Two real parton contributions to non-singlet kernels for exclusive QCD DGLAP evolution

Results for the two real parton differential distributions needed for implementing next-to-leading order (NLO) parton shower Monte Carlo are presented. They are also integrated over the phase space in order to provide solid numerical control of the MC codes and for the discussion of the differences...

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Detalles Bibliográficos
Autores principales: Jadach, S, Kusina, A, Skrzypek, M, Slawinska, M
Lenguaje:eng
Publicado: 2011
Materias:
Particle Physics - Phenomenology
Acceso en línea:https://dx.doi.org/10.1007/JHEP08(2011)012
http://cds.cern.ch/record/1332104
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author Jadach, S
Kusina, A
Skrzypek, M
Slawinska, M
author_facet Jadach, S
Kusina, A
Skrzypek, M
Slawinska, M
author_sort Jadach, S
collection CERN
description Results for the two real parton differential distributions needed for implementing next-to-leading order (NLO) parton shower Monte Carlo are presented. They are also integrated over the phase space in order to provide solid numerical control of the MC codes and for the discussion of the differences between the standard $\bar{MS}$ factorization and Monte Carlo implementation at the level of the inclusive NLO evolution kernels. Presented results cover non-singlet class of the diagrams entering into NLO kernels. Classic work of Curci-Furmanski-Pertonzio was used as a guide in the calculations.
id cern-1332104
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2011
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spelling cern-13321042019-09-30T06:29:59Zdoi:10.1007/JHEP08(2011)012http://cds.cern.ch/record/1332104engJadach, SKusina, ASkrzypek, MSlawinska, MTwo real parton contributions to non-singlet kernels for exclusive QCD DGLAP evolutionParticle Physics - PhenomenologyResults for the two real parton differential distributions needed for implementing next-to-leading order (NLO) parton shower Monte Carlo are presented. They are also integrated over the phase space in order to provide solid numerical control of the MC codes and for the discussion of the differences between the standard $\bar{MS}$ factorization and Monte Carlo implementation at the level of the inclusive NLO evolution kernels. Presented results cover non-singlet class of the diagrams entering into NLO kernels. Classic work of Curci-Furmanski-Pertonzio was used as a guide in the calculations.arXiv:1102.5083IFJPAN-IV-2009-6CERN-PH-TH-2011-032oai:cds.cern.ch:13321042011-02-25
spellingShingle Particle Physics - Phenomenology
Jadach, S
Kusina, A
Skrzypek, M
Slawinska, M
Two real parton contributions to non-singlet kernels for exclusive QCD DGLAP evolution
title Two real parton contributions to non-singlet kernels for exclusive QCD DGLAP evolution
title_full Two real parton contributions to non-singlet kernels for exclusive QCD DGLAP evolution
title_fullStr Two real parton contributions to non-singlet kernels for exclusive QCD DGLAP evolution
title_full_unstemmed Two real parton contributions to non-singlet kernels for exclusive QCD DGLAP evolution
title_short Two real parton contributions to non-singlet kernels for exclusive QCD DGLAP evolution
title_sort two real parton contributions to non-singlet kernels for exclusive qcd dglap evolution
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1007/JHEP08(2011)012
http://cds.cern.ch/record/1332104
work_keys_str_mv AT jadachs tworealpartoncontributionstononsingletkernelsforexclusiveqcddglapevolution
AT kusinaa tworealpartoncontributionstononsingletkernelsforexclusiveqcddglapevolution
AT skrzypekm tworealpartoncontributionstononsingletkernelsforexclusiveqcddglapevolution
AT slawinskam tworealpartoncontributionstononsingletkernelsforexclusiveqcddglapevolution

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