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NNLO QCD corrections to the Higgs-strahlung processes at hadron colliders

We implement, at next-to-next-to-leading order, the QCD corrections to Standard Model Higgs boson production in association with vector bosons at hadron colliders, $q\bar{q} \to HV$ with $V=W,Z$. They consist of the two--loop corrections to the Drell--Yan process for the production of off-shell vect...

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Autores principales: Brein, Oliver, Djouadi, Abdelhak, Harlander, Robert
Lenguaje:eng
Publicado: 2003
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.physletb.2003.10.112
http://cds.cern.ch/record/629117
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author Brein, Oliver
Djouadi, Abdelhak
Harlander, Robert
author_facet Brein, Oliver
Djouadi, Abdelhak
Harlander, Robert
author_sort Brein, Oliver
collection CERN
description We implement, at next-to-next-to-leading order, the QCD corrections to Standard Model Higgs boson production in association with vector bosons at hadron colliders, $q\bar{q} \to HV$ with $V=W,Z$. They consist of the two--loop corrections to the Drell--Yan process for the production of off-shell vector bosons, $q\bar{q} \to V^*$, and in the case of $Z$ final states, of the additional contribution from heavy-quark loop mediated processes, in particular $gg \to HZ$. For the Higgs boson masses relevant at the Tevatron and the LHC, $M_H \lsim 200$--300 GeV, the two-loop corrections are small, increasing the production cross sections by less than 5% and 10%, respectively; the scale dependence is reduced to a level of less than a few per cent. This places these processes among the most theoretically clean Higgs boson production channels at hadron colliders.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2003
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spelling cern-6291172023-09-23T06:08:15Zdoi:10.1016/j.physletb.2003.10.112http://cds.cern.ch/record/629117engBrein, OliverDjouadi, AbdelhakHarlander, RobertNNLO QCD corrections to the Higgs-strahlung processes at hadron collidersParticle Physics - PhenomenologyWe implement, at next-to-next-to-leading order, the QCD corrections to Standard Model Higgs boson production in association with vector bosons at hadron colliders, $q\bar{q} \to HV$ with $V=W,Z$. They consist of the two--loop corrections to the Drell--Yan process for the production of off-shell vector bosons, $q\bar{q} \to V^*$, and in the case of $Z$ final states, of the additional contribution from heavy-quark loop mediated processes, in particular $gg \to HZ$. For the Higgs boson masses relevant at the Tevatron and the LHC, $M_H \lsim 200$--300 GeV, the two-loop corrections are small, increasing the production cross sections by less than 5% and 10%, respectively; the scale dependence is reduced to a level of less than a few per cent. This places these processes among the most theoretically clean Higgs boson production channels at hadron colliders.We implement, at next-to-next-to-leading order, the QCD corrections to Standard Model Higgs boson production in association with vector bosons at hadron colliders, q q ̄ →HV with V = W , Z . They consist of the two-loop corrections to the Drell–Yan process for the production of off-shell vector bosons, q q ̄ →V ∗ , and in the case of Z final states, of the additional contribution from heavy-quark loop mediated processes, in particular gg → HZ . For the Higgs boson masses relevant at the Tevatron and the LHC, M H ≲200–300 GeV, the two-loop corrections are small, increasing the production cross sections by less than 5% and 10%, respectively; the scale dependence is reduced to a level of less than a few per cent. This places these processes among the most theoretically clean Higgs boson production channels at hadron colliders.We implement, at next-to-next-to-leading order, the QCD corrections to Standard Model Higgs boson production in association with vector bosons at hadron colliders, $q\bar{q} \to HV$ with $V=W,Z$. They consist of the two--loop corrections to the Drell--Yan process for the production of off-shell vector bosons, $q\bar{q} \to V^*$, and in the case of $Z$ final states, of the additional contribution from heavy-quark loop mediated processes, in particular $gg \to HZ$. For the Higgs boson masses relevant at the Tevatron and the LHC, $M_H \lsim 200$--300 GeV, the two-loop corrections are small, increasing the production cross sections by less than 5% and 10%, respectively; the scale dependence is reduced to a level of less than a few per cent. This places these processes among the most theoretically clean Higgs boson production channels at hadron colliders.hep-ph/0307206MPP-2003-35CERN-TH-2003-161PM-03-16CERN-TH-2003-161MPP-2003-35PM-2003-16oai:cds.cern.ch:6291172003-07-16
spellingShingle Particle Physics - Phenomenology
Brein, Oliver
Djouadi, Abdelhak
Harlander, Robert
NNLO QCD corrections to the Higgs-strahlung processes at hadron colliders
title NNLO QCD corrections to the Higgs-strahlung processes at hadron colliders
title_full NNLO QCD corrections to the Higgs-strahlung processes at hadron colliders
title_fullStr NNLO QCD corrections to the Higgs-strahlung processes at hadron colliders
title_full_unstemmed NNLO QCD corrections to the Higgs-strahlung processes at hadron colliders
title_short NNLO QCD corrections to the Higgs-strahlung processes at hadron colliders
title_sort nnlo qcd corrections to the higgs-strahlung processes at hadron colliders
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/j.physletb.2003.10.112
http://cds.cern.ch/record/629117
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AT djouadiabdelhak nnloqcdcorrectionstothehiggsstrahlungprocessesathadroncolliders
AT harlanderrobert nnloqcdcorrectionstothehiggsstrahlungprocessesathadroncolliders