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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Online Access: | https://doi.org/10.1007/JHEP10(2021)061 |
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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 |
work_keys_str_mv |
AT alessandrobroggio nexttoleadingpowertwoloopsoftfunctionsforthedrellyanprocessatthreshold AT sebastianjaskiewicz nexttoleadingpowertwoloopsoftfunctionsforthedrellyanprocessatthreshold AT leonardovernazza nexttoleadingpowertwoloopsoftfunctionsforthedrellyanprocessatthreshold |
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1716829469045424128 |