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QCD corrections to W boson plus heavy quark production at the Tevatron
The next-to-leading order QCD corrections to the production of a W-boson in association with a jet containing a heavy quark are presented. The calculation is fully differential in the final state particle momenta and includes the mass of the heavy quark. We study for the case of the Tevatron the sen...
Autores principales: | , , |
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Lenguaje: | eng |
Publicado: |
1995
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/0370-2693(96)00078-0 http://cds.cern.ch/record/292165 |
_version_ | 1780888716922847232 |
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author | Giele, Walter T. Keller, Stephane Laenen, Eric |
author_facet | Giele, Walter T. Keller, Stephane Laenen, Eric |
author_sort | Giele, Walter T. |
collection | CERN |
description | The next-to-leading order QCD corrections to the production of a W-boson in association with a jet containing a heavy quark are presented. The calculation is fully differential in the final state particle momenta and includes the mass of the heavy quark. We study for the case of the Tevatron the sensitivity of the cross section to the strange quark distribution function, the dependence of the cross section on the heavy quark mass, the transverse momentum distribution of the jet containing the heavy quark, and the momentum distribution of the heavy quark in the jet. |
id | cern-292165 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1995 |
record_format | invenio |
spelling | cern-2921652023-01-31T11:08:39Zdoi:10.1016/0370-2693(96)00078-0http://cds.cern.ch/record/292165engGiele, Walter T.Keller, StephaneLaenen, EricQCD corrections to W boson plus heavy quark production at the TevatronParticle Physics - PhenomenologyThe next-to-leading order QCD corrections to the production of a W-boson in association with a jet containing a heavy quark are presented. The calculation is fully differential in the final state particle momenta and includes the mass of the heavy quark. We study for the case of the Tevatron the sensitivity of the cross section to the strange quark distribution function, the dependence of the cross section on the heavy quark mass, the transverse momentum distribution of the jet containing the heavy quark, and the momentum distribution of the heavy quark in the jet.The next-to-leading order QCD corrections to the production of a $W$-boson in association with a jet containing a heavy quark are presented. The calculation is fully differential in the final state particle momenta and includes the mass of the heavy quark. We study for the case of the Tevatron the sensitivity of the cross section to the strange quark distribution function, the dependence of the cross section on the heavy quark mass, the transverse momentum distribution of the jet containing the heavy quark, and the momentum distribution of the heavy quark in the jet.The next-to-leading order QCD corrections to the production of a $W$-boson in association with a jet containing a heavy quark are presented. The calculation is fully differential in the final state particle momenta and includes the mass of the heavy quark. We study for the case of the Tevatron the sensitivity of the cross section to the strange quark distribution function, the dependence of the cross section on the heavy quark mass, the transverse momentum distribution of the jet containing the heavy quark, and the momentum distribution of the heavy quark in the jet.The next-to-leading order QCD corrections to the production of a $W$-boson in association with a jet containing a heavy quark are presented. The calculation is fully differential in the final state particle momenta and includes the mass of the heavy quark. We study for the case of the Tevatron the sensitivity of the cross section to the strange quark distribution function, the dependence of the cross section on the heavy quark mass, the transverse momentum distribution of the jet containing the heavy quark, and the momentum distribution of the heavy quark in the jet.The next-to-leading order QCD corrections to the production of a $W$-boson in association with a jet containing a heavy quark are presented. The calculation is fully differential in the final state particle momenta and includes the mass of the heavy quark. We study for the case of the Tevatron the sensitivity of the cross section to the strange quark distribution function, the dependence of the cross section on the heavy quark mass, the transverse momentum distribution of the jet containing the heavy quark, and the momentum distribution of the heavy quark in the jet.The next-to-leading order QCD correction to the production of a W boson in association with a jet containing a heavy quark are presented. The calculation is fully differential in the final state particle momenta and includes the mass of the heavy quark. We study for the case of the Tevatron the sensitivity of the cross section to the strange quark distribution function, the dependence of the cross section on the heavy quark mass, the transverse momentum distribution of the jet containing the heavy quark, and the momentum distribution of the heavy quark in the jet.hep-ph/9511449CERN-TH-95-282FERMILAB-PUB-95-369-TCERN-TH-95-282FERMILAB-PUB-95-369-Toai:cds.cern.ch:2921651995-11-29 |
spellingShingle | Particle Physics - Phenomenology Giele, Walter T. Keller, Stephane Laenen, Eric QCD corrections to W boson plus heavy quark production at the Tevatron |
title | QCD corrections to W boson plus heavy quark production at the Tevatron |
title_full | QCD corrections to W boson plus heavy quark production at the Tevatron |
title_fullStr | QCD corrections to W boson plus heavy quark production at the Tevatron |
title_full_unstemmed | QCD corrections to W boson plus heavy quark production at the Tevatron |
title_short | QCD corrections to W boson plus heavy quark production at the Tevatron |
title_sort | qcd corrections to w boson plus heavy quark production at the tevatron |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1016/0370-2693(96)00078-0 http://cds.cern.ch/record/292165 |
work_keys_str_mv | AT gielewaltert qcdcorrectionstowbosonplusheavyquarkproductionatthetevatron AT kellerstephane qcdcorrectionstowbosonplusheavyquarkproductionatthetevatron AT laeneneric qcdcorrectionstowbosonplusheavyquarkproductionatthetevatron |