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dc.contributor.authorMäntysaari, Heikki
dc.contributor.authorPenttala, Jani
dc.date.accessioned2022-08-16T16:51:52Z
dc.date.available2022-08-16T16:51:52Z
dc.date.issued2022
dc.identifier.citationMäntysaari, H., & Penttala, J. (2022). Exclusive production of light vector mesons at next-to-leading order in the dipole picture. <i>Physical Review D</i>, <i>105</i>(11), Article 114038. <a href="https://doi.org/10.1103/PhysRevD.105.114038" target="_blank">https://doi.org/10.1103/PhysRevD.105.114038</a>
dc.identifier.otherCONVID_150943279
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/82598
dc.description.abstractExclusive production of light vector mesons in deep inelastic scattering is calculated at next-to-leading order in the dipole picture in the limit of high photon virtuality. The resulting expression is free of any divergences and suitable for numerical evaluations. The higher-order corrections are found to be numerically important, but they can be mostly captured by the nonperturbative fit parameters describing the initial condition for the small-x evolution of the dipole scattering amplitude. The vector meson production cross section is shown to depend only weakly on the meson distribution amplitude and the factorization scale. We also present phenomenological comparisons of our result to the existing exclusive ϕ and ρ production data from HERA and find an excellent agreement at high virtualities.en
dc.format.mimetypeapplication/pdf
dc.language.isoeng
dc.publisherAmerican Physical Society (APS)
dc.relation.ispartofseriesPhysical Review D
dc.rightsCC BY 4.0
dc.titleExclusive production of light vector mesons at next-to-leading order in the dipole picture
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-202208164142
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© The Authors 2022
dc.rights.accesslevelopenAccessfi
dc.relation.grantnumber835105
dc.relation.grantnumber835105
dc.relation.grantnumber338263
dc.relation.grantnumber824093
dc.relation.grantnumber824093
dc.relation.grantnumber346567
dc.relation.grantnumber321840
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.ysokvanttiväridynamiikka
dc.subject.ysohiukkasfysiikka
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p39318
jyx.subject.urihttp://www.yso.fi/onto/yso/p15576
dc.rights.urlhttps://creativecommons.org/licenses/by/4.0/
dc.relation.doi10.1103/PhysRevD.105.114038
dc.relation.funderEuropean Commissionen
dc.relation.funderResearch Council of Finlanden
dc.relation.funderEuropean Commissionen
dc.relation.funderResearch Council of Finlanden
dc.relation.funderResearch Council of Finlanden
dc.relation.funderEuroopan komissiofi
dc.relation.funderSuomen Akatemiafi
dc.relation.funderEuroopan komissiofi
dc.relation.funderSuomen Akatemiafi
dc.relation.funderSuomen Akatemiafi
jyx.fundingprogramERC Advanced Granten
jyx.fundingprogramAcademy Research Fellow, AoFen
jyx.fundingprogramRIA Research and Innovation Action, H2020en
jyx.fundingprogramResearch costs of Academy Research Fellow, AoFen
jyx.fundingprogramAcademy Project, AoFen
jyx.fundingprogramERC Advanced Grantfi
jyx.fundingprogramAkatemiatutkija, SAfi
jyx.fundingprogramRIA Research and Innovation Action, H2020fi
jyx.fundingprogramAkatemiatutkijan tutkimuskulut, SAfi
jyx.fundingprogramAkatemiahanke, SAfi
jyx.fundinginformationThis work was supported by the Academy of Finland, the Centre of Excellence in Quark Matter, and Projects No. 338263, No. 346567, and No. 321840, by the Finnish Cultural Foundation (J. P.), and 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). 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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