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dc.contributor.authorSchenke, B.
dc.contributor.authorSchlichting, S.
dc.contributor.authorSingh, P.
dc.date.accessioned2022-08-16T05:31:47Z
dc.date.available2022-08-16T05:31:47Z
dc.date.issued2022
dc.identifier.citationSchenke, B., Schlichting, S., & Singh, P. (2022). Rapidity dependence of initial state geometry and momentum correlations in p+Pb collisions. <i>Physical Review D</i>, <i>105</i>(9), Article 094023. <a href="https://doi.org/10.1103/PhysRevD.105.094023" target="_blank">https://doi.org/10.1103/PhysRevD.105.094023</a>
dc.identifier.otherCONVID_150893036
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/82560
dc.description.abstractEvent geometry and initial state correlations have been invoked as possible explanations of long-range azimuthal correlations observed in high-multiplicity p+p and p+Pb collisions. We study the rapidity dependence of initial state momentum correlations and event-by-event geometry in √s=5.02 TeV p+Pb collisions within the 3+1D IP-Glasma model [B. Schenke and S. Schlichting, Phys. Rev. C 94, 044907 (2016)], where the longitudinal structure is governed by Jalilian-Marian-Iancu-McLerran-Weigert-Leonidov-Kovner rapidity evolution of the incoming nuclear gluon distributions. We find that the event geometry is correlated across large rapidity intervals whereas initial state momentum correlations are relatively short-range in rapidity. Based on our results, we discuss implications for the relevance of both effects in explaining the origin of collective phenomena in small systems.en
dc.format.mimetypeapplication/pdf
dc.language.isoeng
dc.publisherAmerican Physical Society (APS)
dc.relation.ispartofseriesPhysical Review D
dc.rightsIn Copyright
dc.titleRapidity dependence of initial state geometry and momentum correlations in p+Pb collisions
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-202208164104
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.issn2470-0010
dc.relation.numberinseries9
dc.relation.volume105
dc.type.versionpublishedVersion
dc.rights.copyright© 2022 American Physical Society
dc.rights.accesslevelopenAccessfi
dc.relation.grantnumber321840
dc.relation.grantnumber824093
dc.relation.grantnumber824093
dc.relation.projectidinfo:eu-repo/grantAgreement/EC/H2020/824093/EU//STRONG-2020
dc.subject.ysokvarkki-gluoniplasma
dc.subject.ysohiukkasfysiikka
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p38826
jyx.subject.urihttp://www.yso.fi/onto/yso/p15576
dc.rights.urlhttp://rightsstatements.org/page/InC/1.0/?language=en
dc.relation.doi10.1103/PhysRevD.105.094023
dc.relation.funderResearch Council of Finlanden
dc.relation.funderEuropean Commissionen
dc.relation.funderSuomen Akatemiafi
dc.relation.funderEuroopan komissiofi
jyx.fundingprogramAcademy Project, AoFen
jyx.fundingprogramRIA Research and Innovation Action, H2020en
jyx.fundingprogramAkatemiahanke, SAfi
jyx.fundingprogramRIA Research and Innovation Action, H2020fi
jyx.fundinginformationS. S. and P. S. are supported by the Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) through the CRC-TR 211 “Strong Interaction Matter under Extreme Conditions”—Project No. 315477589–TRR 211. P. S. is also supported by the Academy of Finland under Project No. 321840 and under the European Union’s Horizon 2020 research and innovation program by the STRONG-2020 project (Grant Agreement No. 824093). B. S. is supported by the U.S. Department of Energy, Office of Science, Office of Nuclear Physics, under Contract No. DE-SC0012704. This research used the resources of the National Energy Research Scientific Computing Center, a DOE Office of Science User Facility supported by the Office of Science of the U.S. Department of Energy under Contract No. DE-AC02-05CH11231.
dc.type.okmA1


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