Cargando…

Triple vector boson production through Higgs-Strahlung with NLO multijet merging

Triple gauge boson hadroproduction, in particular the production of three $W$-bosons at the LHC, is considered at next-to leading order accuracy in QCD. The NLO matrix elements are combined with parton showers. Multijet merging is invoked such that NLO matrix elements with one additional jet are als...

Descripción completa

Detalles Bibliográficos
Autores principales: Hoeche, S., Krauss, F., Pozzorini, S., Schoenherr, M., Thompson, J.M., Zapp, K.C.
Lenguaje:eng
Publicado: 2014
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevD.89.093015
http://cds.cern.ch/record/1691162
_version_ 1780935706386890752
author Hoeche, S.
Krauss, F.
Pozzorini, S.
Schoenherr, M.
Thompson, J.M.
Zapp, K.C.
author_facet Hoeche, S.
Krauss, F.
Pozzorini, S.
Schoenherr, M.
Thompson, J.M.
Zapp, K.C.
author_sort Hoeche, S.
collection CERN
description Triple gauge boson hadroproduction, in particular the production of three $W$-bosons at the LHC, is considered at next-to leading order accuracy in QCD. The NLO matrix elements are combined with parton showers. Multijet merging is invoked such that NLO matrix elements with one additional jet are also included. The studies here incorporate both the signal and all relevant backgrounds for $VH$ production with the subsequent decay of the Higgs boson into $W$-- or $\tau$--\-pairs. They have been performed using \SherpaOpenLoops in combination with Collier.
id cern-1691162
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2014
record_format invenio
spelling cern-16911622020-02-14T04:03:42Zdoi:10.1103/PhysRevD.89.093015http://cds.cern.ch/record/1691162engHoeche, S.Krauss, F.Pozzorini, S.Schoenherr, M.Thompson, J.M.Zapp, K.C.Triple vector boson production through Higgs-Strahlung with NLO multijet mergingParticle Physics - PhenomenologyTriple gauge boson hadroproduction, in particular the production of three $W$-bosons at the LHC, is considered at next-to leading order accuracy in QCD. The NLO matrix elements are combined with parton showers. Multijet merging is invoked such that NLO matrix elements with one additional jet are also included. The studies here incorporate both the signal and all relevant backgrounds for $VH$ production with the subsequent decay of the Higgs boson into $W$-- or $\tau$--\-pairs. They have been performed using \SherpaOpenLoops in combination with Collier.Triple gauge boson hadroproduction, in particular the production of three $W$-bosons at the LHC, is considered at next-to leading order accuracy in QCD. The NLO matrix elements are combined with parton showers. Multijet merging is invoked such that NLO matrix elements with one additional jet are also included. The studies here incorporate both the signal and all relevant backgrounds for $VH$ production with the subsequent decay of the Higgs boson into $W$-- or $\tau$--\-pairs. They have been performed using \SherpaOpenLoops in combination with Collier.<p>Triple gauge boson hadroproduction, in particular the production of three <inline-formula><mml:math display="inline"><mml:mi>W</mml:mi></mml:math></inline-formula>-bosons at the LHC, is considered at next-to leading order accuracy in QCD. The NLO matrix elements are combined with parton showers. Multijet merging is invoked such that NLO matrix elements with one additional jet are also included. The studies here incorporate both the signal and all relevant backgrounds for <inline-formula><mml:math display="inline"><mml:mrow><mml:mi>V</mml:mi><mml:mi>H</mml:mi></mml:mrow></mml:math></inline-formula> production with the subsequent decay of the Higgs boson into <inline-formula><mml:math display="inline"><mml:mrow><mml:mi>W</mml:mi></mml:mrow></mml:math></inline-formula>– or <inline-formula><mml:math display="inline"><mml:mrow><mml:mi>τ</mml:mi></mml:mrow></mml:math></inline-formula>–pairs. They have been performed using <sc>Sherpa</sc><inline-formula><mml:math display="inline"><mml:mrow><mml:mo>+</mml:mo></mml:mrow></mml:math></inline-formula><sc>OpenLoops</sc> in combination with <sc>Collier</sc>.</p>DCP-14-46IPPP-14-23MCNET-14-007SLAC-PUB-15933ZU-13-14arXiv:1403.7516CERN-PH-TH-2014-051CERN-PH-TH-2014-051oai:cds.cern.ch:16911622014-03-28
spellingShingle Particle Physics - Phenomenology
Hoeche, S.
Krauss, F.
Pozzorini, S.
Schoenherr, M.
Thompson, J.M.
Zapp, K.C.
Triple vector boson production through Higgs-Strahlung with NLO multijet merging
title Triple vector boson production through Higgs-Strahlung with NLO multijet merging
title_full Triple vector boson production through Higgs-Strahlung with NLO multijet merging
title_fullStr Triple vector boson production through Higgs-Strahlung with NLO multijet merging
title_full_unstemmed Triple vector boson production through Higgs-Strahlung with NLO multijet merging
title_short Triple vector boson production through Higgs-Strahlung with NLO multijet merging
title_sort triple vector boson production through higgs-strahlung with nlo multijet merging
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1103/PhysRevD.89.093015
http://cds.cern.ch/record/1691162
work_keys_str_mv AT hoeches triplevectorbosonproductionthroughhiggsstrahlungwithnlomultijetmerging
AT kraussf triplevectorbosonproductionthroughhiggsstrahlungwithnlomultijetmerging
AT pozzorinis triplevectorbosonproductionthroughhiggsstrahlungwithnlomultijetmerging
AT schoenherrm triplevectorbosonproductionthroughhiggsstrahlungwithnlomultijetmerging
AT thompsonjm triplevectorbosonproductionthroughhiggsstrahlungwithnlomultijetmerging
AT zappkc triplevectorbosonproductionthroughhiggsstrahlungwithnlomultijetmerging