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dc.contributor.authorMace, Mark
dc.contributor.authorMueller, Niklas
dc.contributor.authorSchlichting, Soeren
dc.contributor.authorSharma, Sayantan
dc.date.accessioned2020-06-12T06:23:21Z
dc.date.available2020-06-12T06:23:21Z
dc.date.issued2020
dc.identifier.citationMace, M., Mueller, N., Schlichting, S., & Sharma, S. (2020). Chiral Instabilities and the Onset of Chiral Turbulence in QED Plasmas. <i>Physical Review Letters</i>, <i>124</i>(19), Article 191604. <a href="https://doi.org/10.1103/PhysRevLett.124.191604" target="_blank">https://doi.org/10.1103/PhysRevLett.124.191604</a>
dc.identifier.otherCONVID_35900978
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/69894
dc.description.abstractWe present a first principles study of chiral plasma instabilities and the onset of chiral turbulence in QED plasmas with strong gauge matter interaction (e2Nf=64), far from equilibrium. By performing classical-statistical lattice simulations of the microscopic theory, we show that the generation of strong helical magnetic fields from a helicity imbalance in the fermion sector proceeds via three distinct phases. During the initial linear instability regime the helicity imbalance of the fermion sector causes an exponential growth (damping) of magnetic field modes with right- (left-) handed polarization, for which we extract the characteristic growth (damping) rates. Secondary growth of unstable modes accelerates the helicity transfer from fermions to gauge fields and ultimately leads to the emergence of a self-similar scaling regime characteristic of a decaying turbulence, where magnetic helicity is efficiently transferred to macroscopic length scales. Within this turbulent regime, the evolution of magnetic helicity spectrum can be described by an infrared power spectrum with spectral exponent κ=10.2±0.5 and dynamical scaling exponents α=1.14±0.50 and β=0.37±0.13.en
dc.format.mimetypeapplication/pdf
dc.languageeng
dc.language.isoeng
dc.publisherAmerican Physical Society
dc.relation.ispartofseriesPhysical Review Letters
dc.rightsCC BY 4.0
dc.subject.otherlattice field theory
dc.subject.otherplasma instabilitiles
dc.titleChiral Instabilities and the Onset of Chiral Turbulence in QED Plasmas
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-202006124139
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.issn0031-9007
dc.relation.numberinseries19
dc.relation.volume124
dc.type.versionpublishedVersion
dc.rights.copyright© Authors, 2020
dc.rights.accesslevelopenAccessfi
dc.relation.grantnumber681707
dc.relation.grantnumber681707
dc.relation.projectidinfo:eu-repo/grantAgreement/EC/H2020/681707/EU//CGCglasmaQGP
dc.subject.ysokvanttikenttäteoria
dc.subject.ysohiukkasfysiikka
dc.subject.ysoplasma (kaasut)
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p27496
jyx.subject.urihttp://www.yso.fi/onto/yso/p15576
jyx.subject.urihttp://www.yso.fi/onto/yso/p238
dc.rights.urlhttps://creativecommons.org/licenses/by/4.0/
dc.relation.doi10.1103/PhysRevLett.124.191604
dc.relation.funderEuropean Commissionen
dc.relation.funderEuroopan komissiofi
jyx.fundingprogramERC European Research Council, H2020en
jyx.fundingprogramERC European Research Council, H2020fi
jyx.fundinginformationM. M. was supported by the EuropeanResearch Council Grant No. ERC-2015-CoG-681707.
dc.type.okmA1


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