Predicting $F_{2}^{D(3)}$ from the dipole cross-section

We employ a parameterisation of the proton dipole cross section previously extracted from electroproduction and photoproduction data to predict the diffractive structure function F2D(3)(Q^2, beta, xpom). Comparison with HERA H1 data yields good agreement.

Detalles Bibliográficos
Autores principales: Forshaw, Jeffrey R., Kerley, G.R., Shaw, Graham
Lenguaje:eng
Publicado: 1999
Materias:
Particle Physics - Phenomenology
Acceso en línea:https://dx.doi.org/10.1016/S0375-9474(00)00218-9
http://cds.cern.ch/record/402716
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author Forshaw, Jeffrey R.
Kerley, G.R.
Shaw, Graham
author_facet Forshaw, Jeffrey R.
Kerley, G.R.
Shaw, Graham
author_sort Forshaw, Jeffrey R.
collection CERN
description We employ a parameterisation of the proton dipole cross section previously extracted from electroproduction and photoproduction data to predict the diffractive structure function F2D(3)(Q^2, beta, xpom). Comparison with HERA H1 data yields good agreement.
id cern-402716
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1999
record_format invenio
spelling cern-4027162023-03-14T18:08:19Zdoi:10.1016/S0375-9474(00)00218-9http://cds.cern.ch/record/402716engForshaw, Jeffrey R.Kerley, G.R.Shaw, GrahamPredicting $F_{2}^{D(3)}$ from the dipole cross-sectionParticle Physics - PhenomenologyWe employ a parameterisation of the proton dipole cross section previously extracted from electroproduction and photoproduction data to predict the diffractive structure function F2D(3)(Q^2, beta, xpom). Comparison with HERA H1 data yields good agreement.We employ a parameterisation of the proton dipole cross section previously extracted from electroproduction and photoproduction data to predict the diffractive structure function F2D(3)(Q^2, beta, xpom). Comparison with HERA H1 data yields good agreement.We employ a parameterisation of the proton dipole cross section previously extracted from electroproduction and photoproduction data to predict the diffractive structure function F 2 D (3) ( Q 2 , β , x P ). Comparison with HERA H1 data yields good agreement.hep-ph/9910251MC-TH-99-14CERN-TH-99-306CERN-TH-99-306MC-TH-99-14oai:cds.cern.ch:4027161999-10-07
spellingShingle Particle Physics - Phenomenology
Forshaw, Jeffrey R.
Kerley, G.R.
Shaw, Graham
Predicting $F_{2}^{D(3)}$ from the dipole cross-section
title Predicting $F_{2}^{D(3)}$ from the dipole cross-section
title_full Predicting $F_{2}^{D(3)}$ from the dipole cross-section
title_fullStr Predicting $F_{2}^{D(3)}$ from the dipole cross-section
title_full_unstemmed Predicting $F_{2}^{D(3)}$ from the dipole cross-section
title_short Predicting $F_{2}^{D(3)}$ from the dipole cross-section
title_sort predicting $f_{2}^{d(3)}$ from the dipole cross-section
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/S0375-9474(00)00218-9
http://cds.cern.ch/record/402716
work_keys_str_mv AT forshawjeffreyr predictingf2d3fromthedipolecrosssection
AT kerleygr predictingf2d3fromthedipolecrosssection
AT shawgraham predictingf2d3fromthedipolecrosssection

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