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dc.contributor.authorHänninen, Henri
dc.contributor.authorMäntysaari, Heikki
dc.contributor.authorPaatelainen, Risto
dc.contributor.authorPenttala, Jani
dc.date.accessioned2023-06-08T10:10:08Z
dc.date.available2023-06-08T10:10:08Z
dc.date.issued2023
dc.identifier.citationHänninen, H., Mäntysaari, H., Paatelainen, R., & Penttala, J. (2023). Proton Structure Functions at Next-to-Leading Order in the Dipole Picture with Massive Quarks. <i>Physical Review Letters</i>, <i>130</i>(19), Article 192301. <a href="https://doi.org/10.1103/PhysRevLett.130.192301" target="_blank">https://doi.org/10.1103/PhysRevLett.130.192301</a>
dc.identifier.otherCONVID_183352491
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/87574
dc.description.abstractWe predict heavy quark production cross sections in deep inelastic scattering at high energy by applying the color glass condensate effective theory. We demonstrate that, when the calculation is performed consistently at next-to-leading order accuracy with massive quarks, it becomes possible, for the first time in the dipole picture with perturbatively calculated center-of-mass energy evolution, to simultaneously describe both the light and heavy quark production data at small xBj. Furthermore, we show how the heavy quark cross section data provides additional strong constraints on the extracted nonperturbative initial condition for the small-xBj evolution equations.en
dc.format.mimetypeapplication/pdf
dc.language.isoeng
dc.publisherAmerican Physical Society (APS)
dc.relation.ispartofseriesPhysical Review Letters
dc.rightsCC BY 4.0
dc.titleProton Structure Functions at Next-to-Leading Order in the Dipole Picture with Massive Quarks
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-202306083643
dc.contributor.laitosMatematiikan ja tilastotieteen laitosfi
dc.contributor.laitosFysiikan laitosfi
dc.contributor.laitosDepartment of Mathematics and Statisticsen
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.issn0031-9007
dc.relation.numberinseries19
dc.relation.volume130
dc.type.versionpublishedVersion
dc.rights.copyright© Authors 2023. Published by the American Physical Society
dc.rights.accesslevelopenAccessfi
dc.relation.grantnumber321840
dc.relation.grantnumber338263
dc.relation.grantnumber835105
dc.relation.grantnumber835105
dc.relation.grantnumber346567
dc.relation.grantnumber824093
dc.relation.grantnumber824093
dc.relation.projectidinfo:eu-repo/grantAgreement/EC/H2020/835105/EU//YoctoLHC
dc.relation.projectidinfo:eu-repo/grantAgreement/EC/H2020/824093/EU//STRONG-2020
dc.subject.ysohiukkasfysiikka
dc.subject.ysokvarkit
dc.subject.ysokvanttiväridynamiikka
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p15576
jyx.subject.urihttp://www.yso.fi/onto/yso/p19627
jyx.subject.urihttp://www.yso.fi/onto/yso/p39318
dc.rights.urlhttps://creativecommons.org/licenses/by/4.0/
dc.relation.doi10.1103/PhysRevLett.130.192301
dc.relation.funderResearch Council of Finlanden
dc.relation.funderResearch Council of Finlanden
dc.relation.funderEuropean Commissionen
dc.relation.funderResearch Council of Finlanden
dc.relation.funderEuropean Commissionen
dc.relation.funderSuomen Akatemiafi
dc.relation.funderSuomen Akatemiafi
dc.relation.funderEuroopan komissiofi
dc.relation.funderSuomen Akatemiafi
dc.relation.funderEuroopan komissiofi
jyx.fundingprogramAcademy Project, AoFen
jyx.fundingprogramAcademy Research Fellow, AoFen
jyx.fundingprogramERC Advanced Granten
jyx.fundingprogramResearch costs of Academy Research Fellow, AoFen
jyx.fundingprogramRIA Research and Innovation Action, H2020en
jyx.fundingprogramAkatemiahanke, SAfi
jyx.fundingprogramAkatemiatutkija, SAfi
jyx.fundingprogramERC Advanced Grantfi
jyx.fundingprogramAkatemiatutkijan tutkimuskulut, SAfi
jyx.fundingprogramRIA Research and Innovation Action, H2020fi
jyx.fundinginformationWe thank T. Lappi for discussions, and V. Apaja for computational support. This work was supported by the Academy of Finland, the Centre of Excellence in Quark Matter and Projects No. 338263, No. 346567, No. 321840, No. 347499, and No. 353772. This work was also supported under the European Union’s Horizon 2020 research and innovation programme by the European Research Council (ERC, Grant Agreement No. ERC-2018-ADG-835105 YoctoLHC) and by the STRONG-2020 project (Grant Agreement No. 824093). J. P. is supported by the Finnish Cultural Foundation. 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. Computing resources from CSC–IT Center for Science in Espoo, Finland and from the Finnish Grid and Cloud Infrastructure (persistent identifier urn:nbn:fi:research-infras-2016072533) were used in this work.
dc.type.okmA1


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