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

Abstract We calculate the generalized soft functions at O $$ \mathcal{O} $$ ( α s 2 $$ {\alpha}_s^2 $$ ) 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 d...

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Main Authors: Alessandro Broggio, Sebastian Jaskiewicz, Leonardo Vernazza
Format: Article
Language:English
Published: SpringerOpen 2021-10-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP10(2021)061
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spelling doaj-d89286505fea4f1eb7fef9d4b082f73f2021-10-10T11:52:27ZengSpringerOpenJournal of High Energy Physics1029-84792021-10-0120211013110.1007/JHEP10(2021)061Next-to-leading power two-loop soft functions for the Drell-Yan process at thresholdAlessandro Broggio0Sebastian Jaskiewicz1Leonardo Vernazza2Università degli Studi di Milano-BicoccaInstitute for Particle Physics Phenomenology, Durham UniversityTheoretical Physics Department, CERNAbstract We calculate the generalized soft functions at O $$ \mathcal{O} $$ ( α s 2 $$ {\alpha}_s^2 $$ ) 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 N3LO, finding agreement.https://doi.org/10.1007/JHEP10(2021)061NLO Computations
collection DOAJ
language English
format Article
sources DOAJ
author Alessandro Broggio
Sebastian Jaskiewicz
Leonardo Vernazza
spellingShingle Alessandro Broggio
Sebastian Jaskiewicz
Leonardo Vernazza
Next-to-leading power two-loop soft functions for the Drell-Yan process at threshold
Journal of High Energy Physics
NLO Computations
author_facet Alessandro Broggio
Sebastian Jaskiewicz
Leonardo Vernazza
author_sort Alessandro Broggio
title 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_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_sort next-to-leading power two-loop soft functions for the drell-yan process at threshold
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2021-10-01
description Abstract We calculate the generalized soft functions at O $$ \mathcal{O} $$ ( α s 2 $$ {\alpha}_s^2 $$ ) 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 N3LO, finding agreement.
topic NLO Computations
url https://doi.org/10.1007/JHEP10(2021)061
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AT sebastianjaskiewicz nexttoleadingpowertwoloopsoftfunctionsforthedrellyanprocessatthreshold
AT leonardovernazza nexttoleadingpowertwoloopsoftfunctionsforthedrellyanprocessatthreshold
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