dc.contributor.author | Beuf, G. | |
dc.contributor.author | Lappi, T. | |
dc.contributor.author | Paatelainen, R. | |
dc.date.accessioned | 2022-09-14T04:55:07Z | |
dc.date.available | 2022-09-14T04:55:07Z | |
dc.date.issued | 2022 | |
dc.identifier.citation | Beuf, G., Lappi, T., & Paatelainen, R. (2022). Massive quarks in NLO dipole factorization for DIS : Transverse photon. <i>Physical Review D</i>, <i>106</i>(3), Article 034013. <a href="https://doi.org/10.1103/PhysRevD.106.034013" target="_blank">https://doi.org/10.1103/PhysRevD.106.034013</a> | |
dc.identifier.other | CONVID_156469905 | |
dc.identifier.uri | https://jyx.jyu.fi/handle/123456789/83230 | |
dc.description.abstract | We calculate the light-cone wave functions for the QCD Fock components in a transverse virtual photon necessary for applications at next-to-leading order (NLO) in the QCD coupling, including quark masses. We present a detailed calculation of both the one-loop wave function for the quark-antiquark Fock component and the tree-level wave function for the quark-antiquark-gluon Fock component. The quark masses are renormalized in the pole mass scheme, satisfying constraints from the requirement of Lorentz invariance. In particular the quark Pauli form factor at NLO is recovered from the on-shell limit of the quark-antiquark Fock component. We use our result to calculate the next-to-leading-order correction to the high energy deep inelastic scattering (DIS) transverse structure function on a dense target in the dipole factorization framework. Together with our earlier result for longitudinal photons, this completes the calculation of the total deep inelastic scattering cross section in the dipole picture with massive quarks at next-to-leading order, enabling a comparison with experimental data. | en |
dc.format.mimetype | application/pdf | |
dc.language.iso | eng | |
dc.publisher | American Physical Society (APS) | |
dc.relation.ispartofseries | Physical Review D | |
dc.rights | CC BY 4.0 | |
dc.title | Massive quarks in NLO dipole factorization for DIS : Transverse photon | |
dc.type | article | |
dc.identifier.urn | URN:NBN:fi:jyu-202209144576 | |
dc.contributor.laitos | Fysiikan laitos | fi |
dc.contributor.laitos | Department of Physics | en |
dc.type.uri | http://purl.org/eprint/type/JournalArticle | |
dc.type.coar | http://purl.org/coar/resource_type/c_2df8fbb1 | |
dc.description.reviewstatus | peerReviewed | |
dc.relation.issn | 2470-0010 | |
dc.relation.numberinseries | 3 | |
dc.relation.volume | 106 | |
dc.type.version | publishedVersion | |
dc.rights.copyright | © Authors, 2022 | |
dc.rights.accesslevel | openAccess | fi |
dc.relation.grantnumber | 346324 | |
dc.relation.grantnumber | 835105 | |
dc.relation.grantnumber | 835105 | |
dc.relation.grantnumber | 681707 | |
dc.relation.grantnumber | 681707 | |
dc.relation.grantnumber | 321840 | |
dc.relation.grantnumber | 824093 | |
dc.relation.grantnumber | 824093 | |
dc.relation.projectid | info:eu-repo/grantAgreement/EC/H2020/835105/EU//YoctoLHC | |
dc.relation.projectid | info:eu-repo/grantAgreement/EC/H2020/681707/EU//CGCglasmaQGP | |
dc.relation.projectid | info:eu-repo/grantAgreement/EC/H2020/824093/EU//STRONG-2020 | |
dc.subject.yso | fotonit | |
dc.subject.yso | hiukkasfysiikka | |
dc.subject.yso | sironta | |
dc.subject.yso | kvanttiväridynamiikka | |
dc.subject.yso | kvarkit | |
dc.format.content | fulltext | |
jyx.subject.uri | http://www.yso.fi/onto/yso/p2063 | |
jyx.subject.uri | http://www.yso.fi/onto/yso/p15576 | |
jyx.subject.uri | http://www.yso.fi/onto/yso/p1026 | |
jyx.subject.uri | http://www.yso.fi/onto/yso/p39318 | |
jyx.subject.uri | http://www.yso.fi/onto/yso/p19627 | |
dc.rights.url | https://creativecommons.org/licenses/by/4.0/ | |
dc.relation.doi | 10.1103/PhysRevD.106.034013 | |
dc.relation.funder | Research Council of Finland | en |
dc.relation.funder | European Commission | en |
dc.relation.funder | European Commission | en |
dc.relation.funder | Research Council of Finland | en |
dc.relation.funder | European Commission | en |
dc.relation.funder | Suomen Akatemia | fi |
dc.relation.funder | Euroopan komissio | fi |
dc.relation.funder | Euroopan komissio | fi |
dc.relation.funder | Suomen Akatemia | fi |
dc.relation.funder | Euroopan komissio | fi |
jyx.fundingprogram | Centre of Excellence, AoF | en |
jyx.fundingprogram | ERC Advanced Grant | en |
jyx.fundingprogram | ERC European Research Council, H2020 | en |
jyx.fundingprogram | Academy Project, AoF | en |
jyx.fundingprogram | RIA Research and Innovation Action, H2020 | en |
jyx.fundingprogram | Huippuyksikkörahoitus, SA | fi |
jyx.fundingprogram | ERC Advanced Grant | fi |
jyx.fundingprogram | ERC European Research Council, H2020 | fi |
jyx.fundingprogram | Akatemiahanke, SA | fi |
jyx.fundingprogram | RIA Research and Innovation Action, H2020 | fi |
jyx.fundinginformation | This work has been supported by the Academy of Finland Centre of Excellence in Quark Matter (Project No. 346324) and Projects No. 321840 and No. 322507, under the European Unions Horizon 2020 research and innovation program by the STRONG-2020 project (Grant Agreement No. 824093), by the European Research Council, Grant Agreements No. ERC-2015-CoG-681707, No. ERC-2016-CoG-725369, and No. ERC-2018-AdG-835105 and by the National Science Centre (Poland) under the research Grant No. 2020/38/E/ST2/00122 (SONATA BIS 10). 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.okm | A1 | |