The two-mass contribution to the three-loop gluonic operator matrix element Agg,Q(3)
We calculate the two-mass QCD contributions to the massive operator matrix element Agg,Q at O(αs3) in analytic form in Mellin N- and z-space, maintaining the complete dependence on the heavy quark mass ratio. These terms are important ingredients for the matching relations of the variable flavor num...
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doaj-424cf8574d3745a1b7c65fa94578394c2020-11-25T02:35:45ZengElsevierNuclear Physics B0550-32132018-07-01932129240The two-mass contribution to the three-loop gluonic operator matrix element Agg,Q(3)J. Ablinger0J. Blümlein1A. De Freitas2A. Goedicke3C. Schneider4K. Schönwald5Research Institute for Symbolic Computation (RISC), Johannes Kepler University, Altenbergerstraße 69, A-4040, Linz, AustriaDeutsches Elektronen-Synchrotron, DESY, Platanenallee 6, D-15738 Zeuthen, Germany; Corresponding author.Deutsches Elektronen-Synchrotron, DESY, Platanenallee 6, D-15738 Zeuthen, GermanyInstitut für Theoretische Teilchenphysik Campus Süd, Karlsruher Institut für Technologie (KIT), D-76128 Karlsruhe, GermanyResearch Institute for Symbolic Computation (RISC), Johannes Kepler University, Altenbergerstraße 69, A-4040, Linz, AustriaDeutsches Elektronen-Synchrotron, DESY, Platanenallee 6, D-15738 Zeuthen, GermanyWe calculate the two-mass QCD contributions to the massive operator matrix element Agg,Q at O(αs3) in analytic form in Mellin N- and z-space, maintaining the complete dependence on the heavy quark mass ratio. These terms are important ingredients for the matching relations of the variable flavor number scheme in the presence of two heavy quark flavors, such as charm and bottom. In Mellin N-space the result is given in the form of nested harmonic, generalized harmonic, cyclotomic and binomial sums, with arguments depending on the mass ratio. The Mellin inversion of these quantities to z-space gives rise to generalized iterated integrals with square root valued letters in the alphabet, depending on the mass ratio as well. Numerical results are presented.http://www.sciencedirect.com/science/article/pii/S0550321318301202 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
J. Ablinger J. Blümlein A. De Freitas A. Goedicke C. Schneider K. Schönwald |
spellingShingle |
J. Ablinger J. Blümlein A. De Freitas A. Goedicke C. Schneider K. Schönwald The two-mass contribution to the three-loop gluonic operator matrix element Agg,Q(3) Nuclear Physics B |
author_facet |
J. Ablinger J. Blümlein A. De Freitas A. Goedicke C. Schneider K. Schönwald |
author_sort |
J. Ablinger |
title |
The two-mass contribution to the three-loop gluonic operator matrix element Agg,Q(3) |
title_short |
The two-mass contribution to the three-loop gluonic operator matrix element Agg,Q(3) |
title_full |
The two-mass contribution to the three-loop gluonic operator matrix element Agg,Q(3) |
title_fullStr |
The two-mass contribution to the three-loop gluonic operator matrix element Agg,Q(3) |
title_full_unstemmed |
The two-mass contribution to the three-loop gluonic operator matrix element Agg,Q(3) |
title_sort |
two-mass contribution to the three-loop gluonic operator matrix element agg,q(3) |
publisher |
Elsevier |
series |
Nuclear Physics B |
issn |
0550-3213 |
publishDate |
2018-07-01 |
description |
We calculate the two-mass QCD contributions to the massive operator matrix element Agg,Q at O(αs3) in analytic form in Mellin N- and z-space, maintaining the complete dependence on the heavy quark mass ratio. These terms are important ingredients for the matching relations of the variable flavor number scheme in the presence of two heavy quark flavors, such as charm and bottom. In Mellin N-space the result is given in the form of nested harmonic, generalized harmonic, cyclotomic and binomial sums, with arguments depending on the mass ratio. The Mellin inversion of these quantities to z-space gives rise to generalized iterated integrals with square root valued letters in the alphabet, depending on the mass ratio as well. Numerical results are presented. |
url |
http://www.sciencedirect.com/science/article/pii/S0550321318301202 |
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