Non-local slicing approaches for NNLO QCD in MCFM

Abstract We present the implementation of several processes at Next-to-Next-to Leading Order (NNLO) accuracy in QCD in the parton-level Monte Carlo program MCFM. The processes treated are pp → H, W ± , Z, W ± H, ZH, W ± γ, Zγ and γγ and, for the first time in the code, W + W − , W ± Z and ZZ. Decays...

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Main Authors: John M. Campbell, R. Keith Ellis, Satyajit Seth
Format: Article
Language:English
Published: SpringerOpen 2022-06-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP06(2022)002
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author John M. Campbell
R. Keith Ellis
Satyajit Seth
author_facet John M. Campbell
R. Keith Ellis
Satyajit Seth
author_sort John M. Campbell
collection DOAJ
description Abstract We present the implementation of several processes at Next-to-Next-to Leading Order (NNLO) accuracy in QCD in the parton-level Monte Carlo program MCFM. The processes treated are pp → H, W ± , Z, W ± H, ZH, W ± γ, Zγ and γγ and, for the first time in the code, W + W − , W ± Z and ZZ. Decays of the unstable bosons are fully included, resulting in a flexible fully differential Monte Carlo code. The NNLO corrections have been calculated using two non-local slicing approaches, isolating the doubly unresolved region by cutting on the zero-jettiness, T $$ \mathcal{T} $$ 0, or on q T , the transverse momentum of the colour singlet final-state particles. We find that for most, but not all processes the q T slicing method leads to smaller power corrections for equal computational burden.
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spelling doaj.art-c9ccbddc3d3d457c9e7752bcb733b9ad2023-03-22T10:12:53ZengSpringerOpenJournal of High Energy Physics1029-84792022-06-012022613410.1007/JHEP06(2022)002Non-local slicing approaches for NNLO QCD in MCFMJohn M. Campbell0R. Keith Ellis1Satyajit Seth2FermilabInstitute for Particle Physics Phenomenology, Durham UniversityPhysical Research LaboratoryAbstract We present the implementation of several processes at Next-to-Next-to Leading Order (NNLO) accuracy in QCD in the parton-level Monte Carlo program MCFM. The processes treated are pp → H, W ± , Z, W ± H, ZH, W ± γ, Zγ and γγ and, for the first time in the code, W + W − , W ± Z and ZZ. Decays of the unstable bosons are fully included, resulting in a flexible fully differential Monte Carlo code. The NNLO corrections have been calculated using two non-local slicing approaches, isolating the doubly unresolved region by cutting on the zero-jettiness, T $$ \mathcal{T} $$ 0, or on q T , the transverse momentum of the colour singlet final-state particles. We find that for most, but not all processes the q T slicing method leads to smaller power corrections for equal computational burden.https://doi.org/10.1007/JHEP06(2022)002Electroweak Precision PhysicsHigher-Order Perturbative Calculations
spellingShingle John M. Campbell
R. Keith Ellis
Satyajit Seth
Non-local slicing approaches for NNLO QCD in MCFM
Journal of High Energy Physics
Electroweak Precision Physics
Higher-Order Perturbative Calculations
title Non-local slicing approaches for NNLO QCD in MCFM
title_full Non-local slicing approaches for NNLO QCD in MCFM
title_fullStr Non-local slicing approaches for NNLO QCD in MCFM
title_full_unstemmed Non-local slicing approaches for NNLO QCD in MCFM
title_short Non-local slicing approaches for NNLO QCD in MCFM
title_sort non local slicing approaches for nnlo qcd in mcfm
topic Electroweak Precision Physics
Higher-Order Perturbative Calculations
url https://doi.org/10.1007/JHEP06(2022)002
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