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$\text{Tr}(F^3)$ supersymmetric form factors and maximal transcendentality Part II: $0<\mathcal{N}<4$ super Yang-Mills

The study of form factors has many phenomenologically interesting applications, one of which is Higgs plus gluon amplitudes in QCD. Through effective field theory techniques these are related to form factors of various operators of increasing classical dimension. In this paper we extend our analysis...

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Autores principales: Brandhuber, Andreas, Kostacinska, Martyna, Penante, Brenda, Travaglini, Gabriele
Lenguaje:eng
Publicado: 2018
Materias:
Acceso en línea:https://dx.doi.org/10.1007/JHEP12(2018)077
http://cds.cern.ch/record/2313955
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author Brandhuber, Andreas
Kostacinska, Martyna
Penante, Brenda
Travaglini, Gabriele
author_facet Brandhuber, Andreas
Kostacinska, Martyna
Penante, Brenda
Travaglini, Gabriele
author_sort Brandhuber, Andreas
collection CERN
description The study of form factors has many phenomenologically interesting applications, one of which is Higgs plus gluon amplitudes in QCD. Through effective field theory techniques these are related to form factors of various operators of increasing classical dimension. In this paper we extend our analysis of the first finite top-mass correction, arising from the operator Tr(F$^{3}$), from $ \mathcal{N} $ = 4 super Yang-Mills to theories with $ \mathcal{N} $ < 4, for the case of three gluons and up to two loops. We confirm our earlier result that the maximally transcendental part of the associated Catani remainder is universal and equal to that of the form factor of a protected trilinear operator in the maximally supersymmetric theory. The terms with lower transcendentality deviate from the $ \mathcal{N} $ = 4 answer by a surprisingly small set of terms involving for example ζ$_{2}$, ζ$_{3}$ and simple powers of logarithms, for which we provide explicit expressions.
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spelling cern-23139552023-03-14T18:37:17Zdoi:10.1007/JHEP12(2018)077http://cds.cern.ch/record/2313955engBrandhuber, AndreasKostacinska, MartynaPenante, BrendaTravaglini, Gabriele$\text{Tr}(F^3)$ supersymmetric form factors and maximal transcendentality Part II: $0<\mathcal{N}<4$ super Yang-Millshep-thParticle Physics - TheoryThe study of form factors has many phenomenologically interesting applications, one of which is Higgs plus gluon amplitudes in QCD. Through effective field theory techniques these are related to form factors of various operators of increasing classical dimension. In this paper we extend our analysis of the first finite top-mass correction, arising from the operator Tr(F$^{3}$), from $ \mathcal{N} $ = 4 super Yang-Mills to theories with $ \mathcal{N} $ < 4, for the case of three gluons and up to two loops. We confirm our earlier result that the maximally transcendental part of the associated Catani remainder is universal and equal to that of the form factor of a protected trilinear operator in the maximally supersymmetric theory. The terms with lower transcendentality deviate from the $ \mathcal{N} $ = 4 answer by a surprisingly small set of terms involving for example ζ$_{2}$, ζ$_{3}$ and simple powers of logarithms, for which we provide explicit expressions.The study of form factors has many phenomenologically interesting applications, one of which is Higgs plus gluon amplitudes in QCD. Through effective field theory techniques these are related to form factors of various operators of increasing classical dimension. In this paper we extend our analysis of the first finite top-mass correction, arising from the operator ${\rm Tr} (F^3)$, from $\mathcal{N}=4$ super Yang-Mills to theories with $\mathcal{N}<4$, for the case of three gluons and up to two loops. We confirm our earlier result that the maximally transcendental part of the associated Catani remainder is universal and equal to that of the form factor of a protected trilinear operator in the maximally supersymmetric theory. The terms with lower transcendentality deviate from the $\mathcal{N}=4$ answer by a surprisingly small set of terms involving for example $\zeta_2$, $\zeta_3$ and simple powers of logarithms, for which we provide explicit expressions.arXiv:1804.05828QMUL-PH-18-05CERN-TH-2018-064oai:cds.cern.ch:23139552018-04-16
spellingShingle hep-th
Particle Physics - Theory
Brandhuber, Andreas
Kostacinska, Martyna
Penante, Brenda
Travaglini, Gabriele
$\text{Tr}(F^3)$ supersymmetric form factors and maximal transcendentality Part II: $0<\mathcal{N}<4$ super Yang-Mills
title $\text{Tr}(F^3)$ supersymmetric form factors and maximal transcendentality Part II: $0<\mathcal{N}<4$ super Yang-Mills
title_full $\text{Tr}(F^3)$ supersymmetric form factors and maximal transcendentality Part II: $0<\mathcal{N}<4$ super Yang-Mills
title_fullStr $\text{Tr}(F^3)$ supersymmetric form factors and maximal transcendentality Part II: $0<\mathcal{N}<4$ super Yang-Mills
title_full_unstemmed $\text{Tr}(F^3)$ supersymmetric form factors and maximal transcendentality Part II: $0<\mathcal{N}<4$ super Yang-Mills
title_short $\text{Tr}(F^3)$ supersymmetric form factors and maximal transcendentality Part II: $0<\mathcal{N}<4$ super Yang-Mills
title_sort $\text{tr}(f^3)$ supersymmetric form factors and maximal transcendentality part ii: $0<\mathcal{n}<4$ super yang-mills
topic hep-th
Particle Physics - Theory
url https://dx.doi.org/10.1007/JHEP12(2018)077
http://cds.cern.ch/record/2313955
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