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dc.contributor.authorMäntysaari, Heikki
dc.contributor.authorPenttala, Jani
dc.date.accessioned2021-11-26T09:25:22Z
dc.date.available2021-11-26T09:25:22Z
dc.date.issued2021
dc.identifier.citationMäntysaari, H., & Penttala, J. (2021). Exclusive heavy vector meson production at next-to-leading order in the dipole picture. <i>Physics Letters B</i>, <i>823</i>, Article 136723. <a href="https://doi.org/10.1016/j.physletb.2021.136723" target="_blank">https://doi.org/10.1016/j.physletb.2021.136723</a>
dc.identifier.otherCONVID_102018193
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/78808
dc.description.abstractWe calculate exclusive production of a longitudinally polarized heavy vector meson at next-to-leading order in the dipole picture. The large quark mass allows us to separately include both the first QCD correction proportional to the coupling constant αs, and the first relativistic correction suppressed by the quark velocity v2. Both of these corrections are found to be numerically important in J/ψ production. The results obtained are directly suitable for phenomenological calculations. We also demonstrate how vector meson production provides complementary information to structure function analyses when one extracts the initial condition for the energy evolution of the proton small-x structure.en
dc.format.mimetypeapplication/pdf
dc.language.isoeng
dc.publisherElsevier BV
dc.relation.ispartofseriesPhysics Letters B
dc.rightsCC BY 4.0
dc.titleExclusive heavy vector meson production at next-to-leading order in the dipole picture
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-202111265814
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.issn0370-2693
dc.relation.volume823
dc.type.versionpublishedVersion
dc.rights.copyright© 2021 The Author(s). Published by Elsevier B.V. Funded by SCOAP3.
dc.rights.accesslevelopenAccessfi
dc.relation.grantnumber321840
dc.relation.grantnumber346567
dc.relation.grantnumber314764
dc.relation.grantnumber338263
dc.relation.grantnumber824093
dc.relation.grantnumber824093
dc.relation.projectidinfo:eu-repo/grantAgreement/EC/H2020/824093/EU//STRONG-2020
dc.subject.ysokvarkit
dc.subject.ysohiukkasfysiikka
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p19627
jyx.subject.urihttp://www.yso.fi/onto/yso/p15576
dc.rights.urlhttps://creativecommons.org/licenses/by/4.0/
dc.relation.doi10.1016/j.physletb.2021.136723
dc.relation.funderResearch Council of Finlanden
dc.relation.funderResearch Council of Finlanden
dc.relation.funderResearch Council of Finlanden
dc.relation.funderResearch Council of Finlanden
dc.relation.funderEuropean Commissionen
dc.relation.funderSuomen Akatemiafi
dc.relation.funderSuomen Akatemiafi
dc.relation.funderSuomen Akatemiafi
dc.relation.funderSuomen Akatemiafi
dc.relation.funderEuroopan komissiofi
jyx.fundingprogramAcademy Project, AoFen
jyx.fundingprogramResearch costs of Academy Research Fellow, AoFen
jyx.fundingprogramPostdoctoral Researcher, AoFen
jyx.fundingprogramAcademy Research Fellow, AoFen
jyx.fundingprogramRIA Research and Innovation Action, H2020en
jyx.fundingprogramAkatemiahanke, SAfi
jyx.fundingprogramAkatemiatutkijan tutkimuskulut, SAfi
jyx.fundingprogramTutkijatohtori, SAfi
jyx.fundingprogramAkatemiatutkija, SAfi
jyx.fundingprogramRIA Research and Innovation Action, H2020fi
jyx.fundinginformationThis work was supported by the Academy of Finland, projects 314764, 338263 and 346567 (H.M.) and 321840 (J.P.), and by the EU Horizon 2020 research and innovation programme, 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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