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Next-to-leading power two-loop soft functions for the Drell-Yan process at threshold

We calculate the generalized soft functions at $ \mathcal{O} $($ {\alpha}_s^2 $) at next-to-leading power accuracy for the Drell-Yan process at threshold. The operator definitions of these objects contain explicit insertions of soft gauge and matter fields, giving rise to a dependence on additional...

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Detalles Bibliográficos
Autores principales: Broggio, Alessandro, Jaskiewicz, Sebastian, Vernazza, Leonardo
Lenguaje:eng
Publicado: 2021
Materias:
Acceso en línea:https://dx.doi.org/10.1007/JHEP10(2021)061
http://cds.cern.ch/record/2775939
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author Broggio, Alessandro
Jaskiewicz, Sebastian
Vernazza, Leonardo
author_facet Broggio, Alessandro
Jaskiewicz, Sebastian
Vernazza, Leonardo
author_sort Broggio, Alessandro
collection CERN
description We calculate the generalized soft functions at $ \mathcal{O} $($ {\alpha}_s^2 $) at next-to-leading power accuracy for the Drell-Yan process at threshold. The operator definitions of these objects contain explicit insertions of soft gauge and matter fields, giving rise to a dependence on additional convolution variables with respect to the leading power result. These soft functions constitute the last missing ingredient for the validation of the bare factorization theorem to NNLO accuracy. We carry out the calculations by reducing the soft squared amplitudes into a set of canonical master integrals and we employ the method of differential equations to evaluate them. We retain the exact d-dimensional dependence of the convolution variables at the integration boundaries in order to regulate the fixed-order convolution integrals. After combining the soft functions with the relevant collinear functions, we perform checks of the results at the cross-section level against the literature and expansion-by-regions calculations, at NNLO and partly at N$^{3}$LO, finding agreement.
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spelling cern-27759392023-10-04T06:55:09Zdoi:10.1007/JHEP10(2021)061http://cds.cern.ch/record/2775939engBroggio, AlessandroJaskiewicz, SebastianVernazza, LeonardoNext-to-leading power two-loop soft functions for the Drell-Yan process at thresholdhep-phParticle Physics - PhenomenologyWe calculate the generalized soft functions at $ \mathcal{O} $($ {\alpha}_s^2 $) at next-to-leading power accuracy for the Drell-Yan process at threshold. The operator definitions of these objects contain explicit insertions of soft gauge and matter fields, giving rise to a dependence on additional convolution variables with respect to the leading power result. These soft functions constitute the last missing ingredient for the validation of the bare factorization theorem to NNLO accuracy. We carry out the calculations by reducing the soft squared amplitudes into a set of canonical master integrals and we employ the method of differential equations to evaluate them. We retain the exact d-dimensional dependence of the convolution variables at the integration boundaries in order to regulate the fixed-order convolution integrals. After combining the soft functions with the relevant collinear functions, we perform checks of the results at the cross-section level against the literature and expansion-by-regions calculations, at NNLO and partly at N$^{3}$LO, finding agreement.We calculate the generalized soft functions at $\mathcal{O}(\alpha_s^2)$ at next-to-leading power accuracy for the Drell-Yan process at threshold. The operator definitions of these objects contain explicit insertions of soft gauge and matter fields, giving rise to a dependence on additional convolution variables with respect to the leading power result. These soft functions constitute the last missing ingredient for the validation of the bare factorization theorem to NNLO accuracy. We carry out the calculations by reducing the soft squared amplitudes into a set of canonical master integrals and we employ the method of differential equations to evaluate them. We retain the exact $d$-dimensional dependence of the convolution variables at the integration boundaries in order to regulate the fixed-order convolution integrals. After combining our soft functions with the relevant collinear functions, we perform checks of the results at the cross-section level against the literature and expansion-by-regions calculations, at NNLO and partly at N$^3$LO, finding agreement.arXiv:2107.07353IPPP/21/06CERN-TH-2021-108oai:cds.cern.ch:27759392021-07-15
spellingShingle hep-ph
Particle Physics - Phenomenology
Broggio, Alessandro
Jaskiewicz, Sebastian
Vernazza, Leonardo
Next-to-leading power two-loop soft functions for the Drell-Yan process at threshold
title Next-to-leading power two-loop soft functions for the Drell-Yan process at threshold
title_full Next-to-leading power two-loop soft functions for the Drell-Yan process at threshold
title_fullStr Next-to-leading power two-loop soft functions for the Drell-Yan process at threshold
title_full_unstemmed Next-to-leading power two-loop soft functions for the Drell-Yan process at threshold
title_short Next-to-leading power two-loop soft functions for the Drell-Yan process at threshold
title_sort next-to-leading power two-loop soft functions for the drell-yan process at threshold
topic hep-ph
Particle Physics - Phenomenology
url https://dx.doi.org/10.1007/JHEP10(2021)061
http://cds.cern.ch/record/2775939
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AT jaskiewiczsebastian nexttoleadingpowertwoloopsoftfunctionsforthedrellyanprocessatthreshold
AT vernazzaleonardo nexttoleadingpowertwoloopsoftfunctionsforthedrellyanprocessatthreshold