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dc.contributor.authorBeuf, G.
dc.contributor.authorLappi, T.
dc.contributor.authorPaatelainen, R.
dc.date.accessioned2022-09-14T04:55:07Z
dc.date.available2022-09-14T04:55:07Z
dc.date.issued2022
dc.identifier.citationBeuf, G., Lappi, T., & Paatelainen, R. (2022). Massive quarks in NLO dipole factorization for DIS : Transverse photon. <i>Physical Review D</i>, <i>106</i>(3), Article 034013. <a href="https://doi.org/10.1103/PhysRevD.106.034013" target="_blank">https://doi.org/10.1103/PhysRevD.106.034013</a>
dc.identifier.otherCONVID_156469905
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/83230
dc.description.abstractWe calculate the light-cone wave functions for the QCD Fock components in a transverse virtual photon necessary for applications at next-to-leading order (NLO) in the QCD coupling, including quark masses. We present a detailed calculation of both the one-loop wave function for the quark-antiquark Fock component and the tree-level wave function for the quark-antiquark-gluon Fock component. The quark masses are renormalized in the pole mass scheme, satisfying constraints from the requirement of Lorentz invariance. In particular the quark Pauli form factor at NLO is recovered from the on-shell limit of the quark-antiquark Fock component. We use our result to calculate the next-to-leading-order correction to the high energy deep inelastic scattering (DIS) transverse structure function on a dense target in the dipole factorization framework. Together with our earlier result for longitudinal photons, this completes the calculation of the total deep inelastic scattering cross section in the dipole picture with massive quarks at next-to-leading order, enabling a comparison with experimental data.en
dc.format.mimetypeapplication/pdf
dc.language.isoeng
dc.publisherAmerican Physical Society (APS)
dc.relation.ispartofseriesPhysical Review D
dc.rightsCC BY 4.0
dc.titleMassive quarks in NLO dipole factorization for DIS : Transverse photon
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-202209144576
dc.contributor.laitosFysiikan laitosfi
dc.contributor.laitosDepartment of Physicsen
dc.type.urihttp://purl.org/eprint/type/JournalArticle
dc.type.coarhttp://purl.org/coar/resource_type/c_2df8fbb1
dc.description.reviewstatuspeerReviewed
dc.relation.issn2470-0010
dc.relation.numberinseries3
dc.relation.volume106
dc.type.versionpublishedVersion
dc.rights.copyright© Authors, 2022
dc.rights.accesslevelopenAccessfi
dc.relation.grantnumber346324
dc.relation.grantnumber835105
dc.relation.grantnumber835105
dc.relation.grantnumber681707
dc.relation.grantnumber681707
dc.relation.grantnumber321840
dc.relation.grantnumber824093
dc.relation.grantnumber824093
dc.relation.projectidinfo:eu-repo/grantAgreement/EC/H2020/835105/EU//YoctoLHC
dc.relation.projectidinfo:eu-repo/grantAgreement/EC/H2020/681707/EU//CGCglasmaQGP
dc.relation.projectidinfo:eu-repo/grantAgreement/EC/H2020/824093/EU//STRONG-2020
dc.subject.ysofotonit
dc.subject.ysohiukkasfysiikka
dc.subject.ysosironta
dc.subject.ysokvanttiväridynamiikka
dc.subject.ysokvarkit
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p2063
jyx.subject.urihttp://www.yso.fi/onto/yso/p15576
jyx.subject.urihttp://www.yso.fi/onto/yso/p1026
jyx.subject.urihttp://www.yso.fi/onto/yso/p39318
jyx.subject.urihttp://www.yso.fi/onto/yso/p19627
dc.rights.urlhttps://creativecommons.org/licenses/by/4.0/
dc.relation.doi10.1103/PhysRevD.106.034013
dc.relation.funderResearch Council of Finlanden
dc.relation.funderEuropean Commissionen
dc.relation.funderEuropean Commissionen
dc.relation.funderResearch Council of Finlanden
dc.relation.funderEuropean Commissionen
dc.relation.funderSuomen Akatemiafi
dc.relation.funderEuroopan komissiofi
dc.relation.funderEuroopan komissiofi
dc.relation.funderSuomen Akatemiafi
dc.relation.funderEuroopan komissiofi
jyx.fundingprogramCentre of Excellence, AoFen
jyx.fundingprogramERC Advanced Granten
jyx.fundingprogramERC European Research Council, H2020en
jyx.fundingprogramAcademy Project, AoFen
jyx.fundingprogramRIA Research and Innovation Action, H2020en
jyx.fundingprogramHuippuyksikkörahoitus, SAfi
jyx.fundingprogramERC Advanced Grantfi
jyx.fundingprogramERC European Research Council, H2020fi
jyx.fundingprogramAkatemiahanke, SAfi
jyx.fundingprogramRIA Research and Innovation Action, H2020fi
jyx.fundinginformationThis work has been supported by the Academy of Finland Centre of Excellence in Quark Matter (Project No. 346324) and Projects No. 321840 and No. 322507, under the European Unions Horizon 2020 research and innovation program by the STRONG-2020 project (Grant Agreement No. 824093), by the European Research Council, Grant Agreements No. ERC-2015-CoG-681707, No. ERC-2016-CoG-725369, and No. ERC-2018-AdG-835105 and by the National Science Centre (Poland) under the research Grant No. 2020/38/E/ST2/00122 (SONATA BIS 10). The content of this article does not reflect the official opinion of the European Union and responsibility for the information and views expressed therein lies entirely with the authors.
dc.type.okmA1


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