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The two-loop QCD matrix element for $e^{+}e^{-} \to 3$ jets

We compute the ${\cal O}(\alpha_s^3)$ virtual QCD corrections to the $\gamma^*\to q\bar q g$ matrix element arising from the interference of the two-loop with the tree-level amplitude and from the self-interference of the one-loop amplitude. The calculation is performed by reducing all loop integral...

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Detalles Bibliográficos
Autores principales: Garland, L.W., Gehrmann, T., Glover, E.W.Nigel, Koukoutsakis, A., Remiddi, E.
Lenguaje:eng
Publicado: 2001
Materias:
Acceso en línea:https://dx.doi.org/10.1016/S0550-3213(02)00057-3
http://cds.cern.ch/record/529524
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author Garland, L.W.
Gehrmann, T.
Glover, E.W.Nigel
Koukoutsakis, A.
Remiddi, E.
author_facet Garland, L.W.
Gehrmann, T.
Glover, E.W.Nigel
Koukoutsakis, A.
Remiddi, E.
author_sort Garland, L.W.
collection CERN
description We compute the ${\cal O}(\alpha_s^3)$ virtual QCD corrections to the $\gamma^*\to q\bar q g$ matrix element arising from the interference of the two-loop with the tree-level amplitude and from the self-interference of the one-loop amplitude. The calculation is performed by reducing all loop integrals appearing in the two-loop amplitude to a small set of known master integrals. Infrared and ultraviolet divergences are both regularized using conventional dimensional regularization, and the ultraviolet renormalization is performed in the $\bar{MS}$ scheme. The infrared pole structure of the matrix elements agrees with the prediction made by Catani using an infrared factorization formula. The analytic result for the finite terms of both matrix elements is expressed in terms of one- and two-dimensional harmonic polylogarithms.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2001
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spelling cern-5295242021-07-15T03:30:17Zdoi:10.1016/S0550-3213(02)00057-3http://cds.cern.ch/record/529524engGarland, L.W.Gehrmann, T.Glover, E.W.NigelKoukoutsakis, A.Remiddi, E.The two-loop QCD matrix element for $e^{+}e^{-} \to 3$ jetsParticle Physics - PhenomenologyWe compute the ${\cal O}(\alpha_s^3)$ virtual QCD corrections to the $\gamma^*\to q\bar q g$ matrix element arising from the interference of the two-loop with the tree-level amplitude and from the self-interference of the one-loop amplitude. The calculation is performed by reducing all loop integrals appearing in the two-loop amplitude to a small set of known master integrals. Infrared and ultraviolet divergences are both regularized using conventional dimensional regularization, and the ultraviolet renormalization is performed in the $\bar{MS}$ scheme. The infrared pole structure of the matrix elements agrees with the prediction made by Catani using an infrared factorization formula. The analytic result for the finite terms of both matrix elements is expressed in terms of one- and two-dimensional harmonic polylogarithms.We compute the O (α s 3 ) virtual QCD corrections to the γ ∗ →q q ̄ g matrix element arising from the interference of the two-loop with the tree-level amplitude and from the self-interference of the one-loop amplitude. The calculation is performed by reducing all loop integrals appearing in the two-loop amplitude to a small set of known master integrals. Infrared and ultraviolet divergences are both regularized using conventional dimensional regularization, and the ultraviolet renormalization is performed in the MS scheme. The infrared pole structure of the matrix elements agrees with the prediction made by Catani using an infrared factorization formula. The analytic result for the finite terms of both matrix elements is expressed in terms of one- and two-dimensional harmonic polylogarithms.We compute the ${\cal O}(\alpha_s^3)$ virtual QCD corrections to the $\gamma^*\to q\bar q g$ matrix element arising from the interference of the two-loop with the tree-level amplitude and from the self-interference of the one-loop amplitude. The calculation is performed by reducing all loop integrals appearing in the two-loop amplitude to a small set of known master integrals. Infrared and ultraviolet divergences are both regularized using conventional dimensional regularization, and the ultraviolet renormalization is performed in the $\bar{MS}$ scheme. The infrared pole structure of the matrix elements agrees with the prediction made by Catani using an infrared factorization formula. The analytic result for the finite terms of both matrix elements is expressed in terms of one- and two-dimensional harmonic polylogarithms.hep-ph/0112081IPPP-01-59DCPT-01-118CERN-TH-2001-348CERN-TH-2001-348DCTP-2001-118IPPP-2001-59oai:cds.cern.ch:5295242001-12-05
spellingShingle Particle Physics - Phenomenology
Garland, L.W.
Gehrmann, T.
Glover, E.W.Nigel
Koukoutsakis, A.
Remiddi, E.
The two-loop QCD matrix element for $e^{+}e^{-} \to 3$ jets
title The two-loop QCD matrix element for $e^{+}e^{-} \to 3$ jets
title_full The two-loop QCD matrix element for $e^{+}e^{-} \to 3$ jets
title_fullStr The two-loop QCD matrix element for $e^{+}e^{-} \to 3$ jets
title_full_unstemmed The two-loop QCD matrix element for $e^{+}e^{-} \to 3$ jets
title_short The two-loop QCD matrix element for $e^{+}e^{-} \to 3$ jets
title_sort two-loop qcd matrix element for $e^{+}e^{-} \to 3$ jets
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/S0550-3213(02)00057-3
http://cds.cern.ch/record/529524
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