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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...
Autores principales: | , , |
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Lenguaje: | eng |
Publicado: |
2013
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1103/PhysRevLett.110.252004 http://cds.cern.ch/record/1532829 |
_version_ | 1780929645374341120 |
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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 |
record_format | invenio |
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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