The polarized three-loop anomalous dimensions from on-shell massive operator matrix elements
We calculate all contributions ∝TF to the polarized three–loop anomalous dimensions in the M–scheme using massive operator matrix elements and compare to results in the literature. This includes the complete anomalous dimensions γqq(2),PS and γqg(2). We also obtain the complete two–loop polarized an...
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doaj-db1e0413074f4451a1ed78cb4193b9662020-11-25T02:09:29ZengElsevierNuclear Physics B0550-32132019-11-01948The polarized three-loop anomalous dimensions from on-shell massive operator matrix elementsA. Behring0J. Blümlein1A. De Freitas2A. Goedicke3S. Klein4A. von Manteuffel5C. Schneider6K. Schönwald7Deutsches Elektronen–Synchrotron, DESY, Platanenallee 6, D-15738 Zeuthen, Germany; Institut für Theoretische Teilchenphysik Campus Süd, Karlsruher Institut für Technologie (KIT), D-76128 Karlsruhe, GermanyDeutsches Elektronen–Synchrotron, DESY, Platanenallee 6, D-15738 Zeuthen, Germany; Corresponding author.Deutsches Elektronen–Synchrotron, DESY, Platanenallee 6, D-15738 Zeuthen, GermanyDeutsches Elektronen–Synchrotron, DESY, Platanenallee 6, D-15738 Zeuthen, Germany; Institut für Theoretische Teilchenphysik Campus Süd, Karlsruher Institut für Technologie (KIT), D-76128 Karlsruhe, Germany; Research Institute for Symbolic Computation (RISC), Johannes Kepler University, Altenbergerstraße 69, A-4040 Linz, AustriaInstitut für Theoretische Teilchenphysik und Kosmologie, RWTH Aachen University, D-52056 Aachen, GermanyDepartment of Physics and Astronomy, Michigan State University, East Lansing, MI 48824, USAResearch Institute for Symbolic Computation (RISC), Johannes Kepler University, Altenbergerstraße 69, A-4040 Linz, AustriaDeutsches Elektronen–Synchrotron, DESY, Platanenallee 6, D-15738 Zeuthen, GermanyWe calculate all contributions ∝TF to the polarized three–loop anomalous dimensions in the M–scheme using massive operator matrix elements and compare to results in the literature. This includes the complete anomalous dimensions γqq(2),PS and γqg(2). We also obtain the complete two–loop polarized anomalous dimensions in an independent calculation. While for most of the anomalous dimensions the usual direct computation methods in Mellin N–space can be applied since all recurrences factorize at first order, this is not the case for γqg(2). Due to the necessity of deeper expansions of the master integrals in the dimensional parameter ε=D−4, we had to use the method of arbitrary high moments to eliminate elliptic contributions in intermediate steps. 4000 moments were generated to determine this anomalous dimension and 2640 moments turned out to be sufficient. As an aside, we also recalculate the contributions ∝TF to the three–loop QCD β–function.http://www.sciencedirect.com/science/article/pii/S0550321319302391 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
A. Behring J. Blümlein A. De Freitas A. Goedicke S. Klein A. von Manteuffel C. Schneider K. Schönwald |
spellingShingle |
A. Behring J. Blümlein A. De Freitas A. Goedicke S. Klein A. von Manteuffel C. Schneider K. Schönwald The polarized three-loop anomalous dimensions from on-shell massive operator matrix elements Nuclear Physics B |
author_facet |
A. Behring J. Blümlein A. De Freitas A. Goedicke S. Klein A. von Manteuffel C. Schneider K. Schönwald |
author_sort |
A. Behring |
title |
The polarized three-loop anomalous dimensions from on-shell massive operator matrix elements |
title_short |
The polarized three-loop anomalous dimensions from on-shell massive operator matrix elements |
title_full |
The polarized three-loop anomalous dimensions from on-shell massive operator matrix elements |
title_fullStr |
The polarized three-loop anomalous dimensions from on-shell massive operator matrix elements |
title_full_unstemmed |
The polarized three-loop anomalous dimensions from on-shell massive operator matrix elements |
title_sort |
polarized three-loop anomalous dimensions from on-shell massive operator matrix elements |
publisher |
Elsevier |
series |
Nuclear Physics B |
issn |
0550-3213 |
publishDate |
2019-11-01 |
description |
We calculate all contributions ∝TF to the polarized three–loop anomalous dimensions in the M–scheme using massive operator matrix elements and compare to results in the literature. This includes the complete anomalous dimensions γqq(2),PS and γqg(2). We also obtain the complete two–loop polarized anomalous dimensions in an independent calculation. While for most of the anomalous dimensions the usual direct computation methods in Mellin N–space can be applied since all recurrences factorize at first order, this is not the case for γqg(2). Due to the necessity of deeper expansions of the master integrals in the dimensional parameter ε=D−4, we had to use the method of arbitrary high moments to eliminate elliptic contributions in intermediate steps. 4000 moments were generated to determine this anomalous dimension and 2640 moments turned out to be sufficient. As an aside, we also recalculate the contributions ∝TF to the three–loop QCD β–function. |
url |
http://www.sciencedirect.com/science/article/pii/S0550321319302391 |
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