dc.contributor.author | Hänninen, Henri | |
dc.contributor.author | Mäntysaari, Heikki | |
dc.contributor.author | Paatelainen, Risto | |
dc.contributor.author | Penttala, Jani | |
dc.date.accessioned | 2023-06-08T10:10:08Z | |
dc.date.available | 2023-06-08T10:10:08Z | |
dc.date.issued | 2023 | |
dc.identifier.citation | Hänninen, H., Mäntysaari, H., Paatelainen, R., & Penttala, J. (2023). Proton Structure Functions at Next-to-Leading Order in the Dipole Picture with Massive Quarks. <i>Physical Review Letters</i>, <i>130</i>(19), Article 192301. <a href="https://doi.org/10.1103/PhysRevLett.130.192301" target="_blank">https://doi.org/10.1103/PhysRevLett.130.192301</a> | |
dc.identifier.other | CONVID_183352491 | |
dc.identifier.uri | https://jyx.jyu.fi/handle/123456789/87574 | |
dc.description.abstract | We predict heavy quark production cross sections in deep inelastic scattering at high energy by applying the color glass condensate effective theory. We demonstrate that, when the calculation is performed consistently at next-to-leading order accuracy with massive quarks, it becomes possible, for the first time in the dipole picture with perturbatively calculated center-of-mass energy evolution, to simultaneously describe both the light and heavy quark production data at small xBj. Furthermore, we show how the heavy quark cross section data provides additional strong constraints on the extracted nonperturbative initial condition for the small-xBj evolution equations. | en |
dc.format.mimetype | application/pdf | |
dc.language.iso | eng | |
dc.publisher | American Physical Society (APS) | |
dc.relation.ispartofseries | Physical Review Letters | |
dc.rights | CC BY 4.0 | |
dc.title | Proton Structure Functions at Next-to-Leading Order in the Dipole Picture with Massive Quarks | |
dc.type | article | |
dc.identifier.urn | URN:NBN:fi:jyu-202306083643 | |
dc.contributor.laitos | Matematiikan ja tilastotieteen laitos | fi |
dc.contributor.laitos | Fysiikan laitos | fi |
dc.contributor.laitos | Department of Mathematics and Statistics | en |
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 | 0031-9007 | |
dc.relation.numberinseries | 19 | |
dc.relation.volume | 130 | |
dc.type.version | publishedVersion | |
dc.rights.copyright | © Authors 2023. Published by the American Physical Society | |
dc.rights.accesslevel | openAccess | fi |
dc.relation.grantnumber | 321840 | |
dc.relation.grantnumber | 338263 | |
dc.relation.grantnumber | 835105 | |
dc.relation.grantnumber | 835105 | |
dc.relation.grantnumber | 346567 | |
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/H2020/824093/EU//STRONG-2020 | |
dc.subject.yso | hiukkasfysiikka | |
dc.subject.yso | kvarkit | |
dc.subject.yso | kvanttiväridynamiikka | |
dc.format.content | fulltext | |
jyx.subject.uri | http://www.yso.fi/onto/yso/p15576 | |
jyx.subject.uri | http://www.yso.fi/onto/yso/p19627 | |
jyx.subject.uri | http://www.yso.fi/onto/yso/p39318 | |
dc.rights.url | https://creativecommons.org/licenses/by/4.0/ | |
dc.relation.doi | 10.1103/PhysRevLett.130.192301 | |
dc.relation.funder | Research Council of Finland | en |
dc.relation.funder | Research Council of Finland | 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 | Suomen Akatemia | fi |
dc.relation.funder | Euroopan komissio | fi |
dc.relation.funder | Suomen Akatemia | fi |
dc.relation.funder | Euroopan komissio | fi |
jyx.fundingprogram | Academy Project, AoF | en |
jyx.fundingprogram | Academy Research Fellow, AoF | en |
jyx.fundingprogram | ERC Advanced Grant | en |
jyx.fundingprogram | Research costs of Academy Research Fellow, AoF | en |
jyx.fundingprogram | RIA Research and Innovation Action, H2020 | en |
jyx.fundingprogram | Akatemiahanke, SA | fi |
jyx.fundingprogram | Akatemiatutkija, SA | fi |
jyx.fundingprogram | ERC Advanced Grant | fi |
jyx.fundingprogram | Akatemiatutkijan tutkimuskulut, SA | fi |
jyx.fundingprogram | RIA Research and Innovation Action, H2020 | fi |
jyx.fundinginformation | We thank T. Lappi for discussions, and V. Apaja for computational support. This work was supported by the Academy of Finland, the Centre of Excellence in Quark Matter and Projects No. 338263, No. 346567, No. 321840, No. 347499, and No. 353772. 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). J. P. is supported by the Finnish Cultural Foundation. 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. Computing resources from CSC–IT Center for Science in Espoo, Finland and from the Finnish Grid and Cloud Infrastructure (persistent identifier urn:nbn:fi:research-infras-2016072533) were used in this work. | |
dc.type.okm | A1 | |