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dc.creatorTrifković, Zoran
dc.creatorOsmokrović, Predrag
dc.date.accessioned2022-09-19T16:14:30Z
dc.date.available2022-09-19T16:14:30Z
dc.date.issued2009
dc.identifier.issn1051-9998
dc.identifier.urihttps://machinery.mas.bg.ac.rs/handle/123456789/869
dc.description.abstractA linearly polarized electromagnetic source wave splits into six traveling wave modes (three of them are right-hand circularly-polarized (RCP) modes and three are left-hand circularly-polarized (LCP) modes) due to the interaction with a suddenly created magnetoplasma medium. When the angular frequency of the source wave is in the low-frequency region, the magnetoplasma supports two whistler wave modes (one is the transmitted RCP and the other is the reflected LCP). It is shown that the efficiency of energy conversion of the LCP whistler wave mode into the magnetic field of the wiggler is nearly of the same order of magnitude as the efficiency of the previously considered energy conversion of the RCP whistler wave mode.en
dc.relationinfo:eu-repo/grantAgreement/MESTD/MPN2006-2010/141046/RS//
dc.rightsrestrictedAccess
dc.sourcePlasma Devices and Operations
dc.subjectWiggler waveen
dc.subjectWhistler waveen
dc.subjectSource waveen
dc.subjectRefractive indexen
dc.subjectMagnetoplasmaen
dc.titleConversion of a left-hand circularly polarized whistler wave into the magnetic energy of a controllable helical wiggler waveen
dc.typearticle
dc.rights.licenseARR
dc.citation.epage220
dc.citation.issue3
dc.citation.other17(3): 215-220
dc.citation.rankM23
dc.citation.spage215
dc.citation.volume17
dc.identifier.doi10.1080/10519990902957955
dc.identifier.scopus2-s2.0-70349542851
dc.identifier.wos000267193700006
dc.type.versionpublishedVersion


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