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dc.contributor.authorLappi, Tuomas
dc.contributor.authorLe, Anh Dung
dc.contributor.authorMäntysaari, Heikki
dc.date.accessioned2024-02-16T08:48:51Z
dc.date.available2024-02-16T08:48:51Z
dc.date.issued2023
dc.identifier.citationLappi, T., Le, A. D., & Mäntysaari, H. (2023). Rapidity gap distribution of diffractive small-xp events at HERA and at the EIC. <i>Physical Review D</i>, <i>108</i>(11), Article 114023. <a href="https://doi.org/10.1103/PhysRevD.108.114023" target="_blank">https://doi.org/10.1103/PhysRevD.108.114023</a>
dc.identifier.otherCONVID_202857758
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/93436
dc.description.abstractWe use the Kovchegov-Levin equation to resum contributions of large invariant mass diffractive final states to diffractive structure functions in the dipole picture of deep inelastic scattering. For protons we use a (modified) McLerran-Venugopalan model as the initial condition for the evolution, with free parameters obtained from fits to the HERA inclusive data. We obtain an adequate agreement to the HERA diffractive data in the moderately high-mass regimes when the proton density profile is fitted to the diffractive structure function data in the low-mass region. The HERA data is found to prefer a proton shape that is steeper than a Gaussian. The initial conditions are generalized to the nuclear case using the optical Glauber model. Strong nuclear modification effects are predicted in diffractive scattering off a nuclear target in kinematics accessible at the future Electron-Ion Collider. In particular, the Kovchegov-Levin evolution has a strong effect on the Q2-dependence of the diffractive cross section.en
dc.format.mimetypeapplication/pdf
dc.language.isoeng
dc.publisherAmerican Physical Society (APS)
dc.relation.ispartofseriesPhysical Review D
dc.rightsCC BY 4.0
dc.subject.otherdeep inelastic scattering
dc.subject.otherdiffractive production
dc.subject.otherphenomenology
dc.subject.otherquantum chromodynamics
dc.titleRapidity gap distribution of diffractive small-xp events at HERA and at the EIC
dc.typeresearch article
dc.identifier.urnURN:NBN:fi:jyu-202402161912
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.volume108
dc.type.versionpublishedVersion
dc.rights.copyright© Authors 2023
dc.rights.accesslevelopenAccessfi
dc.type.publicationarticle
dc.relation.grantnumber824093
dc.relation.grantnumber824093
dc.relation.grantnumber346567
dc.relation.grantnumber346324
dc.relation.grantnumber338263
dc.relation.grantnumber321840
dc.relation.projectidinfo:eu-repo/grantAgreement/EC/H2020/824093/EU//STRONG-2020
dc.subject.ysofenomenologia
dc.subject.ysosironta
dc.subject.ysokvanttiväridynamiikka
dc.subject.ysodiffraktio
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p2977
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/p39312
dc.rights.urlhttps://creativecommons.org/licenses/by/4.0/
dc.relation.doi10.1103/PhysRevD.108.114023
dc.relation.funderEuropean Commissionen
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.funderEuroopan komissiofi
dc.relation.funderSuomen Akatemiafi
dc.relation.funderSuomen Akatemiafi
dc.relation.funderSuomen Akatemiafi
dc.relation.funderSuomen Akatemiafi
jyx.fundingprogramRIA Research and Innovation Action, H2020en
jyx.fundingprogramResearch costs of Academy Research Fellow, AoFen
jyx.fundingprogramCentre of Excellence, AoFen
jyx.fundingprogramAcademy Research Fellow, AoFen
jyx.fundingprogramAcademy Project, AoFen
jyx.fundingprogramRIA Research and Innovation Action, H2020fi
jyx.fundingprogramAkatemiatutkijan tutkimuskulut, SAfi
jyx.fundingprogramHuippuyksikkörahoitus, SAfi
jyx.fundingprogramAkatemiatutkija, SAfi
jyx.fundingprogramAkatemiahanke, SAfi
jyx.fundinginformationThis work was supported by the Academy of Finland, the Centre of Excellence in Quark Matter (Project 346324) and Projects 338263 and 346567 (H. M), and 321840 (T. L). 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).
dc.type.okmA1


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