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Dimensionally regulated pentagon integrals

We present methods for evaluating the Feynman parameter integrals associated with the pentagon diagram in 4-2 epsilon dimensions, along with explicit results for the integrals with all masses vanishing or with one non-vanishing external mass. The scalar pentagon integral can be expressed as a linear...

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Autores principales: Bern, Zvi, Dixon, Lance J., Kosower, David A.
Lenguaje:eng
Publicado: 1994
Materias:
Acceso en línea:https://dx.doi.org/10.1016/0550-3213(94)90398-0
http://cds.cern.ch/record/253246
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author Bern, Zvi
Dixon, Lance J.
Kosower, David A.
author_facet Bern, Zvi
Dixon, Lance J.
Kosower, David A.
author_sort Bern, Zvi
collection CERN
description We present methods for evaluating the Feynman parameter integrals associated with the pentagon diagram in 4-2 epsilon dimensions, along with explicit results for the integrals with all masses vanishing or with one non-vanishing external mass. The scalar pentagon integral can be expressed as a linear combination of box integrals, up to O(epsilon) corrections, a result which is the dimensionally-regulated version of a D=4 result of Melrose, and of van Neerven and Vermaseren. We obtain and solve differential equations for various dimensionally-regulated box integrals with massless internal lines, which appear in one-loop n-point calculations in QCD. We give a procedure for constructing the tensor pentagon integrals needed in gauge theory, again through O(epsilon^0).
id cern-253246
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1994
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spelling cern-2532462023-10-04T07:57:01Zdoi:10.1016/0550-3213(94)90398-0http://cds.cern.ch/record/253246engBern, ZviDixon, Lance J.Kosower, David A.Dimensionally regulated pentagon integralsParticle Physics - TheoryWe present methods for evaluating the Feynman parameter integrals associated with the pentagon diagram in 4-2 epsilon dimensions, along with explicit results for the integrals with all masses vanishing or with one non-vanishing external mass. The scalar pentagon integral can be expressed as a linear combination of box integrals, up to O(epsilon) corrections, a result which is the dimensionally-regulated version of a D=4 result of Melrose, and of van Neerven and Vermaseren. We obtain and solve differential equations for various dimensionally-regulated box integrals with massless internal lines, which appear in one-loop n-point calculations in QCD. We give a procedure for constructing the tensor pentagon integrals needed in gauge theory, again through O(epsilon^0).We present methods for evaluating the Feynman parameter integrals associated with the pentagon diagram in 4-2 epsilon dimensions, along with explicit results for the integrals with all masses vanishing or with one non-vanishing external mass. The scalar pentagon integral can be expressed as a linear combination of box integrals, up to O(epsilon) corrections, a result which is the dimensionally-regulated version of a D=4 result of Melrose, and of van Neerven and Vermaseren. We obtain and solve differential equations for various dimensionally-regulated box integrals with massless internal lines, which appear in one-loop n-point calculations in QCD. We give a procedure for constructing the tensor pentagon integrals needed in gauge theory, again through O(epsilon^0).We present methods for evaluating the Feynman parameter integrals associated with the pentagon diagram in 4-2 epsilon dimensions, along with explicit results for the integrals with all masses vanishing or with one non-vanishing external mass. The scalar pentagon integral can be expressed as a linear combination of box integrals, up to O(epsilon) corrections, a result which is the dimensionally-regulated version of a D=4 result of Melrose, and of van Neerven and Vermaseren. We obtain and solve differential equations for various dimensionally-regulated box integrals with massless internal lines, which appear in one-loop n-point calculations in QCD. We give a procedure for constructing the tensor pentagon integrals needed in gauge theory, again through O(epsilon^0).We present methods for evaluating the Feynman parameter integrals associated with the pentagon diagram in 4-2∈ dimensions, along with explicit results for the integrals with all masses vanishing or with one non-vanishing external mass. The scalar pentagon integral can be expressed as a linear combination of box integrals, up to O(∈) corrections, a result which is the dimensionally-regulated version of a D = 4 result of Melrose, and of van Neerven and Vermaseren. We obtain and solve differential equations for various dimensionally-regulated box integrals with massless internal lines, which appear in one-loop n -point calculations in QCD. We give a procedure for constructing the tensor pentagon integrals needed in gauge theory, again through O(∈ 0 ).hep-ph/9306240SLAC-PUB-5947SACLAY-SPH-T-92-048UCLA-92-043SACLAY-SPHT-T-92-048UCLA-92-TEP-43SLAC-PUB-5947oai:cds.cern.ch:2532461994
spellingShingle Particle Physics - Theory
Bern, Zvi
Dixon, Lance J.
Kosower, David A.
Dimensionally regulated pentagon integrals
title Dimensionally regulated pentagon integrals
title_full Dimensionally regulated pentagon integrals
title_fullStr Dimensionally regulated pentagon integrals
title_full_unstemmed Dimensionally regulated pentagon integrals
title_short Dimensionally regulated pentagon integrals
title_sort dimensionally regulated pentagon integrals
topic Particle Physics - Theory
url https://dx.doi.org/10.1016/0550-3213(94)90398-0
http://cds.cern.ch/record/253246
work_keys_str_mv AT bernzvi dimensionallyregulatedpentagonintegrals
AT dixonlancej dimensionallyregulatedpentagonintegrals
AT kosowerdavida dimensionallyregulatedpentagonintegrals