Cargando…
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...
Autores principales: | , , , , |
---|---|
Lenguaje: | eng |
Publicado: |
2020
|
Materias: | |
Acceso en línea: | https://dx.doi.org/10.1103/PhysRevD.101.114012 http://cds.cern.ch/record/2713389 |
_version_ | 1780965329319493632 |
---|---|
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. |
id | cern-2713389 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2020 |
record_format | invenio |
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 |
work_keys_str_mv | AT behringarnd bottomquarkmasseffectsinassociatedwhproductionwithhtobbarbdecaythroughnnloqcd AT bizonwojciech bottomquarkmasseffectsinassociatedwhproductionwithhtobbarbdecaythroughnnloqcd AT caolafabrizio bottomquarkmasseffectsinassociatedwhproductionwithhtobbarbdecaythroughnnloqcd AT melnikovkirill bottomquarkmasseffectsinassociatedwhproductionwithhtobbarbdecaythroughnnloqcd AT rontschraoul bottomquarkmasseffectsinassociatedwhproductionwithhtobbarbdecaythroughnnloqcd |