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Parton distribution function for quarks in an s-channel approach
We use an s-channel picture of hard hadronic collisions to investigate the parton distribution function for quarks at small momentum fraction x, which corresponds to very high energy scattering. We study the renormalized quark distribution at one loop in this approach. In the high-energy picture, th...
Autores principales: | , |
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Lenguaje: | eng |
Publicado: |
2007
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Acceso en línea: | https://dx.doi.org/10.1103/PhysRevD.75.074020 http://cds.cern.ch/record/1015541 |
_version_ | 1780911984772907008 |
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author | Hautmann, F. Soper, Davison E. |
author_facet | Hautmann, F. Soper, Davison E. |
author_sort | Hautmann, F. |
collection | CERN |
description | We use an s-channel picture of hard hadronic collisions to investigate the parton distribution function for quarks at small momentum fraction x, which corresponds to very high energy scattering. We study the renormalized quark distribution at one loop in this approach. In the high-energy picture, the quark distribution function is expressed in terms of a Wilson-line correlator that represents the cross section for a color dipole to scatter from the proton. We model this Wilson-line correlator in a saturation model. We relate this representation of the quark distribution function to the corresponding representation of the structure function F_T(x,Q^2) for deeply inelastic scattering. |
id | cern-1015541 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2007 |
record_format | invenio |
spelling | cern-10155412023-03-14T17:19:58Zdoi:10.1103/PhysRevD.75.074020http://cds.cern.ch/record/1015541engHautmann, F.Soper, Davison E.Parton distribution function for quarks in an s-channel approachParticle Physics - PhenomenologyWe use an s-channel picture of hard hadronic collisions to investigate the parton distribution function for quarks at small momentum fraction x, which corresponds to very high energy scattering. We study the renormalized quark distribution at one loop in this approach. In the high-energy picture, the quark distribution function is expressed in terms of a Wilson-line correlator that represents the cross section for a color dipole to scatter from the proton. We model this Wilson-line correlator in a saturation model. We relate this representation of the quark distribution function to the corresponding representation of the structure function F_T(x,Q^2) for deeply inelastic scattering.We use an s-channel picture of hard hadronic collisions to investigate the parton distribution function for quarks at small momentum fraction x, which corresponds to very high energy scattering. We study the renormalized quark distribution at one loop in this approach. In the high-energy picture, the quark distribution function is expressed in terms of a Wilson-line correlator that represents the cross section for a color dipole to scatter from the proton. We model this Wilson-line correlator in a saturation model. We relate this representation of the quark distribution function to the corresponding representation of the structure function F_T(x,Q^2) for deeply inelastic scattering.hep-ph/0702077CERN-PH-TH-2007-014CERN-PH-TH-2007-014oai:cds.cern.ch:10155412007-02-07 |
spellingShingle | Particle Physics - Phenomenology Hautmann, F. Soper, Davison E. Parton distribution function for quarks in an s-channel approach |
title | Parton distribution function for quarks in an s-channel approach |
title_full | Parton distribution function for quarks in an s-channel approach |
title_fullStr | Parton distribution function for quarks in an s-channel approach |
title_full_unstemmed | Parton distribution function for quarks in an s-channel approach |
title_short | Parton distribution function for quarks in an s-channel approach |
title_sort | parton distribution function for quarks in an s-channel approach |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1103/PhysRevD.75.074020 http://cds.cern.ch/record/1015541 |
work_keys_str_mv | AT hautmannf partondistributionfunctionforquarksinanschannelapproach AT soperdavisone partondistributionfunctionforquarksinanschannelapproach |