-next-to-leading order (NNLO) QCD corrections to neutral vector boson production in association with a charm jet at the LHC. This process is studied in the forward kinematics at TeV, which may provide valuable constraints on the intrinsic charm component of the proton. A comparison is performed between fixed order and NLO predictions matched to a parton shower showing mutual compatibility within the respective uncertainties. NNLO corrections typically lead to a reduction of theoretical uncertainties by a factor of two and the perturbative convergence is further improved through the introduction of a theory-inspired constraint on the transverse momentum of the vector boson plus jet system. A comparison between these predictions with data will require an alignment of a flavour-tagging procedure in theory and experiment that is infrared and collinear safe.
22 pages, 7 figures. v2 matches the published version
References in corpus (9)
- The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations
- An Introduction to PYTHIA 8.2
- Herwig++ Physics and Manual
- LHAPDF6: parton density access in the LHC precision era
- The PDF4LHC21 combination of global PDF fits for the LHC Run III
- Evidence for intrinsic charm quarks in the proton
- NNLO QCD predictions for W+c-jet production at the LHC
- Predictions for -boson production in association with a -jet at
- A Fragmentation Approach to Jet Flavor
Cited by in corpus (5)
- The colourful antenna subtraction method
- Flavoured jet algorithms: a comparative study
- Les Houches 2023 -- Physics at TeV Colliders: Report on the Standard Model Precision Wishlist
- Measurements of the production cross-section for a boson in association with - or -jets in proton-proton collisions at TeV with the ATLAS detector
- Integral of the double-emission eikonal function for a massive and a massless emitter at an arbitrary angle