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Spectral function for overoccupied gluodynamics from classical lattice simulations

dc.contributor.authorBoguslavski, Kirill
dc.contributor.authorKurkela, Aleksi
dc.contributor.authorLappi, Tuomas
dc.contributor.authorPeuron, Jarkko
dc.date.accessioned2019-08-23T11:37:54Z
dc.date.available2019-08-23T11:37:54Z
dc.date.issued2019
dc.identifier.citationBoguslavski, K., Kurkela, A., Lappi, T., & Peuron, J. (2019). Spectral function for overoccupied gluodynamics from classical lattice simulations. <i>Acta Physica Polonica B</i>, <i>50</i>(6), 1105-1116. <a href="https://doi.org/10.5506/APhysPolB.50.1105" target="_blank">https://doi.org/10.5506/APhysPolB.50.1105</a>
dc.identifier.otherCONVID_32425331
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/65289
dc.description.abstractWe study the spectral properties of an overoccupied gluonic system far from equilibrium. Using classical Yang–Mills simulations and linear response theory, we determine the statistical and spectral functions. We measure dispersion relations and damping rates of transversally and longitudinally polarized excitations in the gluonic plasma, and also study further structures in the spectral function.en
dc.format.mimetypeapplication/pdf
dc.languageeng
dc.language.isoeng
dc.publisherJagellonian University
dc.relation.ispartofseriesActa Physica Polonica B
dc.rightsCC BY-SA 4.0
dc.subject.otherdamping rate
dc.subject.otherdispersion relations
dc.subject.othergluonic systems
dc.subject.otherlattice simulation
dc.subject.otherlinear-response theory
dc.subject.otherpolarized excitation
dc.subject.otherspectral function
dc.subject.otherspectral properties
dc.titleSpectral function for overoccupied gluodynamics from classical lattice simulations
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-201908233890
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.format.pagerange1105-1116
dc.relation.issn0587-4254
dc.relation.numberinseries6
dc.relation.volume50
dc.type.versionpublishedVersion
dc.rights.copyright© The Authors, 2019
dc.rights.accesslevelopenAccessfi
dc.relation.grantnumber303756
dc.relation.grantnumber267321
dc.subject.ysohiukkasfysiikka
dc.subject.ysokvanttikenttäteoria
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p15576
jyx.subject.urihttp://www.yso.fi/onto/yso/p27496
dc.rights.urlhttps://creativecommons.org/licenses/by-sa/4.0/
dc.relation.doi10.5506/APhysPolB.50.1105
dc.relation.funderSuomen Akatemiafi
dc.relation.funderSuomen Akatemiafi
dc.relation.funderResearch Council of Finlanden
dc.relation.funderResearch Council of Finlanden
jyx.fundingprogramAkatemiatutkijan tutkimuskulut, SAfi
jyx.fundingprogramAkatemiatutkija, SAfi
jyx.fundingprogramResearch costs of Academy Research Fellow, AoFen
jyx.fundingprogramAcademy Research Fellow, AoFen
jyx.fundinginformationThis work is supported by the European Research Council, grant ERC-2015-CoG-681707. T.L. has been supported by the Academy of Finland, projects No. 267321 and No. 303756. J.P. has been supported by the Jenny and Antti Wihuri Foundation and a travel grant from the Magnus Ehrnrooth foundation. K.B. and J.P. would like to thank the CERN Theory group for hospitality during part of this work. We acknowledge computational resources from CSC — IT Center for Science, Finland.
dc.type.okmA1


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