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Higgs Boson Production via Gluon Fusion: Squark Loops at NLO QCD

The loop-induced processes gg -> h,H,A provide the dominant Higgs boson production mechanisms at the Tevatron and LHC in a large range of the minimal supersymmetric extension of the Standard Model. For squark masses below \sim 400 GeV squark loop contributions become important in addition to the...

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Detalles Bibliográficos
Autores principales: Muhlleitner, Margarete, Spira, Michael
Lenguaje:eng
Publicado: 2006
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.nuclphysb.2007.08.011
http://cds.cern.ch/record/1006973
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author Muhlleitner, Margarete
Spira, Michael
author_facet Muhlleitner, Margarete
Spira, Michael
author_sort Muhlleitner, Margarete
collection CERN
description The loop-induced processes gg -> h,H,A provide the dominant Higgs boson production mechanisms at the Tevatron and LHC in a large range of the minimal supersymmetric extension of the Standard Model. For squark masses below \sim 400 GeV squark loop contributions become important in addition to the top and bottom quark loops. The next-to-leading order QCD corrections to the squark contributions of these processes are determined including the full squark and Higgs mass dependences. They turn out to be large and thus important for the Tevatron and LHC experiments. Squark mass effects of the K factors can be of O(20%). In addition we derive the QCD corrections to the squark contributions of the rare photonic Higgs decays h,H -> gamma gamma, which play a role for the Higgs searches at the LHC.
id cern-1006973
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2006
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spelling cern-10069732023-03-14T18:48:52Zdoi:10.1016/j.nuclphysb.2007.08.011http://cds.cern.ch/record/1006973engMuhlleitner, MargareteSpira, MichaelHiggs Boson Production via Gluon Fusion: Squark Loops at NLO QCDParticle Physics - PhenomenologyThe loop-induced processes gg -> h,H,A provide the dominant Higgs boson production mechanisms at the Tevatron and LHC in a large range of the minimal supersymmetric extension of the Standard Model. For squark masses below \sim 400 GeV squark loop contributions become important in addition to the top and bottom quark loops. The next-to-leading order QCD corrections to the squark contributions of these processes are determined including the full squark and Higgs mass dependences. They turn out to be large and thus important for the Tevatron and LHC experiments. Squark mass effects of the K factors can be of O(20%). In addition we derive the QCD corrections to the squark contributions of the rare photonic Higgs decays h,H -> gamma gamma, which play a role for the Higgs searches at the LHC.The loop-induced processes gg -> h,H,A provide the dominant Higgs boson production mechanisms at the Tevatron and LHC in a large range of the minimal supersymmetric extension of the Standard Model. For squark masses below \sim 400 GeV squark loop contributions become important in addition to the top and bottom quark loops. The next-to-leading order QCD corrections to the squark contributions of these processes are determined including the full squark and Higgs mass dependences. They turn out to be large and thus important for the Tevatron and LHC experiments. Squark mass effects of the K factors can be of O(20%). In addition we derive the QCD corrections to the squark contributions of the rare photonic Higgs decays h,H -> gamma gamma, which play a role for the Higgs searches at the LHC.The loop-induced processes g g → h , H , A provide the dominant Higgs boson production mechanisms at the Tevatron and LHC in a large range of the minimal supersymmetric extension of the Standard Model. For squark masses below ∼400 GeV squark loop contributions become important in addition to the top and bottom quark loops. The next-to-leading order QCD corrections to the squark contributions of these processes are determined including the full squark and Higgs mass dependences. They turn out to be large and thus important for the Tevatron and LHC experiments. Squark mass effects of the K factors can be of O ( 20 % ) . In addition we derive the QCD corrections to the squark contributions of the rare photonic Higgs decays h , H → γ γ , which play a role for the Higgs searches at the LHC.hep-ph/0612254PSI-PR-06-15CERN-PH-TH-2006-265LAPTH-1168-06CERN-PH-TH-2006-265LAPTH-1168PSI-PR-06-15oai:cds.cern.ch:10069732006-12-20
spellingShingle Particle Physics - Phenomenology
Muhlleitner, Margarete
Spira, Michael
Higgs Boson Production via Gluon Fusion: Squark Loops at NLO QCD
title Higgs Boson Production via Gluon Fusion: Squark Loops at NLO QCD
title_full Higgs Boson Production via Gluon Fusion: Squark Loops at NLO QCD
title_fullStr Higgs Boson Production via Gluon Fusion: Squark Loops at NLO QCD
title_full_unstemmed Higgs Boson Production via Gluon Fusion: Squark Loops at NLO QCD
title_short Higgs Boson Production via Gluon Fusion: Squark Loops at NLO QCD
title_sort higgs boson production via gluon fusion: squark loops at nlo qcd
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/j.nuclphysb.2007.08.011
http://cds.cern.ch/record/1006973
work_keys_str_mv AT muhlleitnermargarete higgsbosonproductionviagluonfusionsquarkloopsatnloqcd
AT spiramichael higgsbosonproductionviagluonfusionsquarkloopsatnloqcd