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Higgs Radiation off Top Quarks in $e^{+}e^{-}$ Collisions

The strength of the Yukawa coupling of the leptons and quarks with the Higgs boson is uniquely determined by the Higgs mechanism for generating masses in the Standard Model. The top-Higgs coupling can be measured directly in the process e^+e^- --> t tbar H. This process therefore provides a funda...

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Detalles Bibliográficos
Autores principales: Dittmaier, S., Kramer, M., Liao, Y., Spira, M., Zerwas, P.M.
Lenguaje:eng
Publicado: 1998
Materias:
Acceso en línea:https://dx.doi.org/10.1016/S0370-2693(98)01192-7
http://cds.cern.ch/record/363359
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author Dittmaier, S.
Kramer, M.
Liao, Y.
Spira, M.
Zerwas, P.M.
author_facet Dittmaier, S.
Kramer, M.
Liao, Y.
Spira, M.
Zerwas, P.M.
author_sort Dittmaier, S.
collection CERN
description The strength of the Yukawa coupling of the leptons and quarks with the Higgs boson is uniquely determined by the Higgs mechanism for generating masses in the Standard Model. The top-Higgs coupling can be measured directly in the process e^+e^- --> t tbar H. This process therefore provides a fundamental test of the Higgs mechanism. Extending earlier analyses carried out in the Born approximation, we have determined the cross section for this process including QCD corrections, which turn out to be important.
id cern-363359
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1998
record_format invenio
spelling cern-3633592023-03-14T20:37:07Zdoi:10.1016/S0370-2693(98)01192-7http://cds.cern.ch/record/363359engDittmaier, S.Kramer, M.Liao, Y.Spira, M.Zerwas, P.M.Higgs Radiation off Top Quarks in $e^{+}e^{-}$ CollisionsParticle Physics - PhenomenologyThe strength of the Yukawa coupling of the leptons and quarks with the Higgs boson is uniquely determined by the Higgs mechanism for generating masses in the Standard Model. The top-Higgs coupling can be measured directly in the process e^+e^- --> t tbar H. This process therefore provides a fundamental test of the Higgs mechanism. Extending earlier analyses carried out in the Born approximation, we have determined the cross section for this process including QCD corrections, which turn out to be important.The strength of the Yukawa coupling of the leptons and quarks with the Higgs boson is uniquely determined by the Higgs mechanism for generating masses in the Standard Model. The top-Higgs coupling can be measured directly in the process e^+e^- --> t tbar H. This process therefore provides a fundamental test of the Higgs mechanism. Extending earlier analyses carried out in the Born approximation, we have determined the cross section for this process including QCD corrections, which turn out to be important.The strength of the Yukawa coupling of the leptons and quarks with the Higgs boson is uniquely determined by the Higgs mechanism for generating masses in the Standard Model. The top-Higgs coupling can be measured directly in the process e^+e^- --> t tbar H. This process therefore provides a fundamental test of the Higgs mechanism. Extending earlier analyses carried out in the Born approximation, we have determined the cross section for this process including QCD corrections, which turn out to be important.The strength of the Yukawa coupling of the leptons and quarks with the Higgs boson is uniquely determined by the Higgs mechanism for generating masses in the Standard Model. The top-Higgs coupling can be measured directly in the process e^+e^- --> t tbar H. This process therefore provides a fundamental test of the Higgs mechanism. Extending earlier analyses carried out in the Born approximation, we have determined the cross section for this process including QCD corrections, which turn out to be important.The strength of the Yukawa coupling of the leptons and quarks with the Higgs boson is uniquely determined by the Higgs mechanism for generating masses in the Standard Model. The top-Higgs coupling can be measured directly in the process e + e − →t t ̄ H . This process therefore provides a fundamental test of the Higgs mechanism. Extending earlier analyses carried out in the Born approximation, we have determined the cross section for this process including QCD corrections, which turn out to be important.hep-ph/9808433CERN-TH-98-277DESY-98-111RAL-TR-1998-062CERN-TH-98-277RAL-TR-98-062DESY-98-111oai:cds.cern.ch:3633591998-08-28
spellingShingle Particle Physics - Phenomenology
Dittmaier, S.
Kramer, M.
Liao, Y.
Spira, M.
Zerwas, P.M.
Higgs Radiation off Top Quarks in $e^{+}e^{-}$ Collisions
title Higgs Radiation off Top Quarks in $e^{+}e^{-}$ Collisions
title_full Higgs Radiation off Top Quarks in $e^{+}e^{-}$ Collisions
title_fullStr Higgs Radiation off Top Quarks in $e^{+}e^{-}$ Collisions
title_full_unstemmed Higgs Radiation off Top Quarks in $e^{+}e^{-}$ Collisions
title_short Higgs Radiation off Top Quarks in $e^{+}e^{-}$ Collisions
title_sort higgs radiation off top quarks in $e^{+}e^{-}$ collisions
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/S0370-2693(98)01192-7
http://cds.cern.ch/record/363359
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AT kramerm higgsradiationofftopquarksineecollisions
AT liaoy higgsradiationofftopquarksineecollisions
AT spiram higgsradiationofftopquarksineecollisions
AT zerwaspm higgsradiationofftopquarksineecollisions