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Doped Parton Distributions
Calculations of high-energy processes involving the production of b-quarks are typically performed in two different ways, the massive four-flavour scheme (4FS) and the massless five-flavour scheme (5FS). For processes where the combination of the 4FS and 5FS results into a matched calculation is tec...
Autores principales: | , , |
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Lenguaje: | eng |
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2015
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Materias: | |
Acceso en línea: | http://cds.cern.ch/record/2052827 |
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author | Bertone, Valerio Carrazza, Stefano Rojo, Juan |
author_facet | Bertone, Valerio Carrazza, Stefano Rojo, Juan |
author_sort | Bertone, Valerio |
collection | CERN |
description | Calculations of high-energy processes involving the production of b-quarks are typically performed in two different ways, the massive four-flavour scheme (4FS) and the massless five-flavour scheme (5FS). For processes where the combination of the 4FS and 5FS results into a matched calculation is technically difficult, it is possible to define a hybrid scheme known as the doped scheme, where above the b-quark threshold the strong coupling runs with $n_f=5$, as in the massless calculation, while the DGLAP splitting functions are those of the $n_f=4$ scheme. In this contribution we present NNPDF3.0 PDF sets in this doped scheme, compare them with the corresponding 4FS and 5FS sets, and discuss their relevance for LHC phenomenology. |
id | cern-2052827 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2015 |
record_format | invenio |
spelling | cern-20528272021-05-03T08:16:22Zhttp://cds.cern.ch/record/2052827engBertone, ValerioCarrazza, StefanoRojo, JuanDoped Parton DistributionsParticle Physics - PhenomenologyCalculations of high-energy processes involving the production of b-quarks are typically performed in two different ways, the massive four-flavour scheme (4FS) and the massless five-flavour scheme (5FS). For processes where the combination of the 4FS and 5FS results into a matched calculation is technically difficult, it is possible to define a hybrid scheme known as the doped scheme, where above the b-quark threshold the strong coupling runs with $n_f=5$, as in the massless calculation, while the DGLAP splitting functions are those of the $n_f=4$ scheme. In this contribution we present NNPDF3.0 PDF sets in this doped scheme, compare them with the corresponding 4FS and 5FS sets, and discuss their relevance for LHC phenomenology.arXiv:1509.04022oai:cds.cern.ch:20528272015-09-14 |
spellingShingle | Particle Physics - Phenomenology Bertone, Valerio Carrazza, Stefano Rojo, Juan Doped Parton Distributions |
title | Doped Parton Distributions |
title_full | Doped Parton Distributions |
title_fullStr | Doped Parton Distributions |
title_full_unstemmed | Doped Parton Distributions |
title_short | Doped Parton Distributions |
title_sort | doped parton distributions |
topic | Particle Physics - Phenomenology |
url | http://cds.cern.ch/record/2052827 |
work_keys_str_mv | AT bertonevalerio dopedpartondistributions AT carrazzastefano dopedpartondistributions AT rojojuan dopedpartondistributions |