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dc.contributor.authorBerges, Jürgen
dc.contributor.authorBoguslavski, Kirill
dc.contributor.authorMace, Mark
dc.contributor.authorPawlowski, Jan M.
dc.date.accessioned2020-09-08T09:50:45Z
dc.date.available2020-09-08T09:50:45Z
dc.date.issued2020
dc.identifier.citationBerges, J., Boguslavski, K., Mace, M., & Pawlowski, J. M. (2020). Gauge-invariant condensation in the nonequilibrium quark-gluon plasma. <i>Physical Review D</i>, <i>102</i>(3), Article 034014. <a href="https://doi.org/10.1103/PhysRevD.102.034014" target="_blank">https://doi.org/10.1103/PhysRevD.102.034014</a>
dc.identifier.otherCONVID_41922557
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/71687
dc.description.abstractThe large density of gluons, which is present shortly after a nuclear collision at very high energies, can lead to the formation of a condensate. We identify a gauge-invariant order parameter for condensation based on elementary nonperturbative excitations of the plasma, which are described by spatial Wilson loops. Using real-time lattice simulations, we demonstrate that a self-similar transport process towards low momenta builds up a macroscopic zero mode. Our findings reveal intriguing similarities to recent discoveries of condensation phenomena out of equilibrium in table-top experiments with ultracold Bose gases.en
dc.format.mimetypeapplication/pdf
dc.languageeng
dc.language.isoeng
dc.publisherAmerican Physical Society (APS)
dc.relation.ispartofseriesPhysical Review D
dc.rightsCC BY 4.0
dc.titleGauge-invariant condensation in the nonequilibrium quark-gluon plasma
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-202009085795
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.numberinseries3
dc.relation.volume102
dc.type.versionpublishedVersion
dc.rights.copyright© 2020 the Authors
dc.rights.accesslevelopenAccessfi
dc.relation.grantnumber681707
dc.relation.grantnumber681707
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.doi10.1103/PhysRevD.102.034014
dc.relation.funderEuropean Commissionen
dc.relation.funderEuroopan komissiofi
jyx.fundingprogramERC European Research Council, H2020en
jyx.fundingprogramERC European Research Council, H2020fi
jyx.fundinginformationThe work is supported by EMMI, the BMBF Grant No. 05P18VHFCA and is part of and supported by the DFG Collaborative Research Centre SFB 1225 (ISOQUANT) as well as by the DFG under Germany’s Excellence Strategy EXC–2181/1–390900948 (the Heidelberg Excellence Cluster STRUCTURES). M. M. is supported by the European Research Council, Grant No. ERC-2015-CoG-681707. This research used resources of the National Energy Research Scientific Computing Center (NERSC), a U.S. Department of Energy Office of Science User Facility operated under Contract No. DE-AC02-05CH11231. The computational results presented have been achieved in part using the Vienna Scientific Cluster (VSC).
dc.type.okmA1


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