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The $p_{T}$ Spectrum in Heavy-Flavour Hadroproduction

We consider the transverse-momentum distribution of heavy flavours in hadronic collisions. We present a formalism in which large transverse-momentum logarithms are resummed at the next-to-leading level, and mass effects are included exactly up to order \alpha_strong^3, so as to retain predictivity a...

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Detalles Bibliográficos
Autores principales: Cacciari, Matteo, Greco, Mario, Nason, Paolo
Lenguaje:eng
Publicado: 1998
Materias:
Acceso en línea:https://dx.doi.org/10.1088/1126-6708/1998/05/007
http://cds.cern.ch/record/349658
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author Cacciari, Matteo
Greco, Mario
Nason, Paolo
author_facet Cacciari, Matteo
Greco, Mario
Nason, Paolo
author_sort Cacciari, Matteo
collection CERN
description We consider the transverse-momentum distribution of heavy flavours in hadronic collisions. We present a formalism in which large transverse-momentum logarithms are resummed at the next-to-leading level, and mass effects are included exactly up to order \alpha_strong^3, so as to retain predictivity at both small and large transverse momenta. As an example, we apply our formalism to b production at the Tevatron.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1998
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spelling cern-3496582023-08-19T02:43:34Zdoi:10.1088/1126-6708/1998/05/007http://cds.cern.ch/record/349658engCacciari, MatteoGreco, MarioNason, PaoloThe $p_{T}$ Spectrum in Heavy-Flavour HadroproductionParticle Physics - PhenomenologyWe consider the transverse-momentum distribution of heavy flavours in hadronic collisions. We present a formalism in which large transverse-momentum logarithms are resummed at the next-to-leading level, and mass effects are included exactly up to order \alpha_strong^3, so as to retain predictivity at both small and large transverse momenta. As an example, we apply our formalism to b production at the Tevatron.We consider the transverse-momentum distribution of heavy flavours in hadronic collisions. We present a formalism in which large transverse-momentum logarithms are resummed at the next-to-leading level, and mass effects are included exactly up to order \alpha_strong^3, so as to retain predictivity at both small and large transverse momenta. As an example, we apply our formalism to b production at the Tevatron.hep-ph/9803400CERN-TH-98-77LPTHE-ORSAY-98-11IFUM-613-FTLNF-98-008-PCERN-TH-98-077IFUM-613-FTLNF-98-008-PLPTHE-98-11oai:cds.cern.ch:3496581998-03-23
spellingShingle Particle Physics - Phenomenology
Cacciari, Matteo
Greco, Mario
Nason, Paolo
The $p_{T}$ Spectrum in Heavy-Flavour Hadroproduction
title The $p_{T}$ Spectrum in Heavy-Flavour Hadroproduction
title_full The $p_{T}$ Spectrum in Heavy-Flavour Hadroproduction
title_fullStr The $p_{T}$ Spectrum in Heavy-Flavour Hadroproduction
title_full_unstemmed The $p_{T}$ Spectrum in Heavy-Flavour Hadroproduction
title_short The $p_{T}$ Spectrum in Heavy-Flavour Hadroproduction
title_sort $p_{t}$ spectrum in heavy-flavour hadroproduction
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1088/1126-6708/1998/05/007
http://cds.cern.ch/record/349658
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