Diagrammatic resummation of leading-logarithmic threshold effects at next-to-leading power

Abstract Perturbative cross-sections in QCD are beset by logarithms of kinematic invariants, whose arguments vanish when heavy particles are produced near threshold. Contributions of this type often need to be summed to all orders in the coupling, in order to improve the behaviour of the perturbativ...

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Main Authors: N. Bahjat-Abbas, D. Bonocore, J. Sinninghe Damsté, E. Laenen, L. Magnea, L. Vernazza, C. D. White
Format: Article
Language:English
Published: SpringerOpen 2019-11-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP11(2019)002
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spelling doaj-309094fee974494db164a140fad205dc2020-11-25T04:09:59ZengSpringerOpenJournal of High Energy Physics1029-84792019-11-0120191114610.1007/JHEP11(2019)002Diagrammatic resummation of leading-logarithmic threshold effects at next-to-leading powerN. Bahjat-Abbas0D. Bonocore1J. Sinninghe Damsté2E. Laenen3L. Magnea4L. Vernazza5C. D. White6Centre for Research in String Theory, School of Physics and Astronomy, Queen Mary University of LondonInstitut für Theoretische Physik, Westfälische Wilhelms-Universität MünsterITFA, University of AmsterdamITFA, University of AmsterdamDipartimento di Fisica Teorica and Arnold-Regge Center, Università di Torino, and INFN, Sezione di TorinoNikhefCentre for Research in String Theory, School of Physics and Astronomy, Queen Mary University of LondonAbstract Perturbative cross-sections in QCD are beset by logarithms of kinematic invariants, whose arguments vanish when heavy particles are produced near threshold. Contributions of this type often need to be summed to all orders in the coupling, in order to improve the behaviour of the perturbative expansion, and it has long been known how to do this at leading power in the threshold variable, using a variety of approaches. Recently, the problem of extending this resummation to logarithms suppressed by a single power of the threshold variable has received considerable attention. In this paper, we show that such next-to-leading power (NLP) contributions can indeed be resummed, to leading logarithmic (LL) accuracy, for any QCD process with a colour-singlet final state, using a direct generalisation of the diagrammatic methods available at leading power. We compare our results with other approaches, and comment on the implications for further generalisations beyond leading-logarithmic accuracy.http://link.springer.com/article/10.1007/JHEP11(2019)002QCD Phenomenology
collection DOAJ
language English
format Article
sources DOAJ
author N. Bahjat-Abbas
D. Bonocore
J. Sinninghe Damsté
E. Laenen
L. Magnea
L. Vernazza
C. D. White
spellingShingle N. Bahjat-Abbas
D. Bonocore
J. Sinninghe Damsté
E. Laenen
L. Magnea
L. Vernazza
C. D. White
Diagrammatic resummation of leading-logarithmic threshold effects at next-to-leading power
Journal of High Energy Physics
QCD Phenomenology
author_facet N. Bahjat-Abbas
D. Bonocore
J. Sinninghe Damsté
E. Laenen
L. Magnea
L. Vernazza
C. D. White
author_sort N. Bahjat-Abbas
title Diagrammatic resummation of leading-logarithmic threshold effects at next-to-leading power
title_short Diagrammatic resummation of leading-logarithmic threshold effects at next-to-leading power
title_full Diagrammatic resummation of leading-logarithmic threshold effects at next-to-leading power
title_fullStr Diagrammatic resummation of leading-logarithmic threshold effects at next-to-leading power
title_full_unstemmed Diagrammatic resummation of leading-logarithmic threshold effects at next-to-leading power
title_sort diagrammatic resummation of leading-logarithmic threshold effects at next-to-leading power
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2019-11-01
description Abstract Perturbative cross-sections in QCD are beset by logarithms of kinematic invariants, whose arguments vanish when heavy particles are produced near threshold. Contributions of this type often need to be summed to all orders in the coupling, in order to improve the behaviour of the perturbative expansion, and it has long been known how to do this at leading power in the threshold variable, using a variety of approaches. Recently, the problem of extending this resummation to logarithms suppressed by a single power of the threshold variable has received considerable attention. In this paper, we show that such next-to-leading power (NLP) contributions can indeed be resummed, to leading logarithmic (LL) accuracy, for any QCD process with a colour-singlet final state, using a direct generalisation of the diagrammatic methods available at leading power. We compare our results with other approaches, and comment on the implications for further generalisations beyond leading-logarithmic accuracy.
topic QCD Phenomenology
url http://link.springer.com/article/10.1007/JHEP11(2019)002
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