dc.contributor.author | Ducloue, Bertrand | |
dc.contributor.author | Lappi, Tuomas | |
dc.contributor.author | Zhu, Yan | |
dc.date.accessioned | 2017-07-03T10:11:39Z | |
dc.date.available | 2017-07-03T10:11:39Z | |
dc.date.issued | 2017 | |
dc.identifier.citation | Ducloue, B., Lappi, T., & Zhu, Y. (2017). Implementation of NLO high energy factorization in single inclusive forward hadron production. <i>Physical Review D</i>, <i>95</i>(11), Article 114007. <a href="https://doi.org/10.1103/PhysRevD.95.114007" target="_blank">https://doi.org/10.1103/PhysRevD.95.114007</a> | |
dc.identifier.other | CONVID_27061176 | |
dc.identifier.other | TUTKAID_74111 | |
dc.identifier.uri | https://jyx.jyu.fi/handle/123456789/54811 | |
dc.description.abstract | Single inclusive particle production cross sections in high energy hadron collisions at forward rapidity
are an important benchmark process for the Color Glass Condensate picture of small x QCD. Recent
calculations of this process have not led to a stable perturbative expansion for this quantity at high
transverse momenta. We consider the quark channel production cross section using the new rapidity
factorization procedure proposed by Iancu et al. We show that for fixed coupling one does indeed obtain a
physically meaningful cross section which is positive and reduces in a controlled way to previous leading
order calculations. We also consider a running coupling that depends on the transverse momentum of the
produced particle. This gives a stable result which, however, is not fully consistent with previous leading
order calculations that use a coordinate space running coupling. | |
dc.language.iso | eng | |
dc.publisher | American Physical Society | |
dc.relation.ispartofseries | Physical Review D | |
dc.subject.other | high energy physics | |
dc.subject.other | nuclear theory | |
dc.title | Implementation of NLO high energy factorization in single inclusive forward hadron production | |
dc.type | article | |
dc.identifier.urn | URN:NBN:fi:jyu-201706283123 | |
dc.contributor.laitos | Fysiikan laitos | fi |
dc.contributor.laitos | Department of Physics | en |
dc.contributor.oppiaine | Fysiikka | fi |
dc.contributor.oppiaine | Physics | en |
dc.type.uri | http://purl.org/eprint/type/JournalArticle | |
dc.date.updated | 2017-06-28T03:17:24Z | |
dc.type.coar | http://purl.org/coar/resource_type/c_2df8fbb1 | |
dc.description.reviewstatus | peerReviewed | |
dc.relation.issn | 2470-0010 | |
dc.relation.numberinseries | 11 | |
dc.relation.volume | 95 | |
dc.type.version | publishedVersion | |
dc.rights.copyright | © 2017 American Physical Society. Published in this repository with the kind permission of the publisher. | |
dc.rights.accesslevel | openAccess | fi |
dc.relation.grantnumber | 267321 | |
dc.relation.grantnumber | 681707 | |
dc.relation.grantnumber | 681707 | |
dc.relation.grantnumber | 303756 | |
dc.relation.projectid | info:eu-repo/grantAgreement/EC/H2020/681707/EU//CGCglasmaQGP | |
dc.subject.yso | fenomenologia | |
jyx.subject.uri | http://www.yso.fi/onto/yso/p2977 | |
dc.relation.doi | 10.1103/PhysRevD.95.114007 | |
dc.relation.funder | Suomen Akatemia | fi |
dc.relation.funder | Euroopan komissio | fi |
dc.relation.funder | Suomen Akatemia | fi |
dc.relation.funder | Research Council of Finland | en |
dc.relation.funder | European Commission | en |
dc.relation.funder | Research Council of Finland | en |
jyx.fundingprogram | Akatemiatutkija, SA | fi |
jyx.fundingprogram | ERC European Research Council, H2020 | fi |
jyx.fundingprogram | Akatemiatutkijan tutkimuskulut, SA | fi |
jyx.fundingprogram | Academy Research Fellow, AoF | en |
jyx.fundingprogram | ERC European Research Council, H2020 | en |
jyx.fundingprogram | Research costs of Academy Research Fellow, AoF | en |
jyx.fundinginformation | We thank E. Iancu and D. Zaslavsky for discussions and H. Mäntysaari for providing his BK solutions. This work has been supported by the Academy of Finland, Grants No. 267321, No. 273464 and No. 303756 and by the European Research Council, Grant No. ERC-2015-CoG681707. | |
dc.type.okm | A1 | |