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dc.contributor.authorBeuf, G.
dc.contributor.authorLappi, T.
dc.contributor.authorPaatelainen, R.
dc.date.accessioned2022-09-06T11:37:17Z
dc.date.available2022-09-06T11:37:17Z
dc.date.issued2022
dc.identifier.citationBeuf, G., Lappi, T., & Paatelainen, R. (2022). Massive Quarks at One Loop in the Dipole Picture of Deep Inelastic Scattering. <i>Physical Review Letters</i>, <i>129</i>(7), Article 072001. <a href="https://doi.org/10.1103/PhysRevLett.129.072001" target="_blank">https://doi.org/10.1103/PhysRevLett.129.072001</a>
dc.identifier.otherCONVID_155853254
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/82968
dc.description.abstractWe calculate the light cone wave functions for a virtual photon to split into quark-antiquark states, including for the first time quark masses at one loop accuracy. These wave functions can be used to calculate cross sections for several precision probes of perturbative gluon saturation at the Electron-Ion Collider. Using these wave functions we derive, for the first time, the dipole picture deep inelastic scattering cross sections at one loop for longitudinal and transverse virtual photons including quark masses. The quark masses are renormalized in the pole mass scheme, satisfying constraints from the requirement of Lorentz invariance of the quark Dirac and Pauli form factors.en
dc.format.mimetypeapplication/pdf
dc.language.isoeng
dc.publisherAmerican Physical Society (APS)
dc.relation.ispartofseriesPhysical Review Letters
dc.rightsCC BY 4.0
dc.titleMassive Quarks at One Loop in the Dipole Picture of Deep Inelastic Scattering
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-202209064495
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.issn0031-9007
dc.relation.numberinseries7
dc.relation.volume129
dc.type.versionpublishedVersion
dc.rights.copyright© Authors, 2022
dc.rights.accesslevelopenAccessfi
dc.relation.grantnumber321840
dc.relation.grantnumber824093
dc.relation.grantnumber824093
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/H2020/681707/EU//CGCglasmaQGP
dc.subject.ysohiukkasfysiikka
dc.subject.ysokvarkit
dc.subject.ysosironta
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p15576
jyx.subject.urihttp://www.yso.fi/onto/yso/p19627
jyx.subject.urihttp://www.yso.fi/onto/yso/p1026
dc.rights.urlhttps://creativecommons.org/licenses/by/4.0/
dc.relation.doi10.1103/PhysRevLett.129.072001
dc.relation.funderResearch Council of Finlanden
dc.relation.funderEuropean Commissionen
dc.relation.funderEuropean Commissionen
dc.relation.funderSuomen Akatemiafi
dc.relation.funderEuroopan komissiofi
dc.relation.funderEuroopan komissiofi
jyx.fundingprogramAcademy Project, AoFen
jyx.fundingprogramRIA Research and Innovation Action, H2020en
jyx.fundingprogramERC European Research Council, H2020en
jyx.fundingprogramAkatemiahanke, SAfi
jyx.fundingprogramRIA Research and Innovation Action, H2020fi
jyx.fundingprogramERC European Research Council, H2020fi
jyx.fundinginformationThis work has been supported by the Academy of Finland, projects 321840 and 1322502, under the European Union’s Horizon 2020 research and innovation programme by the STRONG-2020 project (Grant Agreement No. 824093), by the European Research Council, Grant Agreements No. ERC-2015-CoG-681707 and No. ERC-2016-CoG-725369, and by the National Science Centre (Poland) under the research Grant No. 2020/38/E/ST2/00122 (SONATA BIS 10). The content of this Letter 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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