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dc.contributor.authorArmesto, Nestor
dc.contributor.authorLappi, Tuomas
dc.contributor.authorMäntysaari, Heikki
dc.contributor.authorPaukkunen, Hannu
dc.contributor.authorTevio, Mirja
dc.date.accessioned2022-08-16T08:55:10Z
dc.date.available2022-08-16T08:55:10Z
dc.date.issued2022
dc.identifier.citationArmesto, N., Lappi, T., Mäntysaari, H., Paukkunen, H., & Tevio, M. (2022). Signatures of gluon saturation from structure-function measurements. <i>Physical Review D</i>, <i>105</i>(11), Article 114017. <a href="https://doi.org/10.1103/PhysRevD.105.114017" target="_blank">https://doi.org/10.1103/PhysRevD.105.114017</a>
dc.identifier.otherCONVID_150899510
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/82584
dc.description.abstractWe study experimentally observable signals for nonlinear QCD dynamics in deep inelastic scattering (DIS) at small Bjorken variable x and moderate virtuality Q2, by quantifying differences between the linear Dokshitzer-Gribov-Lipatov-Altarelli-Parisi evolution and nonlinear evolution with the Balitsky-Kovchegov equation. To remove the effect of the parametrization freedom in the initial conditions of both equations, we first match the predictions for the DIS structure functions F2 and FL from both frameworks in a region in x, Q2 where both frameworks should provide an accurate description of the relevant physics. The differences in the dynamics are then quantified by the deviations when one moves away from this matching region. For free protons we find that the differences in F2 remain at a few-percent level, while in FL the deviations are larger, up to 10% at the Electron Ion Collider (EIC) and 40% at the Large Hadron-electron Collider (LHeC) kinematics. With a heavy nucleus the differences are up to 10% in F2, and can reach 20% and 60% in FL for the EIC and the LHeC, respectively.en
dc.format.mimetypeapplication/pdf
dc.language.isoeng
dc.publisherAmerican Physical Society (APS)
dc.relation.ispartofseriesPhysical Review D
dc.rightsCC BY 4.0
dc.titleSignatures of gluon saturation from structure-function measurements
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-202208164128
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.numberinseries11
dc.relation.volume105
dc.type.versionpublishedVersion
dc.rights.copyright© Authors, 2022
dc.rights.accesslevelopenAccessfi
dc.relation.grantnumber346567
dc.relation.grantnumber835105
dc.relation.grantnumber835105
dc.relation.grantnumber321840
dc.relation.grantnumber308301
dc.relation.grantnumber824093
dc.relation.grantnumber824093
dc.relation.grantnumber338263
dc.relation.grantnumber346324
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.ysokvanttiväridynamiikka
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p15576
jyx.subject.urihttp://www.yso.fi/onto/yso/p39318
dc.rights.urlhttps://creativecommons.org/licenses/by/4.0/
dc.relation.doi10.1103/PhysRevD.105.114017
dc.relation.funderResearch Council of Finlanden
dc.relation.funderEuropean Commissionen
dc.relation.funderResearch Council of Finlanden
dc.relation.funderResearch Council of Finlanden
dc.relation.funderEuropean Commissionen
dc.relation.funderResearch Council of Finlanden
dc.relation.funderResearch Council of Finlanden
dc.relation.funderSuomen Akatemiafi
dc.relation.funderEuroopan komissiofi
dc.relation.funderSuomen Akatemiafi
dc.relation.funderSuomen Akatemiafi
dc.relation.funderEuroopan komissiofi
dc.relation.funderSuomen Akatemiafi
dc.relation.funderSuomen Akatemiafi
jyx.fundingprogramResearch costs of Academy Research Fellow, AoFen
jyx.fundingprogramERC Advanced Granten
jyx.fundingprogramAcademy Project, AoFen
jyx.fundingprogramAcademy Research Fellow, AoFen
jyx.fundingprogramRIA Research and Innovation Action, H2020en
jyx.fundingprogramAcademy Research Fellow, AoFen
jyx.fundingprogramCentre of Excellence, AoFen
jyx.fundingprogramAkatemiatutkijan tutkimuskulut, SAfi
jyx.fundingprogramERC Advanced Grantfi
jyx.fundingprogramAkatemiahanke, SAfi
jyx.fundingprogramAkatemiatutkija, SAfi
jyx.fundingprogramRIA Research and Innovation Action, H2020fi
jyx.fundingprogramAkatemiatutkija, SAfi
jyx.fundingprogramHuippuyksikkörahoitus, SAfi
jyx.fundinginformationThis work was supported by the Academy of Finland, the Centre of Excellence in Quark Matter (Project No. 346324), and Projects No. 321840, No. 338263, No. 346567, and No. 308301. This work was also supported by the European Union’s Horizon 2020 research and innovation program under Grant Agreement No. 824093 and the European Research Council under Project No. ERC-2018-ADG-835105 YoctoLHC. N. A. acknowledges financial support by Xunta de Galicia (Centro singular de investigación de Galicia accreditation 2019–2022); the “María de Maeztu” Units of Excellence Program No. MDM2016-0692 and the Spanish Research State Agency under Project No. FPA2017-83814-P; European Union European Regional Development Fund (ERDF); and Marie Skłodowska-Curie Research and Innovation Staff Exchange (MSCA RISE) 823947 “Heavy ion collisions: collectivity and precision in saturation physics” (HIEIC); and the Spanish Research State Agency (Agencia Estatal de Investigación). 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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