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NLO QCD+EW predictions for $tHj$ and $tZj$ production at the LHC
In this work we calculate the cross sections for the hadroproduction of a single top quark or antiquark in association with a Higgs (tHj) or Z boson (tZj) at NLO QCD+EW accuracy. In the case of tZj production we consider both the case of the Z boson undecayed and the complete final state tℓ$^{+}$ℓ$^...
Autores principales: | , , |
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Lenguaje: | eng |
Publicado: |
2020
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1007/JHEP08(2020)082 http://cds.cern.ch/record/2722578 |
_version_ | 1780965906108645376 |
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author | Pagani, Davide Tsinikos, Ioannis Vryonidou, Eleni |
author_facet | Pagani, Davide Tsinikos, Ioannis Vryonidou, Eleni |
author_sort | Pagani, Davide |
collection | CERN |
description | In this work we calculate the cross sections for the hadroproduction of a single top quark or antiquark in association with a Higgs (tHj) or Z boson (tZj) at NLO QCD+EW accuracy. In the case of tZj production we consider both the case of the Z boson undecayed and the complete final state tℓ$^{+}$ℓ$^{−}$j, including off-shell and non-resonant effects. We perform our calculation in the five-flavour-scheme (5FS), without selecting any specific production channel (s-, t- or tW associated). Moreover, we provide a more realistic estimate of the theory uncertainty by carefully including the differences between the four-flavour-scheme (4FS) and 5FS predictions. The difficulties underlying this procedure in the presence of EW corrections are discussed in detail. We find that NLO EW corrections are in general within the NLO QCD theory uncertainties only if the flavour scheme uncertainty (4FS vs. 5FS) is taken into account. For the case of tℓ$^{+}$ℓ$^{−}$j production we also investigate differences between NLO QCD+EW predictions and NLO QCD predictions matched with a parton shower simulation including multiple photon emissions. |
id | cern-2722578 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2020 |
record_format | invenio |
spelling | cern-27225782022-07-28T07:21:21Zdoi:10.1007/JHEP08(2020)082http://cds.cern.ch/record/2722578engPagani, DavideTsinikos, IoannisVryonidou, EleniNLO QCD+EW predictions for $tHj$ and $tZj$ production at the LHChep-exParticle Physics - Experimenthep-phParticle Physics - PhenomenologyIn this work we calculate the cross sections for the hadroproduction of a single top quark or antiquark in association with a Higgs (tHj) or Z boson (tZj) at NLO QCD+EW accuracy. In the case of tZj production we consider both the case of the Z boson undecayed and the complete final state tℓ$^{+}$ℓ$^{−}$j, including off-shell and non-resonant effects. We perform our calculation in the five-flavour-scheme (5FS), without selecting any specific production channel (s-, t- or tW associated). Moreover, we provide a more realistic estimate of the theory uncertainty by carefully including the differences between the four-flavour-scheme (4FS) and 5FS predictions. The difficulties underlying this procedure in the presence of EW corrections are discussed in detail. We find that NLO EW corrections are in general within the NLO QCD theory uncertainties only if the flavour scheme uncertainty (4FS vs. 5FS) is taken into account. For the case of tℓ$^{+}$ℓ$^{−}$j production we also investigate differences between NLO QCD+EW predictions and NLO QCD predictions matched with a parton shower simulation including multiple photon emissions.In this work we calculate the cross sections for the hadroproduction of a single top quark or antiquark in association with a Higgs ($tHj$) or $Z$ boson ($tZj$) at NLO QCD+EW accuracy. In the case of $tZj$ production we consider both the case of the $Z$ boson undecayed and the complete final state $t \ell^+ \ell^- j$, including off-shell and non-resonant effects. We perform our calculation in the five-flavour-scheme (5FS), without selecting any specific production channel ($s$-, $t$- or $tW$ associated). Moreover, we provide a more realistic estimate of the theory uncertainty by carefully including the differences between the four-flavour-scheme (4FS) and 5FS predictions. The difficulties underlying this procedure in the presence of EW corrections are discussed in detail. We find that NLO EW corrections are in general within the NLO QCD theory uncertainties only if the flavour scheme uncertainty (4FS vs.~5FS) is taken into account. For the case of $t \ell^+ \ell^- j$ production we also investigate differences between NLO QCD+EW predictions and NLO QCD predictions matched with a parton shower simulation including multiple photon emissions.arXiv:2006.10086DESY-20-101LU-TP 20-33CERN-TH-2020-090oai:cds.cern.ch:27225782020-06-17 |
spellingShingle | hep-ex Particle Physics - Experiment hep-ph Particle Physics - Phenomenology Pagani, Davide Tsinikos, Ioannis Vryonidou, Eleni NLO QCD+EW predictions for $tHj$ and $tZj$ production at the LHC |
title | NLO QCD+EW predictions for $tHj$ and $tZj$ production at the LHC |
title_full | NLO QCD+EW predictions for $tHj$ and $tZj$ production at the LHC |
title_fullStr | NLO QCD+EW predictions for $tHj$ and $tZj$ production at the LHC |
title_full_unstemmed | NLO QCD+EW predictions for $tHj$ and $tZj$ production at the LHC |
title_short | NLO QCD+EW predictions for $tHj$ and $tZj$ production at the LHC |
title_sort | nlo qcd+ew predictions for $thj$ and $tzj$ production at the lhc |
topic | hep-ex Particle Physics - Experiment hep-ph Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1007/JHEP08(2020)082 http://cds.cern.ch/record/2722578 |
work_keys_str_mv | AT paganidavide nloqcdewpredictionsforthjandtzjproductionatthelhc AT tsinikosioannis nloqcdewpredictionsforthjandtzjproductionatthelhc AT vryonidoueleni nloqcdewpredictionsforthjandtzjproductionatthelhc |