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dc.contributor.authorFleming, Sean
dc.contributor.authorLabun, Ou Z.
dc.date.accessioned2017-07-27T18:31:33Z
dc.date.available2017-07-27T18:31:33Z
dc.date.issued2017-06-23
dc.identifier.citationRapidity regulators in the semi-inclusive deep inelastic scattering and Drell-Yan processes 2017, 95 (11) Physical Review Den
dc.identifier.issn2470-0010
dc.identifier.issn2470-0029
dc.identifier.doi10.1103/PhysRevD.95.114020
dc.identifier.urihttp://hdl.handle.net/10150/624943
dc.description.abstractWe study the semi-inclusive limit of the deep inelastic scattering and Drell-Yan (DY) processes in soft collinear effective theory. In this regime so-called threshold logarithms must be resummed to render perturbation theory well behaved. Part of this resummation occurs via the Dokshitzer, Gribov, Lipatov, Altarelli, Parisi (DGLAP) equation, which at threshold contains a large logarithm that calls into question the convergence of the anomalous dimension. We demonstrate here that the problematic logarithm is related to rapidity divergences, and by introducing a rapidity regulator can be tamed. We show that resumming the rapidity logarithms allows us to reproduce the standard DGLAP running at threshold as long as a set of potentially large nonperturbative logarithms are absorbed into the definition of the parton distribution function (PDF). These terms could, in turn, explain the steep falloff of the PDF in the end point. We then go on to show that the resummation of rapidity divergences does not change the standard threshold resummation in DY, nor do our results depend on the rapidity regulator we choose to use.
dc.description.sponsorshipOffice of Science, Office of Nuclear Physics of the US Department of Energy [DE-FG02-04ER41338]en
dc.language.isoenen
dc.publisherAMER PHYSICAL SOCen
dc.relation.urlhttp://link.aps.org/doi/10.1103/PhysRevD.95.114020en
dc.rights© 2017 American Physical Society.en
dc.rights.urihttp://rightsstatements.org/vocab/InC/1.0/
dc.titleRapidity regulators in the semi-inclusive deep inelastic scattering and Drell-Yan processesen
dc.typeArticleen
dc.contributor.departmentUniv Arizona, Dept Physen
dc.identifier.journalPhysical Review Den
dc.description.collectioninformationThis item from the UA Faculty Publications collection is made available by the University of Arizona with support from the University of Arizona Libraries. If you have questions, please contact us at repository@u.library.arizona.edu.en
dc.eprint.versionFinal published versionen
refterms.dateFOA2018-06-15T11:01:12Z
html.description.abstractWe study the semi-inclusive limit of the deep inelastic scattering and Drell-Yan (DY) processes in soft collinear effective theory. In this regime so-called threshold logarithms must be resummed to render perturbation theory well behaved. Part of this resummation occurs via the Dokshitzer, Gribov, Lipatov, Altarelli, Parisi (DGLAP) equation, which at threshold contains a large logarithm that calls into question the convergence of the anomalous dimension. We demonstrate here that the problematic logarithm is related to rapidity divergences, and by introducing a rapidity regulator can be tamed. We show that resumming the rapidity logarithms allows us to reproduce the standard DGLAP running at threshold as long as a set of potentially large nonperturbative logarithms are absorbed into the definition of the parton distribution function (PDF). These terms could, in turn, explain the steep falloff of the PDF in the end point. We then go on to show that the resummation of rapidity divergences does not change the standard threshold resummation in DY, nor do our results depend on the rapidity regulator we choose to use.


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