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a bibo:Issue;
dcterms:medium ;
rdau:P60049 ;
rdau:P60050 ;
rdau:P60048 ;
dc:identifier "(DE-101)1329070658";
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a bibo:Article;
dc:title "Momentum Space Diffusion from Spatially Amplified Waves in a Plasma in a Magnetic Field";
dcterms:creator _:node1jrarau8gx93557811 .
_:node1jrarau8gx93557811 gndo:preferredName "Lehmann, H. ‐R." .
marcRole:aut _:node1jrarau8gx93557812 .
_:node1jrarau8gx93557812 gndo:preferredName "Lehmann, H. ‐R." .
marcRole:aut _:node1jrarau8gx93557813 .
_:node1jrarau8gx93557813 gndo:preferredName "Treumann, R." .
bibo:pageStart "211";
bibo:pageEnd "225";
dcterms:extent "15 S.";
dcterms:isPartOf ;
dcterms:description "Abstract: Quasilinear equations for relativistic plasmas in external magnetic fields are derived for the case of spatially growing wave turbulence. This generalizes the well‐known quasilinear approach to an amplifying relativistic plasma. The equations can be cast in condensed momentum‐space diffusive form. The diffusion tensor is given. As a result an inhomogeneity is produced in the space charge distribution giving rise to the development of a second‐order field‐aligned dc electric field. A general formula for the electrostatic potential is presented, which is specialised to the case of ion‐cyclotron turbulence. Here the field points out of the interaction region."@de;
dcterms:license ;
wdrs:describedby .
dcterms:license ;
dcterms:modified "2024-05-13T18:32:07.000"^^xsd:dateTime .
dcterms:issued "2006";
bibo:issue "16.2006, 3";
owl:sameAs .