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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...
Autores principales: | , , |
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Lenguaje: | eng |
Publicado: |
1994
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/0550-3213(94)90398-0 http://cds.cern.ch/record/253246 |
_version_ | 1780885657383600128 |
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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 |
record_format | invenio |
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 |