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Diffractive deep inelastic scattering at NLO in the dipole picture : The qq¯g contribution

dc.contributor.authorBeuf, G.
dc.contributor.authorHänninen, H.
dc.contributor.authorLappi, T.
dc.contributor.authorMulian, Y.
dc.contributor.authorMäntysaari, H.
dc.date.accessioned2023-01-13T10:55:26Z
dc.date.available2023-01-13T10:55:26Z
dc.date.issued2022
dc.identifier.citationBeuf, G., Hänninen, H., Lappi, T., Mulian, Y., & Mäntysaari, H. (2022). Diffractive deep inelastic scattering at NLO in the dipole picture : The qq¯g contribution. <i>Physical Review D</i>, <i>106</i>(9), Article 094014. <a href="https://doi.org/10.1103/PhysRevD.106.094014" target="_blank">https://doi.org/10.1103/PhysRevD.106.094014</a>
dc.identifier.otherCONVID_164981336
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/84999
dc.description.abstractWe calculate the contribution from the qq¯g state production to the diffractive cross sections in deep inelastic scattering at high energy. The obtained cross section is finite by itself and a part of the full next-to-leading order result for the diffractive structure functions. We perform the calculation in exact kinematics in the eikonal limit, and show that the previously known high-Q2 and large MX2 results for the structure functions can be extracted from our results in the appropriate limits. We furthermore discuss the steps required to obtain the full next-to-leading order results for the structure functions. © 2022 authors.en
dc.format.mimetypeapplication/pdf
dc.language.isoeng
dc.publisherAmerican Physical Society (APS)
dc.relation.ispartofseriesPhysical Review D
dc.rightsCC BY 4.0
dc.titleDiffractive deep inelastic scattering at NLO in the dipole picture : The qq¯g contribution
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-202301131309
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.numberinseries9
dc.relation.volume106
dc.type.versionpublishedVersion
dc.rights.copyright© Authors, 2022
dc.rights.accesslevelopenAccessfi
dc.relation.grantnumber321840
dc.relation.grantnumber824093
dc.relation.grantnumber824093
dc.relation.grantnumber346567
dc.relation.grantnumber346324
dc.relation.grantnumber338263
dc.relation.grantnumber835105
dc.relation.grantnumber835105
dc.relation.projectidinfo:eu-repo/grantAgreement/EC/H2020/824093/EU//STRONG-2020
dc.relation.projectidinfo:eu-repo/grantAgreement/EC/H2020/835105/EU//YoctoLHC
dc.subject.ysosironta
dc.subject.ysohiukkasfysiikka
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p1026
jyx.subject.urihttp://www.yso.fi/onto/yso/p15576
dc.rights.urlhttps://creativecommons.org/licenses/by/4.0/
dc.relation.doi10.1103/PhysRevD.106.094014
dc.relation.funderResearch Council of Finlanden
dc.relation.funderEuropean Commissionen
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.funderEuroopan komissiofi
dc.relation.funderSuomen Akatemiafi
dc.relation.funderSuomen Akatemiafi
dc.relation.funderSuomen Akatemiafi
dc.relation.funderEuroopan komissiofi
jyx.fundingprogramAcademy Project, AoFen
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.fundingprogramERC Advanced Granten
jyx.fundingprogramAkatemiahanke, SAfi
jyx.fundingprogramRIA Research and Innovation Action, H2020fi
jyx.fundingprogramAkatemiatutkijan tutkimuskulut, SAfi
jyx.fundingprogramHuippuyksikkörahoitus, SAfi
jyx.fundingprogramAkatemiatutkija, SAfi
jyx.fundingprogramERC Advanced Grantfi
jyx.fundinginformationWe thank K. Golec-Biernat, A. van Hameren, C. Marquet, R. Paatelainen, and J. Penttala for discussions. H. H., T. L., and H. M. are supported by the Academy of Finland, the Centre of Excellence in Quark Matter (project 346324) and Projects No. 338263, No. 346567, and No. 321840. G. B. is supported in part by the National Science Centre (Poland) under the research Grant No. 2020/38/E/ST2/00122 (SONATA BIS 10). Y. M. acknowledges financial support from Xunta de Galicia (Centro singular de investigación de Galicia accreditation 2019–2022); the “María de Maeztu” Units of Excellence program MDM2016-0692 and the Spanish Research State Agency under Project No. PID2020–119632 GB-I00; European Union ERDF. G. B. and Y. M. acknowledge financial support from MSCA RISE 823947 “Heavy ion collisions: collectivity and precision in saturation physics” (HIEIC). 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). 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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