The three-loop single mass polarized pure singlet operator matrix element
We calculate the massive polarized three-loop pure singlet operator matrix element AQq(3),PS in the single mass case in the Larin scheme. This operator matrix element contributes to the massive polarized three-loop Wilson coefficient HQq(3),PS in deep-inelastic scattering and constitutes a three-loo...
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doaj-cd765b7c5db24e7d9b71b9244d3cb7652020-11-25T02:36:06ZengElsevierNuclear Physics B0550-32132020-04-01953The three-loop single mass polarized pure singlet operator matrix elementJ. Ablinger0A. Behring1J. Blümlein2A. De Freitas3A. von Manteuffel4C. Schneider5K. Schönwald6Research Institute for Symbolic Computation (RISC), Johannes Kepler University, Altenbergerstraße 69, A–4040, Linz, AustriaInstitut für Theoretische Teilchenphysik, Karlsruher Institut für Technologie (KIT), D-76128 Karlsruhe, GermanyDeutsches Elektronen–Synchrotron, DESY, Platanenallee 6, D-15738 Zeuthen, GermanyDeutsches Elektronen–Synchrotron, DESY, Platanenallee 6, D-15738 Zeuthen, 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, AustriaInstitut für Theoretische Teilchenphysik, Karlsruher Institut für Technologie (KIT), D-76128 Karlsruhe, Germany; Deutsches Elektronen–Synchrotron, DESY, Platanenallee 6, D-15738 Zeuthen, GermanyWe calculate the massive polarized three-loop pure singlet operator matrix element AQq(3),PS in the single mass case in the Larin scheme. This operator matrix element contributes to the massive polarized three-loop Wilson coefficient HQq(3),PS in deep-inelastic scattering and constitutes a three-loop transition matrix element in the variable flavor number scheme. We provide analytic results in Mellin N and in x space and study the behaviour of this operator matrix element in the region of small and large values of the Bjorken variable x.http://www.sciencedirect.com/science/article/pii/S0550321320300316 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
J. Ablinger A. Behring J. Blümlein A. De Freitas A. von Manteuffel C. Schneider K. Schönwald |
spellingShingle |
J. Ablinger A. Behring J. Blümlein A. De Freitas A. von Manteuffel C. Schneider K. Schönwald The three-loop single mass polarized pure singlet operator matrix element Nuclear Physics B |
author_facet |
J. Ablinger A. Behring J. Blümlein A. De Freitas A. von Manteuffel C. Schneider K. Schönwald |
author_sort |
J. Ablinger |
title |
The three-loop single mass polarized pure singlet operator matrix element |
title_short |
The three-loop single mass polarized pure singlet operator matrix element |
title_full |
The three-loop single mass polarized pure singlet operator matrix element |
title_fullStr |
The three-loop single mass polarized pure singlet operator matrix element |
title_full_unstemmed |
The three-loop single mass polarized pure singlet operator matrix element |
title_sort |
three-loop single mass polarized pure singlet operator matrix element |
publisher |
Elsevier |
series |
Nuclear Physics B |
issn |
0550-3213 |
publishDate |
2020-04-01 |
description |
We calculate the massive polarized three-loop pure singlet operator matrix element AQq(3),PS in the single mass case in the Larin scheme. This operator matrix element contributes to the massive polarized three-loop Wilson coefficient HQq(3),PS in deep-inelastic scattering and constitutes a three-loop transition matrix element in the variable flavor number scheme. We provide analytic results in Mellin N and in x space and study the behaviour of this operator matrix element in the region of small and large values of the Bjorken variable x. |
url |
http://www.sciencedirect.com/science/article/pii/S0550321320300316 |
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