Cargando…

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...

Descripción completa

Detalles Bibliográficos
Autores principales: Bertone, Valerio, Carrazza, Stefano, Rojo, Juan
Lenguaje:eng
Publicado: 2015
Materias:
Acceso en línea:http://cds.cern.ch/record/2052827
_version_ 1780948190134009856
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