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NLO $W W Z$ production at the LHC
The tri-boson production is one of the key processes for the study of quartic gauge couplings. Next-to-leading order (NLO) corrections are mandatory to reduce theoretical uncertainties. In this study, the most up-to-date predictions including NLO QCD and NLO EW corrections to the total cross section...
Autores principales: | , , |
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Lenguaje: | eng |
Publicado: |
2013
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Materias: | |
Acceso en línea: | http://cds.cern.ch/record/1616493 |
_version_ | 1780932672717062144 |
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author | Nhung, Dao Thi Ninh, Le Duc Weber, Marcus M |
author_facet | Nhung, Dao Thi Ninh, Le Duc Weber, Marcus M |
author_sort | Nhung, Dao Thi |
collection | CERN |
description | The tri-boson production is one of the key processes for the study of quartic gauge couplings. Next-to-leading order (NLO) corrections are mandatory to reduce theoretical uncertainties. In this study, the most up-to-date predictions including NLO QCD and NLO EW corrections to the total cross section and distributions of the WWZ production at the LHC are presented. We show that the QCD correction is about 100% and the EW correction is of a few percent at the total cross section level. The EW correction however becomes significant in the high energy regime of the gauge boson transverse momentum distributions. |
id | cern-1616493 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2013 |
record_format | invenio |
spelling | cern-16164932019-09-30T06:29:59Zhttp://cds.cern.ch/record/1616493engNhung, Dao ThiNinh, Le DucWeber, Marcus MNLO $W W Z$ production at the LHCParticle Physics - PhenomenologyParticle Physics - ExperimentThe tri-boson production is one of the key processes for the study of quartic gauge couplings. Next-to-leading order (NLO) corrections are mandatory to reduce theoretical uncertainties. In this study, the most up-to-date predictions including NLO QCD and NLO EW corrections to the total cross section and distributions of the WWZ production at the LHC are presented. We show that the QCD correction is about 100% and the EW correction is of a few percent at the total cross section level. The EW correction however becomes significant in the high energy regime of the gauge boson transverse momentum distributions.arXiv:1310.6159KA-TP-34-2013SFB-CPP-13-79oai:cds.cern.ch:16164932013-10-23 |
spellingShingle | Particle Physics - Phenomenology Particle Physics - Experiment Nhung, Dao Thi Ninh, Le Duc Weber, Marcus M NLO $W W Z$ production at the LHC |
title | NLO $W W Z$ production at the LHC |
title_full | NLO $W W Z$ production at the LHC |
title_fullStr | NLO $W W Z$ production at the LHC |
title_full_unstemmed | NLO $W W Z$ production at the LHC |
title_short | NLO $W W Z$ production at the LHC |
title_sort | nlo $w w z$ production at the lhc |
topic | Particle Physics - Phenomenology Particle Physics - Experiment |
url | http://cds.cern.ch/record/1616493 |
work_keys_str_mv | AT nhungdaothi nlowwzproductionatthelhc AT ninhleduc nlowwzproductionatthelhc AT webermarcusm nlowwzproductionatthelhc |