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dc.contributor.authorDemirci, S.
dc.contributor.authorLappi, T.
dc.contributor.authorSchlichting, S.
dc.date.accessioned2023-01-04T11:38:10Z
dc.date.available2023-01-04T11:38:10Z
dc.date.issued2022
dc.identifier.citationDemirci, S., Lappi, T., & Schlichting, S. (2022). Proton hot spots and exclusive vector meson production. <i>Physical Review D</i>, <i>106</i>(7), Article 074025. <a href="https://doi.org/10.1103/PhysRevD.106.074025" target="_blank">https://doi.org/10.1103/PhysRevD.106.074025</a>
dc.identifier.otherCONVID_164724265
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/84770
dc.description.abstractWe explore consequences of the existence of gluonic hot spots inside the proton for coherent and incoherent exclusive vector meson production cross sections in deep inelastic scattering. By working in the dilute limit of the Color Glass Condensate framework to compute the cross sections for Gaussian hot spots of fluctuating color charges and employing a nonrelativistic vector meson wave function, we are able to perform large parts of the calculation analytically. We find that the coherent cross section is sensitive to both the size of the target and the structure of the probe. The incoherent cross section is dominated by color fluctuations at small transverse momentum transfer (t), by proton and hot spot sizes as well as the structure of the probe at medium t and again by color fluctuations at large t. While the t-dependence of the cross section is well reproduced in our model, the relative normalization between the coherent and the incoherent cross sections points to the need for additional fluctuations in the proton.en
dc.format.mimetypeapplication/pdf
dc.language.isoeng
dc.publisherAmerican Physical Society (APS)
dc.relation.ispartofseriesPhysical Review D
dc.rightsCC BY 4.0
dc.titleProton hot spots and exclusive vector meson production
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-202301041125
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.numberinseries7
dc.relation.volume106
dc.type.versionpublishedVersion
dc.rights.copyright© Authors, 2022
dc.rights.accesslevelopenAccessfi
dc.relation.grantnumber321840
dc.relation.grantnumber346324
dc.relation.grantnumber824093
dc.relation.grantnumber824093
dc.relation.grantnumber835105
dc.relation.grantnumber835105
dc.relation.grantnumber681707
dc.relation.grantnumber681707
dc.relation.projectidinfo:eu-repo/grantAgreement/EC/H2020/824093/EU//STRONG-2020
dc.relation.projectidinfo:eu-repo/grantAgreement/EC/H2020/835105/EU//YoctoLHC
dc.relation.projectidinfo:eu-repo/grantAgreement/EC/H2020/681707/EU//CGCglasmaQGP
dc.subject.ysohiukkasfysiikka
dc.subject.ysokvanttiväridynamiikka
dc.subject.ysoprotonit
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p15576
jyx.subject.urihttp://www.yso.fi/onto/yso/p39318
jyx.subject.urihttp://www.yso.fi/onto/yso/p12428
dc.rights.urlhttps://creativecommons.org/licenses/by/4.0/
dc.relation.doi10.1103/PhysRevD.106.074025
dc.relation.funderResearch Council of Finlanden
dc.relation.funderResearch Council of Finlanden
dc.relation.funderEuropean Commissionen
dc.relation.funderEuropean Commissionen
dc.relation.funderEuropean Commissionen
dc.relation.funderSuomen Akatemiafi
dc.relation.funderSuomen Akatemiafi
dc.relation.funderEuroopan komissiofi
dc.relation.funderEuroopan komissiofi
dc.relation.funderEuroopan komissiofi
jyx.fundingprogramAcademy Project, AoFen
jyx.fundingprogramCentre of Excellence, AoFen
jyx.fundingprogramRIA Research and Innovation Action, H2020en
jyx.fundingprogramERC Advanced Granten
jyx.fundingprogramERC European Research Council, H2020en
jyx.fundingprogramAkatemiahanke, SAfi
jyx.fundingprogramHuippuyksikkörahoitus, SAfi
jyx.fundingprogramRIA Research and Innovation Action, H2020fi
jyx.fundingprogramERC Advanced Grantfi
jyx.fundingprogramERC European Research Council, H2020fi
jyx.fundinginformationS. D. acknowledges the support of the Vilho, Yrjö and Kalle Väisälä Foundation. S. S. acknowledges support by the Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) through the CRC-TR 211 ’Strong-interaction matter under extreme conditions’- Project No. 315477589—TRR 211. S. D. and T. L. have been supported by the Academy of Finland, by the Centre of Excellence in Quark Matter (Project No. 346324) and Project No. 321840. This work has also been supported under the European Union’s Horizon 2020 research and innovation programme by the STRONG-2020 project (Grant Agreement No. 824093) and by the European Research Council, Grant Agreements No. ERC-2015-CoG-681707 and No. ERC-2018-AdG-835105. 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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