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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-...

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Autores principales: Grazzini, Massimiliano, Heinrich, Gudrun, Jones, Stephen, Kallweit, Stefan, Kerner, Matthias, Lindert, Jonas M., Mazzitelli, Javier
Lenguaje:eng
Publicado: 2018
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.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2018
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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
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