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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...
Autores principales: | , |
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Lenguaje: | eng |
Publicado: |
2006
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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 |
record_format | invenio |
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 |