On the maximum longitudinal electric field of a large amplitude electron plasma wave excited by a short electromagnetic radiation pulse (Articolo in rivista)

Type
Label
  • On the maximum longitudinal electric field of a large amplitude electron plasma wave excited by a short electromagnetic radiation pulse (Articolo in rivista) (literal)
Anno
  • 1993-01-01T00:00:00+01:00 (literal)
Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#doi
  • 10.1016/0375-9601(93)90156-T (literal)
Alternative label
  • S. Dalla, M. Lontano (1993)
    On the maximum longitudinal electric field of a large amplitude electron plasma wave excited by a short electromagnetic radiation pulse
    in Physics Letters A
    (literal)
Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#autori
  • S. Dalla, M. Lontano (literal)
Pagina inizio
  • 456 (literal)
Pagina fine
  • 461 (literal)
Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#url
  • http://www.sciencedirect.com/science/article/pii/037596019390156T# (literal)
Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#numeroVolume
  • 173 (literal)
Rivista
Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#numeroFascicolo
  • 6 (literal)
Note
  • ISI Web of Science (WOS) (literal)
Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#affiliazioni
  • Istituto di Fisica del Plasma, EURATOM-ENEA-CNR Association, Via Bassini 15, 20133 Milan, Italy (literal)
Titolo
  • On the maximum longitudinal electric field of a large amplitude electron plasma wave excited by a short electromagnetic radiation pulse (literal)
Abstract
  • The excitation of large amplitude plasma oscillations by the ponderomotive force exerted by a short electromagnetic (e.m.) radiation pulse on the electrons, is described within a one-dimensional, relativistic, cold plasma model. The quasistatic approximation, which assumes that the fluid variables follow adiabatically the temporal evolution of the field variables, is assumed to be valid. For a fixed rectangular profile of the e.m. wavepacket, travelling with group velocity upsilon(g) < c, the analytical solution of the problem is obtained. It is shown that, after the transit of the pulse, the coherent longitudinal electric field (travelling with phase velocity upsilon(phi)=upsilon(g)) can reach values higher than E(st)MAX=square-root 2 (m(e)comega(pe))/e)(gamma(phi)-1)1/2, where gamma(phi)=(1-upsilon(phi)2/c2)-1/2, up to E(MAX)= square-root 2 (m(e)comega(pe)/e)(gamma(phi)2upsilon(phi)/c)(3-upsilon(phi)2/c2 - square-root 5-2upsilon(phi)2/c2 + upsilon(phi)4/c4)1/2. However, this is only a transient dynamics which leads inevitably to the wavebreaking at a distance of approximately one wavelength from the beginning of the pulse. Actually, only for E < E(st)MAX stationary plasma oscillations can be sustained. (literal)
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