Massive quarks in NLO dipole factorization for DIS : Longitudinal photon

Beuf, G.; Lappi, T.; Paatelainen, R.

doi:10.1103/PhysRevD.104.056032

dc.contributor.author	Beuf, G.
dc.contributor.author	Lappi, T.
dc.contributor.author	Paatelainen, R.
dc.date.accessioned	2021-11-11T11:36:16Z
dc.date.available	2021-11-11T11:36:16Z
dc.date.issued	2021
dc.identifier.citation	Beuf, G., Lappi, T., & Paatelainen, R. (2021). Massive quarks in NLO dipole factorization for DIS : Longitudinal photon. <i>Physical Review D</i>, <i>104</i>(5), Article 056032. <a href="https://doi.org/10.1103/PhysRevD.104.056032" target="_blank">https://doi.org/10.1103/PhysRevD.104.056032</a>
dc.identifier.other	CONVID_101867373
dc.identifier.uri	https://jyx.jyu.fi/handle/123456789/78627
dc.description.abstract	In this work, we will present the first complete calculation of the one-loop longitudinal photon-to-quark-antiquark light cone wave function, with massive quarks. The quark masses are renormalized in the pole mass scheme. The result is used to calculate the next-to-leading order correction to the high energy deep inelastic scattering longitudinal structure function on a dense target in the dipole factorization framework. For massless quarks the next-to-leading order correction was already known to be sizeable, and our result makes it possible to evaluate it also for massive quarks.	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 : Longitudinal photon
dc.type	article
dc.identifier.urn	URN:NBN:fi:jyu-202111115644
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	5
dc.relation.volume	104
dc.type.version	publishedVersion
dc.rights.copyright	© Authors, 2021
dc.rights.accesslevel	openAccess	fi
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/H2020/681707/EU//CGCglasmaQGP
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/PhysRevD.104.056032
dc.relation.funder	European Commission	en
dc.relation.funder	Research Council of Finland	en
dc.relation.funder	European Commission	en
dc.relation.funder	Euroopan komissio	fi
dc.relation.funder	Suomen Akatemia	fi
dc.relation.funder	Euroopan komissio	fi
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	ERC European Research Council, H2020	fi
jyx.fundingprogram	Akatemiahanke, SA	fi
jyx.fundingprogram	RIA Research and Innovation Action, H2020	fi
jyx.fundinginformation	This work was supported by the Academy of Finland, Projects No. 321840 (T. L.) and No. 1322507 (R. P.), and under the European Union’s Horizon 2020 research and innovation program by the European Research Council (ERC, Grant Agreements No. ERC-2015-CoG-681707 and No. ERC-2016-CoG-725369) 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.okm	A1