W±Z production at NNLO QCD and NLO EW matched to parton showers with MiNNLOPS

被引:0
作者
Jonas M. Lindert
Daniele Lombardi
Marius Wiesemann
Giulia Zanderighi
Silvia Zanoli
机构
[1] University of Sussex,Department of Physics and Astronomy
[2] Max-Planck-Institut für Physik,Physik
[3] Technische Universität München,Department
来源
Journal of High Energy Physics | / 2022卷
关键词
Electroweak Precision Physics; Higher-Order Perturbative Calculations; Parton Shower; Resummation;
D O I
暂无
中图分类号
学科分类号
摘要
We consider W±Z production in hadronic collisions and present high-precision predictions in QCD and electroweak (EW) perturbation theory matched to parton showers. To this end, we match next-to-next-to-leading order QCD corrections to parton showers using the MiNNLOPS method and consistently combine them with next-to-leading order EW corrections matched to parton showers. This is the first time such accuracy in the event generation is achieved for any collider process, and we study in detail the impact of different choices in the combination of QCD and EW corrections as well as QCD and QED showers. Spin correlations, interferences and off-shell effects are retained by considering the full leptonic processes pp→ℓ+ℓ−ℓ′±νℓ′\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ pp\to {\ell}^{+}{\ell}^{-}{\ell}^{\prime \pm }{\nu}_{\ell}^{\prime } $$\end{document} with ℓ′ ≠ ℓ and ℓ′ = ℓ without approximations, and the matching to QED radiation is performed preserving the resonance structure of the process. We find that NNLO QCD predictions including QCD and QED shower effects provide a very good approximation in the bulk-region of the phase space, while EW effects become increasingly important in the high-energy tails of kinematic distributions. Our default predictions are in excellent agreement with recent ATLAS data.
引用
收藏
相关论文
共 217 条
[1]  
Morrissey DE(2012)( Phys. Rept. 515 1-undefined
[2]  
Plehn T(2011)) JHEP 07 018-undefined
[3]  
Tait TMP(2021) + 0 Phys. Lett. B 814 076-undefined
[4]  
Campbell JM(2010) 1 JHEP 07 179-undefined
[5]  
Ellis RK(2016) 2 Phys. Lett. B 761 139-undefined
[6]  
Williams C(2017) 1 JHEP 05 537-undefined
[7]  
Denner A(2018)PS Eur. Phys. J. C 78 002-undefined
[8]  
Pelliccioli G(2022) 2 JHEP 06 154-undefined
[9]  
Campanario F(2015)6 JHEP 08 147-undefined
[10]  
Englert C(2020) 8 JHEP 12 108-undefined