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Higgs boson pair production at NNLO with top quark mass effects
We consider QCD radiative corrections to Higgs boson pair production through gluon fusion in proton collisions. We combine the exact next-to-leading order (NLO) contribution, which features two-loop virtual amplitudes with the full dependence on the top quark mass M$_{t}$ , with the next-to-next-to-...
Autores principales: | , , , , , , |
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Lenguaje: | eng |
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2018
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1007/JHEP05(2018)059 http://cds.cern.ch/record/2307580 |
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author | Grazzini, Massimiliano Heinrich, Gudrun Jones, Stephen Kallweit, Stefan Kerner, Matthias Lindert, Jonas M. Mazzitelli, Javier |
author_facet | Grazzini, Massimiliano Heinrich, Gudrun Jones, Stephen Kallweit, Stefan Kerner, Matthias Lindert, Jonas M. Mazzitelli, Javier |
author_sort | Grazzini, Massimiliano |
collection | CERN |
description | We consider QCD radiative corrections to Higgs boson pair production through gluon fusion in proton collisions. We combine the exact next-to-leading order (NLO) contribution, which features two-loop virtual amplitudes with the full dependence on the top quark mass M$_{t}$ , with the next-to-next-to-leading order (NNLO) corrections computed in the large-M$_{t}$ approximation. The latter are improved with different reweighting techniques in order to account for finite-M$_{t}$ effects beyond NLO. Our reference NNLO result is obtained by combining one-loop double-real corrections with full M$_{t}$ dependence with suitably reweighted real-virtual and double-virtual contributions evaluated in the large-M$_{t}$ approximation. We present predictions for inclusive cross sections in pp collisions at $ \sqrt{s} $ = 13, 14, 27 and 100 TeV and we discuss their uncertainties due to missing M$_{t}$ effects. Our approximated NNLO corrections increase the NLO result by an amount ranging from +12% at $ \sqrt{s}=13 $ TeV to +7% at $ \sqrt{s}=100 $ TeV, and the residual uncertainty of the inclusive cross section from missing M$_{t}$ effects is estimated to be at the few percent level. Our calculation is fully differential in the Higgs boson pair and the associated jet activity: we also present predictions for various differential distributions at $ \sqrt{s}=14 $ and 100 TeV, and discuss the size of the missing M$_{t}$ effects, which can be larger, especially in the tails of certain observables. Our results represent the most advanced perturbative prediction available to date for this process. |
id | cern-2307580 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2018 |
record_format | invenio |
spelling | cern-23075802021-11-13T12:15:15Zdoi:10.1007/JHEP05(2018)059http://cds.cern.ch/record/2307580engGrazzini, MassimilianoHeinrich, GudrunJones, StephenKallweit, StefanKerner, MatthiasLindert, Jonas M.Mazzitelli, JavierHiggs boson pair production at NNLO with top quark mass effectshep-phParticle Physics - PhenomenologyWe consider QCD radiative corrections to Higgs boson pair production through gluon fusion in proton collisions. We combine the exact next-to-leading order (NLO) contribution, which features two-loop virtual amplitudes with the full dependence on the top quark mass M$_{t}$ , with the next-to-next-to-leading order (NNLO) corrections computed in the large-M$_{t}$ approximation. The latter are improved with different reweighting techniques in order to account for finite-M$_{t}$ effects beyond NLO. Our reference NNLO result is obtained by combining one-loop double-real corrections with full M$_{t}$ dependence with suitably reweighted real-virtual and double-virtual contributions evaluated in the large-M$_{t}$ approximation. We present predictions for inclusive cross sections in pp collisions at $ \sqrt{s} $ = 13, 14, 27 and 100 TeV and we discuss their uncertainties due to missing M$_{t}$ effects. Our approximated NNLO corrections increase the NLO result by an amount ranging from +12% at $ \sqrt{s}=13 $ TeV to +7% at $ \sqrt{s}=100 $ TeV, and the residual uncertainty of the inclusive cross section from missing M$_{t}$ effects is estimated to be at the few percent level. Our calculation is fully differential in the Higgs boson pair and the associated jet activity: we also present predictions for various differential distributions at $ \sqrt{s}=14 $ and 100 TeV, and discuss the size of the missing M$_{t}$ effects, which can be larger, especially in the tails of certain observables. Our results represent the most advanced perturbative prediction available to date for this process.We consider QCD radiative corrections to Higgs boson pair production through gluon fusion in proton collisions. We combine the exact next-to-leading order (NLO) contribution, which features two-loop virtual amplitudes with the full dependence on the top quark mass $M_t$, with the next-to-next-to-leading order (NNLO) corrections computed in the large-$M_t$ approximation. The latter are improved with different reweighting techniques in order to account for finite-$M_t$ effects beyond NLO. Our reference NNLO result is obtained by combining one-loop double-real corrections with full $M_t$ dependence with suitably reweighted real--virtual and double-virtual contributions evaluated in the large-$M_t$ approximation. We present predictions for inclusive cross sections in $pp$ collisions at $\sqrt{s}$=13, 14, 27 and 100TeV and we discuss their uncertainties due to missing $M_t$ effects. Our approximated NNLO corrections increase the NLO result by an amount ranging from +12% at $\sqrt{s}$=13TeV to +7% at $\sqrt{s}$=100TeV, and the residual uncertainty from missing $M_t$ effects is estimated to be at the few percent level. Our calculation is fully differential in the Higgs boson pair and the associated jet activity: we also present predictions for various differential distributions at $\sqrt{s}$=14 and 100TeV. Our results represent the most advanced perturbative prediction available to date for this process.arXiv:1803.02463CERN-TH-2018-044IPPP/18/15MPP-2018-30ZU-TH 10/18IPPP-18-15ZU-TH-10-18oai:cds.cern.ch:23075802018-03-06 |
spellingShingle | hep-ph Particle Physics - Phenomenology Grazzini, Massimiliano Heinrich, Gudrun Jones, Stephen Kallweit, Stefan Kerner, Matthias Lindert, Jonas M. Mazzitelli, Javier Higgs boson pair production at NNLO with top quark mass effects |
title | Higgs boson pair production at NNLO with top quark mass effects |
title_full | Higgs boson pair production at NNLO with top quark mass effects |
title_fullStr | Higgs boson pair production at NNLO with top quark mass effects |
title_full_unstemmed | Higgs boson pair production at NNLO with top quark mass effects |
title_short | Higgs boson pair production at NNLO with top quark mass effects |
title_sort | higgs boson pair production at nnlo with top quark mass effects |
topic | hep-ph Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1007/JHEP05(2018)059 http://cds.cern.ch/record/2307580 |
work_keys_str_mv | AT grazzinimassimiliano higgsbosonpairproductionatnnlowithtopquarkmasseffects AT heinrichgudrun higgsbosonpairproductionatnnlowithtopquarkmasseffects AT jonesstephen higgsbosonpairproductionatnnlowithtopquarkmasseffects AT kallweitstefan higgsbosonpairproductionatnnlowithtopquarkmasseffects AT kernermatthias higgsbosonpairproductionatnnlowithtopquarkmasseffects AT lindertjonasm higgsbosonpairproductionatnnlowithtopquarkmasseffects AT mazzitellijavier higgsbosonpairproductionatnnlowithtopquarkmasseffects |