Abstract
The propagation and absorption of an electromagnetic wave, near the electron cyclotron zone, of a cold plasma (T{sub e} {approx} 1-5 eV) confined in a flaring magnetic field is studied. The case of both extraordinary and ordinary modes has been considered. Temperature effects and electron-neutral collisions have been taken account in the dielectric tensor.
Meis, C;
Compant La Fontaine, A;
Louvet, P;
[1]
Meyer, R L
[2]
- CEA Centre d`Etudes de Saclay, 91 - Gif-sur-Yvette (France). Direction du Cycle du Combustible
- Nancy-1 Univ., 54 (France)
Citation Formats
Meis, C, Compant La Fontaine, A, Louvet, P, and Meyer, R L.
ECR plasma source in a flaring magnetic field.
France: N. p.,
1992.
Web.
Meis, C, Compant La Fontaine, A, Louvet, P, & Meyer, R L.
ECR plasma source in a flaring magnetic field.
France.
Meis, C, Compant La Fontaine, A, Louvet, P, and Meyer, R L.
1992.
"ECR plasma source in a flaring magnetic field."
France.
@misc{etde_10127678,
title = {ECR plasma source in a flaring magnetic field}
author = {Meis, C, Compant La Fontaine, A, Louvet, P, and Meyer, R L}
abstractNote = {The propagation and absorption of an electromagnetic wave, near the electron cyclotron zone, of a cold plasma (T{sub e} {approx} 1-5 eV) confined in a flaring magnetic field is studied. The case of both extraordinary and ordinary modes has been considered. Temperature effects and electron-neutral collisions have been taken account in the dielectric tensor.}
place = {France}
year = {1992}
month = {Dec}
}
title = {ECR plasma source in a flaring magnetic field}
author = {Meis, C, Compant La Fontaine, A, Louvet, P, and Meyer, R L}
abstractNote = {The propagation and absorption of an electromagnetic wave, near the electron cyclotron zone, of a cold plasma (T{sub e} {approx} 1-5 eV) confined in a flaring magnetic field is studied. The case of both extraordinary and ordinary modes has been considered. Temperature effects and electron-neutral collisions have been taken account in the dielectric tensor.}
place = {France}
year = {1992}
month = {Dec}
}