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Higgs boson production at the LHC using the $q_T$ subtraction formalism at N$^3$LO QCD

We consider higher-order QCD corrections to Higgs boson production through gluon-gluon fusion in the large top quark mass limit in hadron collisions. We extend the transverse-momentum (q$_{T}$ ) subtraction method to next-to-next-to-next-to-leading order (N$^{3}$LO) and combine it with the NNLO Higg...

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Autores principales: Cieri, Leandro, Chen, Xuan, Gehrmann, Thomas, Glover, E.W. N., Huss, Alexander
Lenguaje:eng
Publicado: 2018
Materias:
Acceso en línea:https://dx.doi.org/10.1007/JHEP02(2019)096
http://cds.cern.ch/record/2633095
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author Cieri, Leandro
Chen, Xuan
Gehrmann, Thomas
Glover, E.W. N.
Huss, Alexander
author_facet Cieri, Leandro
Chen, Xuan
Gehrmann, Thomas
Glover, E.W. N.
Huss, Alexander
author_sort Cieri, Leandro
collection CERN
description We consider higher-order QCD corrections to Higgs boson production through gluon-gluon fusion in the large top quark mass limit in hadron collisions. We extend the transverse-momentum (q$_{T}$ ) subtraction method to next-to-next-to-next-to-leading order (N$^{3}$LO) and combine it with the NNLO Higgs-plus-jet calculation to numerically compute differential infrared-safe observables at N$^{3}$LO for Higgs boson production in gluon fusion. To cancel the infrared divergences, we exploit the universal behaviour of the associated q$_{T}$ distributions in the small-q$_{T}$ region. We document all the necessary ingredients of the transverse-momentum subtraction method up to N$^{3}$LO. The missing third-order collinear functions, which contribute only at q$_{T}$ = 0, are approximated using a prescription which uses the known result for the total Higgs boson cross section at this order. As a first application of the third-order q$_{T}$ subtraction method, we present the N$^{3}$LO rapidity distribution of the Higgs boson at the LHC.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2018
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spelling cern-26330952022-06-27T02:18:46Zdoi:10.1007/JHEP02(2019)096http://cds.cern.ch/record/2633095engCieri, LeandroChen, XuanGehrmann, ThomasGlover, E.W. N.Huss, AlexanderHiggs boson production at the LHC using the $q_T$ subtraction formalism at N$^3$LO QCDhep-phParticle Physics - PhenomenologyWe consider higher-order QCD corrections to Higgs boson production through gluon-gluon fusion in the large top quark mass limit in hadron collisions. We extend the transverse-momentum (q$_{T}$ ) subtraction method to next-to-next-to-next-to-leading order (N$^{3}$LO) and combine it with the NNLO Higgs-plus-jet calculation to numerically compute differential infrared-safe observables at N$^{3}$LO for Higgs boson production in gluon fusion. To cancel the infrared divergences, we exploit the universal behaviour of the associated q$_{T}$ distributions in the small-q$_{T}$ region. We document all the necessary ingredients of the transverse-momentum subtraction method up to N$^{3}$LO. The missing third-order collinear functions, which contribute only at q$_{T}$ = 0, are approximated using a prescription which uses the known result for the total Higgs boson cross section at this order. As a first application of the third-order q$_{T}$ subtraction method, we present the N$^{3}$LO rapidity distribution of the Higgs boson at the LHC.We consider higher-order QCD corrections to Higgs boson production through gluon-gluon fusion in the large top quark mass limit in hadron collisions. We extend the transverse-momentum ($q_T$) subtraction method to next-to-next-to-next-to-leading order (N$^3$LO) and combine it with the NNLO Higgs-plus-jet calculation to numerically compute differential infrared-safe observables at N$^3$LO for Higgs boson production in gluon fusion. To cancel the infrared divergences, we exploit the universal behaviour of the associated $q_T$ distributions in the small-$q_T$ region. We document all the necessary ingredients of the transverse-momentum subtraction method up to N$^3$LO. The missing third order collinear functions, which contribute only at $q_T$ =0, are approximated using a prescription which uses the known result for the total Higgs boson cross section at this order. As a first application of the third-order $q_T$ subtraction method, we present the N$^3$LO rapidity distribution of the Higgs boson at the LHC.arXiv:1807.11501ZU-TH 27/18IPPP/18/67CERN-TH-2018-167oai:cds.cern.ch:26330952018-07-30
spellingShingle hep-ph
Particle Physics - Phenomenology
Cieri, Leandro
Chen, Xuan
Gehrmann, Thomas
Glover, E.W. N.
Huss, Alexander
Higgs boson production at the LHC using the $q_T$ subtraction formalism at N$^3$LO QCD
title Higgs boson production at the LHC using the $q_T$ subtraction formalism at N$^3$LO QCD
title_full Higgs boson production at the LHC using the $q_T$ subtraction formalism at N$^3$LO QCD
title_fullStr Higgs boson production at the LHC using the $q_T$ subtraction formalism at N$^3$LO QCD
title_full_unstemmed Higgs boson production at the LHC using the $q_T$ subtraction formalism at N$^3$LO QCD
title_short Higgs boson production at the LHC using the $q_T$ subtraction formalism at N$^3$LO QCD
title_sort higgs boson production at the lhc using the $q_t$ subtraction formalism at n$^3$lo qcd
topic hep-ph
Particle Physics - Phenomenology
url https://dx.doi.org/10.1007/JHEP02(2019)096
http://cds.cern.ch/record/2633095
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