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Dipole model at Next-to-Leading Order meets HERA data

<!--HTML-->Deep inelastic scattering (DIS) total cross section data at small-x as measured by the HERA experiments is well described by Balitsky-Kovchegov (BK) evolution in the leading order dipole picture [1-3]. Recently the full Next-to-Leading Order (NLO) dipole picture total cross sections...

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Autor principal: Hänninen, Henri
Lenguaje:eng
Publicado: 2020
Materias:
Acceso en línea:http://cds.cern.ch/record/2721395
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author Hänninen, Henri
author_facet Hänninen, Henri
author_sort Hänninen, Henri
collection CERN
description <!--HTML-->Deep inelastic scattering (DIS) total cross section data at small-x as measured by the HERA experiments is well described by Balitsky-Kovchegov (BK) evolution in the leading order dipole picture [1-3]. Recently the full Next-to-Leading Order (NLO) dipole picture total cross sections have become available for DIS [4-6], and a working factorization scheme has been deviced which substracts the soft gluon divergence present at NLO [7]. We report our ongoing work in which we make the first comparisons of the NLO DIS total cross sections to HERA data. The non-perturbative initial condition to BK evolution is fixed by fitting the HERA reduced cross section data. As the NLO results for the DIS total cross section are currently available only in the massless quark limit, we also fit a light quark only cross section constructed with a parametrization of published total and heavy quark data. We find an excellent description of the HERA data. Since the full NLO BK equation is computationally expensive [8], we use a number of beyond LO prescriptions for the evolution that include most important higher order corrections enhanced by large transverse logarithms, including the recent version of the equation formulated in terms of the target rapidity [9]. [1] T. Lappi, H. Mäntysaari, Phys.Rev. D88 (2013) 114020 [2] E. Iancu, J.D. Madrigal, A.H. Mueller, G. Soyez, D.N. Triantafyllopoulos, Phys.Lett. B750 (2015) 643-652 [3] B. Ducloué, E. Iancu, G. Soyez, D.N. Triantafyllopoulos, arXiv:1912.09196 [hep-ph] [4] G. Beuf, Phys.Rev. D94 (2016) no.5, 054016 [5] G. Beuf, Phys.Rev. D96 (2017) no.7, 074033 [6] H. Hänninen, T. Lappi, R. Paatelainen, arXiv:1711.08207 [hep-ph] [7] B. Ducloué, H. Hänninen, T. Lappi, Y. Zhu, Phys.Rev. D96 (2017) no.9, 094017 [8] T. Lappi, H. Mäntysaari, Phys.Rev. D91 (2015) no.7, 074016 [9] B. Ducloué, E. Iancu, A.H. Mueller, G. Soyez, D.N. Triantafyllopoulos, JHEP 1904 (2019) 081
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spelling cern-27213952022-11-02T22:22:34Zhttp://cds.cern.ch/record/2721395engHänninen, HenriDipole model at Next-to-Leading Order meets HERA data10th International Conference on Hard and Electromagnetic Probes of High-Energy Nuclear CollisionsConferences<!--HTML-->Deep inelastic scattering (DIS) total cross section data at small-x as measured by the HERA experiments is well described by Balitsky-Kovchegov (BK) evolution in the leading order dipole picture [1-3]. Recently the full Next-to-Leading Order (NLO) dipole picture total cross sections have become available for DIS [4-6], and a working factorization scheme has been deviced which substracts the soft gluon divergence present at NLO [7]. We report our ongoing work in which we make the first comparisons of the NLO DIS total cross sections to HERA data. The non-perturbative initial condition to BK evolution is fixed by fitting the HERA reduced cross section data. As the NLO results for the DIS total cross section are currently available only in the massless quark limit, we also fit a light quark only cross section constructed with a parametrization of published total and heavy quark data. We find an excellent description of the HERA data. Since the full NLO BK equation is computationally expensive [8], we use a number of beyond LO prescriptions for the evolution that include most important higher order corrections enhanced by large transverse logarithms, including the recent version of the equation formulated in terms of the target rapidity [9]. [1] T. Lappi, H. Mäntysaari, Phys.Rev. D88 (2013) 114020 [2] E. Iancu, J.D. Madrigal, A.H. Mueller, G. Soyez, D.N. Triantafyllopoulos, Phys.Lett. B750 (2015) 643-652 [3] B. Ducloué, E. Iancu, G. Soyez, D.N. Triantafyllopoulos, arXiv:1912.09196 [hep-ph] [4] G. Beuf, Phys.Rev. D94 (2016) no.5, 054016 [5] G. Beuf, Phys.Rev. D96 (2017) no.7, 074033 [6] H. Hänninen, T. Lappi, R. Paatelainen, arXiv:1711.08207 [hep-ph] [7] B. Ducloué, H. Hänninen, T. Lappi, Y. Zhu, Phys.Rev. D96 (2017) no.9, 094017 [8] T. Lappi, H. Mäntysaari, Phys.Rev. D91 (2015) no.7, 074016 [9] B. Ducloué, E. Iancu, A.H. Mueller, G. Soyez, D.N. Triantafyllopoulos, JHEP 1904 (2019) 081oai:cds.cern.ch:27213952020
spellingShingle Conferences
Hänninen, Henri
Dipole model at Next-to-Leading Order meets HERA data
title Dipole model at Next-to-Leading Order meets HERA data
title_full Dipole model at Next-to-Leading Order meets HERA data
title_fullStr Dipole model at Next-to-Leading Order meets HERA data
title_full_unstemmed Dipole model at Next-to-Leading Order meets HERA data
title_short Dipole model at Next-to-Leading Order meets HERA data
title_sort dipole model at next-to-leading order meets hera data
topic Conferences
url http://cds.cern.ch/record/2721395
work_keys_str_mv AT hanninenhenri dipolemodelatnexttoleadingordermeetsheradata
AT hanninenhenri 10thinternationalconferenceonhardandelectromagneticprobesofhighenergynuclearcollisions