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Bottom quark mass effects in associated $WH$ production with $H \to b\bar{b}$ decay through NNLO QCD

We present a computation of next-to-next-to-leading-order (NNLO) QCD corrections to the production of a Higgs boson in association with a W boson at the LHC followed by the decay of the Higgs boson to a bb¯ pair. At variance with previous NNLO QCD studies of the same process, we treat b quarks as ma...

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Detalles Bibliográficos
Autores principales: Behring, Arnd, Bizoń, Wojciech, Caola, Fabrizio, Melnikov, Kirill, Röntsch, Raoul
Lenguaje:eng
Publicado: 2020
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevD.101.114012
http://cds.cern.ch/record/2713389
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author Behring, Arnd
Bizoń, Wojciech
Caola, Fabrizio
Melnikov, Kirill
Röntsch, Raoul
author_facet Behring, Arnd
Bizoń, Wojciech
Caola, Fabrizio
Melnikov, Kirill
Röntsch, Raoul
author_sort Behring, Arnd
collection CERN
description We present a computation of next-to-next-to-leading-order (NNLO) QCD corrections to the production of a Higgs boson in association with a W boson at the LHC followed by the decay of the Higgs boson to a bb¯ pair. At variance with previous NNLO QCD studies of the same process, we treat b quarks as massive. An important advantage of working with massive b quarks is that it makes the use of flavor jet algorithms unnecessary and allows us to employ conventional jet algorithms to define b jets. We compare NNLO QCD descriptions of the associated WH(bb¯) production with massive and massless b quarks and also contrast them with the results provided by parton showers. We find O(5%) differences in fiducial cross sections computed with massless and massive b quarks. We also observe that much larger differences between massless and massive results, as well as between fixed-order and parton-shower results, can arise in selected kinematic distributions.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2020
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spelling cern-27133892022-02-17T03:12:59Zdoi:10.1103/PhysRevD.101.114012http://cds.cern.ch/record/2713389engBehring, ArndBizoń, WojciechCaola, FabrizioMelnikov, KirillRöntsch, RaoulBottom quark mass effects in associated $WH$ production with $H \to b\bar{b}$ decay through NNLO QCDhep-phParticle Physics - PhenomenologyWe present a computation of next-to-next-to-leading-order (NNLO) QCD corrections to the production of a Higgs boson in association with a W boson at the LHC followed by the decay of the Higgs boson to a bb¯ pair. At variance with previous NNLO QCD studies of the same process, we treat b quarks as massive. An important advantage of working with massive b quarks is that it makes the use of flavor jet algorithms unnecessary and allows us to employ conventional jet algorithms to define b jets. We compare NNLO QCD descriptions of the associated WH(bb¯) production with massive and massless b quarks and also contrast them with the results provided by parton showers. We find O(5%) differences in fiducial cross sections computed with massless and massive b quarks. We also observe that much larger differences between massless and massive results, as well as between fixed-order and parton-shower results, can arise in selected kinematic distributions.We present a computation of NNLO QCD corrections to the production of a Higgs boson in association with a $W$ boson at the LHC followed by the decay of the Higgs boson to a $b\bar{b}$ pair. At variance with previous NNLO QCD studies of the same process, we treat $b$ quarks as massive. An important advantage of working with massive $b$ quarks is that it makes the use of flavor jet algorithms unnecessary and allows us to employ conventional jet algorithms to define $b$ jets. We compare NNLO QCD descriptions of the associated $WH(b\bar{b})$ production with massive and massless $b$ quarks and also contrast them with the results provided by parton showers. We find ${\cal O}(5\%)$ differences in fiducial cross sections computed with massless and massive $b$ quarks. We also observe that much larger differences between massless and massive results, as well as between fixed-order and parton-shower results, can arise in selected kinematic distributions.arXiv:2003.08321TTP20-011P3H-20-009CERN-TH-2020-043oai:cds.cern.ch:27133892020-03-18
spellingShingle hep-ph
Particle Physics - Phenomenology
Behring, Arnd
Bizoń, Wojciech
Caola, Fabrizio
Melnikov, Kirill
Röntsch, Raoul
Bottom quark mass effects in associated $WH$ production with $H \to b\bar{b}$ decay through NNLO QCD
title Bottom quark mass effects in associated $WH$ production with $H \to b\bar{b}$ decay through NNLO QCD
title_full Bottom quark mass effects in associated $WH$ production with $H \to b\bar{b}$ decay through NNLO QCD
title_fullStr Bottom quark mass effects in associated $WH$ production with $H \to b\bar{b}$ decay through NNLO QCD
title_full_unstemmed Bottom quark mass effects in associated $WH$ production with $H \to b\bar{b}$ decay through NNLO QCD
title_short Bottom quark mass effects in associated $WH$ production with $H \to b\bar{b}$ decay through NNLO QCD
title_sort bottom quark mass effects in associated $wh$ production with $h \to b\bar{b}$ decay through nnlo qcd
topic hep-ph
Particle Physics - Phenomenology
url https://dx.doi.org/10.1103/PhysRevD.101.114012
http://cds.cern.ch/record/2713389
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