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dc.contributor.authorGuerrero-Rodríguez, Pablo
dc.contributor.authorLappi, Tuomas
dc.date.accessioned2021-07-20T07:22:35Z
dc.date.available2021-07-20T07:22:35Z
dc.date.issued2021
dc.identifier.citationGuerrero-Rodríguez, P., & Lappi, T. (2021). Evolution of initial stage fluctuations in the glasma. <i>Physical Review D</i>, <i>104</i>(1), Article 014011. <a href="https://doi.org/10.1103/physrevd.104.014011" target="_blank">https://doi.org/10.1103/physrevd.104.014011</a>
dc.identifier.otherCONVID_99050141
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/77191
dc.description.abstractWe perform a calculation of the one- and two-point correlation functions of energy density and axial charge deposited in the glasma in the initial stage of a heavy ion collision at finite proper time. We do this by describing the initial stage of heavy ion collisions in terms of freely evolving classical fields whose dynamics obey the linearized Yang-Mills equations. Our approach allows us to systematically resum the contributions of high momentum modes that would make a power series expansion in proper time divergent. We evaluate the field correlators in the McLerran-Venugopalan model using the glasma graph approximation, but our approach for the time dependence can be applied to a general four-point function of the initial color fields. Our results provide analytical insight into the preequilibrium phase of heavy ion collisions without requiring a numerical solution to the Yang-Mills equations.en
dc.format.mimetypeapplication/pdf
dc.language.isoeng
dc.publisherAmerican Physical Society
dc.relation.ispartofseriesPhysical Review D
dc.rightsCC BY 4.0
dc.subject.otherquark-gluon plasma
dc.subject.otherrelativistic heavy-ion collisions
dc.subject.othernuclear physics
dc.titleEvolution of initial stage fluctuations in the glasma
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-202107204365
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.numberinseries1
dc.relation.volume104
dc.type.versionpublishedVersion
dc.rights.copyright© Authors, 2021
dc.rights.accesslevelopenAccessfi
dc.relation.grantnumber824093
dc.relation.grantnumber824093
dc.relation.grantnumber321840
dc.relation.grantnumber681707
dc.relation.grantnumber681707
dc.relation.projectidinfo:eu-repo/grantAgreement/EC/H2020/824093/EU//STRONG-2020
dc.relation.projectidinfo:eu-repo/grantAgreement/EC/H2020/681707/EU//CGCglasmaQGP
dc.subject.ysokvarkki-gluoniplasma
dc.subject.ysoydinfysiikka
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p38826
jyx.subject.urihttp://www.yso.fi/onto/yso/p14759
dc.rights.urlhttps://creativecommons.org/licenses/by/4.0/
dc.relation.doi10.1103/physrevd.104.014011
dc.relation.funderEuropean Commissionen
dc.relation.funderResearch Council of Finlanden
dc.relation.funderEuropean Commissionen
dc.relation.funderEuroopan komissiofi
dc.relation.funderSuomen Akatemiafi
dc.relation.funderEuroopan komissiofi
jyx.fundingprogramRIA Research and Innovation Action, H2020en
jyx.fundingprogramAcademy Project, AoFen
jyx.fundingprogramERC European Research Council, H2020en
jyx.fundingprogramRIA Research and Innovation Action, H2020fi
jyx.fundingprogramAkatemiahanke, SAfi
jyx.fundingprogramERC European Research Council, H2020fi
jyx.fundinginformationThis work was supported by the Academy of Finland, Project No. 321840 and under the European Union’s Horizon 2020 research and innovation programme by the European Research Council (ERC, Grant No. ERC-2015-CoG-681707) and by the H2020 Research InfrastructuresSTRONG-2020 project (Grant No. 824093). The content of this paper 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.okmA1


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