Rapidity regulators in the semi-inclusive deep inelastic scattering and Drell-Yan processes
| dc.contributor.author | Fleming, Sean | |
| dc.contributor.author | Labun, Ou Z. | |
| dc.date.accessioned | 2017-07-27T18:31:33Z | |
| dc.date.available | 2017-07-27T18:31:33Z | |
| dc.date.issued | 2017-06-23 | |
| dc.identifier.citation | Rapidity regulators in the semi-inclusive deep inelastic scattering and Drell-Yan processes 2017, 95 (11) Physical Review D | en |
| dc.identifier.issn | 2470-0010 | |
| dc.identifier.issn | 2470-0029 | |
| dc.identifier.doi | 10.1103/PhysRevD.95.114020 | |
| dc.identifier.uri | http://hdl.handle.net/10150/624943 | |
| dc.description.abstract | We 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.sponsorship | Office of Science, Office of Nuclear Physics of the US Department of Energy [DE-FG02-04ER41338] | en |
| dc.language.iso | en | en |
| dc.publisher | AMER PHYSICAL SOC | en |
| dc.relation.url | http://link.aps.org/doi/10.1103/PhysRevD.95.114020 | en |
| dc.rights | © 2017 American Physical Society. | en |
| dc.rights.uri | http://rightsstatements.org/vocab/InC/1.0/ | |
| dc.title | Rapidity regulators in the semi-inclusive deep inelastic scattering and Drell-Yan processes | en |
| dc.type | Article | en |
| dc.contributor.department | Univ Arizona, Dept Phys | en |
| dc.identifier.journal | Physical Review D | en |
| dc.description.collectioninformation | This 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.version | Final published version | en |
| refterms.dateFOA | 2018-06-15T11:01:12Z | |
| html.description.abstract | We 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. |
