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The inverse Mellin transform via analytic continuation

We present a method to calculate the x-space expressions of massless or massive operator matrix elements in QCD and QED containing local composite operator insertions, depending on the discrete Mellin index N, directly, without computing the Mellin-space expressions in explicit form analytically. He...

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Detalles Bibliográficos
Autores principales: Behring, A., Blümlein, J., Schönwald, K.
Lenguaje:eng
Publicado: 2023
Materias:
Acceso en línea:https://dx.doi.org/10.1007/JHEP06(2023)062
http://cds.cern.ch/record/2852232
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author Behring, A.
Blümlein, J.
Schönwald, K.
author_facet Behring, A.
Blümlein, J.
Schönwald, K.
author_sort Behring, A.
collection CERN
description We present a method to calculate the x-space expressions of massless or massive operator matrix elements in QCD and QED containing local composite operator insertions, depending on the discrete Mellin index N, directly, without computing the Mellin-space expressions in explicit form analytically. Here N belongs either to the even or odd positive integers. The method is based on the resummation of the operators into effective propagators and relies on an analytic continuation between two continuous variables. We apply it to iterated integrals as well as to the more general case of iterated non-iterative integrals, generalizing the former ones. The x-space expressions are needed to derive the small-x behaviour of the respective quantities, which usually cannot be accessed in N-space. We illustrate the method for different (iterated) alphabets, including non-iterative $_{2}$F$_{1}$ and elliptic structures, as examples. These structures occur in different massless and massive three-loop calculations. Likewise the method applies even to the analytic closed form solutions of more general cases of differential equations which do not factorize into first-order factors.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2023
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spelling cern-28522322023-08-22T03:47:14Zdoi:10.1007/JHEP06(2023)062http://cds.cern.ch/record/2852232engBehring, A.Blümlein, J.Schönwald, K.The inverse Mellin transform via analytic continuationmath.MPMathematical Physics and Mathematicsmath-phMathematical Physics and Mathematicshep-thParticle Physics - Theoryhep-phParticle Physics - PhenomenologyWe present a method to calculate the x-space expressions of massless or massive operator matrix elements in QCD and QED containing local composite operator insertions, depending on the discrete Mellin index N, directly, without computing the Mellin-space expressions in explicit form analytically. Here N belongs either to the even or odd positive integers. The method is based on the resummation of the operators into effective propagators and relies on an analytic continuation between two continuous variables. We apply it to iterated integrals as well as to the more general case of iterated non-iterative integrals, generalizing the former ones. The x-space expressions are needed to derive the small-x behaviour of the respective quantities, which usually cannot be accessed in N-space. We illustrate the method for different (iterated) alphabets, including non-iterative $_{2}$F$_{1}$ and elliptic structures, as examples. These structures occur in different massless and massive three-loop calculations. Likewise the method applies even to the analytic closed form solutions of more general cases of differential equations which do not factorize into first-order factors.We present a method to calculate the $x$--space expressions of massless or massive operator matrix elements in QCD and QED containing local composite operator insertions, depending on the discrete Mellin index $N$, directly, without computing the Mellin--space expressions in explicit form analytically. Here $N$ belongs either to the even or odd positive integers. The method is based on the resummation of the operators into effective propagators and relies on an analytic continuation between two continuous variables. We apply it to iterated integrals as well as to the more general case of iterated non--iterative integrals, generalizing the former ones. The $x$--space expressions are needed to derive the small--$x$ behaviour of the respective quantities, which usually cannot be accessed in $N$--space. We illustrate the method for different (iterated) alphabets, including non--iterative $_2F_1$ and elliptic structures, as examples. These structures occur in different massless and massive three--loop calculations. Likewise the method applies even to the analytic closed form solutions of more general cases of differential equations which do not factorize into first--order factors.arXiv:2303.05943DESY 20-053DESY 20--053DO-TH 23/01CERN-TH-2023-020ZU-TH 13/23ZU--TH 13/23 13/23oai:cds.cern.ch:28522322023-03-10
spellingShingle math.MP
Mathematical Physics and Mathematics
math-ph
Mathematical Physics and Mathematics
hep-th
Particle Physics - Theory
hep-ph
Particle Physics - Phenomenology
Behring, A.
Blümlein, J.
Schönwald, K.
The inverse Mellin transform via analytic continuation
title The inverse Mellin transform via analytic continuation
title_full The inverse Mellin transform via analytic continuation
title_fullStr The inverse Mellin transform via analytic continuation
title_full_unstemmed The inverse Mellin transform via analytic continuation
title_short The inverse Mellin transform via analytic continuation
title_sort inverse mellin transform via analytic continuation
topic math.MP
Mathematical Physics and Mathematics
math-ph
Mathematical Physics and Mathematics
hep-th
Particle Physics - Theory
hep-ph
Particle Physics - Phenomenology
url https://dx.doi.org/10.1007/JHEP06(2023)062
http://cds.cern.ch/record/2852232
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