t t ¯ b b ¯ $$ t\overline{t}b\overline{b} $$ at the LHC: on the size of corrections and b-jet definitions

Abstract We report on the calculation of the next-to-leading order QCD corrections to the production of a t t ¯ $$ t\overline{t} $$ pair in association with two heavy-flavour jets. We concentrate on the di-lepton t t ¯ $$ t\overline{t} $$ decay channel at the LHC with s $$ \sqrt{s} $$ = 13 TeV. The...

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Main Authors: Giuseppe Bevilacqua, Huan-Yu Bi, Heribertus Bayu Hartanto, Manfred Kraus, Michele Lupattelli, Malgorzata Worek
Format: Article
Language:English
Published: SpringerOpen 2021-08-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP08(2021)008
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author Giuseppe Bevilacqua
Huan-Yu Bi
Heribertus Bayu Hartanto
Manfred Kraus
Michele Lupattelli
Malgorzata Worek
author_facet Giuseppe Bevilacqua
Huan-Yu Bi
Heribertus Bayu Hartanto
Manfred Kraus
Michele Lupattelli
Malgorzata Worek
author_sort Giuseppe Bevilacqua
collection DOAJ
description Abstract We report on the calculation of the next-to-leading order QCD corrections to the production of a t t ¯ $$ t\overline{t} $$ pair in association with two heavy-flavour jets. We concentrate on the di-lepton t t ¯ $$ t\overline{t} $$ decay channel at the LHC with s $$ \sqrt{s} $$ = 13 TeV. The computation is based on pp → e + ν e μ − ν ¯ $$ \overline{\nu} $$ μ b b ¯ b b ¯ $$ b\overline{b}b\overline{b} $$ matrix elements and includes all resonant and non-resonant diagrams, interferences and off-shell effects of the top quark and the W gauge boson. As it is customary for such studies, results are presented in the form of inclusive and differential fiducial cross sections. We extensively investigate the dependence of our results upon variation of renormalisation and factorisation scales and parton distribution functions in the quest for an accurate estimate of the theoretical uncertainties. We additionally study the impact of the contributions induced by the bottom-quark parton density. Results presented here are particularly relevant for measurements of t t ¯ H $$ t\overline{t}H $$ (H → b b ¯ $$ b\overline{b} $$ ) and the determination of the Higgs coupling to the top quark. In addition, they might be used for precise measurements of the top-quark fiducial cross sections and to investigate top-quark decay modelling at the LHC.
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spelling doaj.art-2aed56440e02489b8d9da46fc9e9f3cd2022-12-21T20:40:49ZengSpringerOpenJournal of High Energy Physics1029-84792021-08-012021813710.1007/JHEP08(2021)008t t ¯ b b ¯ $$ t\overline{t}b\overline{b} $$ at the LHC: on the size of corrections and b-jet definitionsGiuseppe Bevilacqua0Huan-Yu Bi1Heribertus Bayu Hartanto2Manfred Kraus3Michele Lupattelli4Malgorzata Worek5MTA-DE Particle Physics Research Group, University of DebrecenInstitute for Theoretical Particle Physics and Cosmology, RWTH Aachen UniversityCavendish Laboratory, University of CambridgePhysics Department, Florida State UniversityInstitute for Theoretical Particle Physics and Cosmology, RWTH Aachen UniversityInstitute for Theoretical Particle Physics and Cosmology, RWTH Aachen UniversityAbstract We report on the calculation of the next-to-leading order QCD corrections to the production of a t t ¯ $$ t\overline{t} $$ pair in association with two heavy-flavour jets. We concentrate on the di-lepton t t ¯ $$ t\overline{t} $$ decay channel at the LHC with s $$ \sqrt{s} $$ = 13 TeV. The computation is based on pp → e + ν e μ − ν ¯ $$ \overline{\nu} $$ μ b b ¯ b b ¯ $$ b\overline{b}b\overline{b} $$ matrix elements and includes all resonant and non-resonant diagrams, interferences and off-shell effects of the top quark and the W gauge boson. As it is customary for such studies, results are presented in the form of inclusive and differential fiducial cross sections. We extensively investigate the dependence of our results upon variation of renormalisation and factorisation scales and parton distribution functions in the quest for an accurate estimate of the theoretical uncertainties. We additionally study the impact of the contributions induced by the bottom-quark parton density. Results presented here are particularly relevant for measurements of t t ¯ H $$ t\overline{t}H $$ (H → b b ¯ $$ b\overline{b} $$ ) and the determination of the Higgs coupling to the top quark. In addition, they might be used for precise measurements of the top-quark fiducial cross sections and to investigate top-quark decay modelling at the LHC.https://doi.org/10.1007/JHEP08(2021)008NLO ComputationsQCD Phenomenology
spellingShingle Giuseppe Bevilacqua
Huan-Yu Bi
Heribertus Bayu Hartanto
Manfred Kraus
Michele Lupattelli
Malgorzata Worek
t t ¯ b b ¯ $$ t\overline{t}b\overline{b} $$ at the LHC: on the size of corrections and b-jet definitions
Journal of High Energy Physics
NLO Computations
QCD Phenomenology
title t t ¯ b b ¯ $$ t\overline{t}b\overline{b} $$ at the LHC: on the size of corrections and b-jet definitions
title_full t t ¯ b b ¯ $$ t\overline{t}b\overline{b} $$ at the LHC: on the size of corrections and b-jet definitions
title_fullStr t t ¯ b b ¯ $$ t\overline{t}b\overline{b} $$ at the LHC: on the size of corrections and b-jet definitions
title_full_unstemmed t t ¯ b b ¯ $$ t\overline{t}b\overline{b} $$ at the LHC: on the size of corrections and b-jet definitions
title_short t t ¯ b b ¯ $$ t\overline{t}b\overline{b} $$ at the LHC: on the size of corrections and b-jet definitions
title_sort t t ¯ b b ¯ t overline t b overline b at the lhc on the size of corrections and b jet definitions
topic NLO Computations
QCD Phenomenology
url https://doi.org/10.1007/JHEP08(2021)008
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