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dc.contributor.authorBoguslavski, Kirill
dc.contributor.authorKurkela, Aleksi
dc.contributor.authorLappi, Tuomas
dc.contributor.authorPeuron, Jarkko
dc.date.accessioned2020-09-18T07:56:17Z
dc.date.available2020-09-18T07:56:17Z
dc.date.issued2020
dc.identifier.citationBoguslavski, K., Kurkela, A., Lappi, T., & Peuron, J. (2020). Heavy quark diffusion in an overoccupied gluon plasma. <i>Journal of High Energy Physics</i>, <i>2020</i>(9), Article 77. <a href="https://doi.org/10.1007/jhep09(2020)077" target="_blank">https://doi.org/10.1007/jhep09(2020)077</a>
dc.identifier.otherCONVID_42071377
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/71805
dc.description.abstractWe extract the heavy-quark diffusion coefficient κ and the resulting momentum broadening 〈p2〉 in a far-from-equilibrium non-Abelian plasma. We find several features in the time dependence of the momentum broadening: a short initial rapid growth of 〈p2〉, followed by linear growth with time due to Langevin-type dynamics and damped oscillations around this growth at the plasmon frequency. We show that these novel oscillations are not easily explained using perturbative techniques but result from an excess of gluons at low momenta. These oscillation are therefore a gauge invariant confirmation of the infrared enhancement we had previously observed in gauge-fixed correlation functions. We argue that the kinetic theory description of such systems becomes less reliable in the presence of this IR enhancement.en
dc.format.mimetypeapplication/pdf
dc.languageeng
dc.language.isoeng
dc.publisherSpringer
dc.relation.ispartofseriesJournal of High Energy Physics
dc.rightsCC BY 4.0
dc.subject.otherLattice QCD
dc.subject.otherQuark-Gluon Plasma
dc.subject.otherHeavy Quark Physics
dc.titleHeavy quark diffusion in an overoccupied gluon plasma
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-202009185891
dc.contributor.laitosFysiikan laitosfi
dc.contributor.laitosDepartment of Physicsen
dc.contributor.oppiaineFysiikkafi
dc.contributor.oppiainePhysicsen
dc.type.urihttp://purl.org/eprint/type/JournalArticle
dc.type.coarhttp://purl.org/coar/resource_type/c_2df8fbb1
dc.description.reviewstatuspeerReviewed
dc.relation.issn1126-6708
dc.relation.numberinseries9
dc.relation.volume2020
dc.type.versionpublishedVersion
dc.rights.copyright© The Authors. Article funded by SCOAP3
dc.rights.accesslevelopenAccessfi
dc.relation.grantnumber681707
dc.relation.grantnumber681707
dc.relation.grantnumber321840
dc.relation.projectidinfo:eu-repo/grantAgreement/EC/H2020/681707/EU//CGCglasmaQGP
dc.subject.ysohiukkasfysiikka
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p15576
dc.rights.urlhttps://creativecommons.org/licenses/by/4.0/
dc.relation.doi10.1007/jhep09(2020)077
dc.relation.funderEuropean Commissionen
dc.relation.funderResearch Council of Finlanden
dc.relation.funderEuroopan komissiofi
dc.relation.funderSuomen Akatemiafi
jyx.fundingprogramERC European Research Council, H2020en
jyx.fundingprogramAcademy Project, AoFen
jyx.fundingprogramERC European Research Council, H2020fi
jyx.fundingprogramAkatemiahanke, SAfi
jyx.fundinginformationT. L. is supported by the Academy of Finland, project No. 321840.This work is supported by the European Research Council, grant ERC-2015-CoG-681707.
dc.type.okmA1


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