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The total top quark pair production cross-section at hadron colliders through $\cal{O} (\alpha_{S}^{4})$

We compute the next-to-next-to-leading order (NNLO) QCD correction to the total cross-section for the reaction gg \to t\bar t + X. Together with the partonic channels we computed previously, the result derived in this letter completes the set of NNLO QCD corrections to the total top pair production...

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Detalles Bibliográficos
Autores principales: Czakon, Michał, Fiedler, Paul, Mitov, Alexander
Lenguaje:eng
Publicado: 2013
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevLett.110.252004
http://cds.cern.ch/record/1532829
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author Czakon, Michał
Fiedler, Paul
Mitov, Alexander
author_facet Czakon, Michał
Fiedler, Paul
Mitov, Alexander
author_sort Czakon, Michał
collection CERN
description We compute the next-to-next-to-leading order (NNLO) QCD correction to the total cross-section for the reaction gg \to t\bar t + X. Together with the partonic channels we computed previously, the result derived in this letter completes the set of NNLO QCD corrections to the total top pair production cross-section at hadron colliders. Supplementing the fixed order results with soft-gluon resummation with next-to-next-to-leading logarithmic accuracy we estimate that the theoretical uncertainty of this observable due to unknown higher order corrections is about 3% at the LHC and 2.2% at the Tevatron. We observe a good agreement between the Standard Model predictions and the available experimental measurements. The very high theoretical precision of this observable allows a new level of scrutiny in parton distribution functions and new physics searches.
id cern-1532829
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2013
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spelling cern-15328292020-06-25T08:16:00Zdoi:10.1103/PhysRevLett.110.252004http://cds.cern.ch/record/1532829engCzakon, MichałFiedler, PaulMitov, AlexanderThe total top quark pair production cross-section at hadron colliders through $\cal{O} (\alpha_{S}^{4})$Particle Physics - PhenomenologyWe compute the next-to-next-to-leading order (NNLO) QCD correction to the total cross-section for the reaction gg \to t\bar t + X. Together with the partonic channels we computed previously, the result derived in this letter completes the set of NNLO QCD corrections to the total top pair production cross-section at hadron colliders. Supplementing the fixed order results with soft-gluon resummation with next-to-next-to-leading logarithmic accuracy we estimate that the theoretical uncertainty of this observable due to unknown higher order corrections is about 3% at the LHC and 2.2% at the Tevatron. We observe a good agreement between the Standard Model predictions and the available experimental measurements. The very high theoretical precision of this observable allows a new level of scrutiny in parton distribution functions and new physics searches.We compute the next-to-next-to-leading order (NNLO) quantum chromodynamics (QCD) correction to the total cross section for the reaction gg→tt¯+X. Together with the partonic channels we computed previously, the result derived in this Letter completes the set of NNLO QCD corrections to the total top pair-production cross section at hadron colliders. Supplementing the fixed order results with soft-gluon resummation with next-to-next-to-leading logarithmic accuracy, we estimate that the theoretical uncertainty of this observable due to unknown higher order corrections is about 3% at the LHC and 2.2% at the Tevatron. We observe a good agreement between the standard model predictions and the available experimental measurements. The very high theoretical precision of this observable allows a new level of scrutiny in parton distribution functions and new physics searches.We compute the next-to-next-to-leading order (NNLO) QCD correction to the total cross-section for the reaction gg \to t\bar t + X. Together with the partonic channels we computed previously, the result derived in this letter completes the set of NNLO QCD corrections to the total top pair production cross-section at hadron colliders. Supplementing the fixed order results with soft-gluon resummation with next-to-next-to-leading logarithmic accuracy we estimate that the theoretical uncertainty of this observable due to unknown higher order corrections is about 3% at the LHC and 2.2% at the Tevatron. We observe a good agreement between the Standard Model predictions and the available experimental measurements. The very high theoretical precision of this observable allows a new level of scrutiny in parton distribution functions and new physics searches.arXiv:1303.6254CERN-PH-TH-2013-056TTK-13-08CERN-PH-TH-2013-056TTK-13-08oai:cds.cern.ch:15328292013-03-26
spellingShingle Particle Physics - Phenomenology
Czakon, Michał
Fiedler, Paul
Mitov, Alexander
The total top quark pair production cross-section at hadron colliders through $\cal{O} (\alpha_{S}^{4})$
title The total top quark pair production cross-section at hadron colliders through $\cal{O} (\alpha_{S}^{4})$
title_full The total top quark pair production cross-section at hadron colliders through $\cal{O} (\alpha_{S}^{4})$
title_fullStr The total top quark pair production cross-section at hadron colliders through $\cal{O} (\alpha_{S}^{4})$
title_full_unstemmed The total top quark pair production cross-section at hadron colliders through $\cal{O} (\alpha_{S}^{4})$
title_short The total top quark pair production cross-section at hadron colliders through $\cal{O} (\alpha_{S}^{4})$
title_sort total top quark pair production cross-section at hadron colliders through $\cal{o} (\alpha_{s}^{4})$
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1103/PhysRevLett.110.252004
http://cds.cern.ch/record/1532829
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