Effect of nonlinear circularly polarized waves on linear instabilities triggered by an alpha particle beam
Author
dc.contributor.author
Gomberoff, L.
Admission date
dc.date.accessioned
2019-01-29T15:34:30Z
Available date
dc.date.available
2019-01-29T15:34:30Z
Publication date
dc.date.issued
2006
Cita de ítem
dc.identifier.citation
Journal of Geophysical Research: Space Physics, Volumen 111, Issue 2, 2018,
Identifier
dc.identifier.issn
21699402
Identifier
dc.identifier.other
10.1029/2005JA011407
Identifier
dc.identifier.uri
https://repositorio.uchile.cl/handle/2250/161655
Abstract
dc.description.abstract
It is shown that nonlinear left-hand polarized waves can either stabilize or destabilize linear right-hand polarized instabilities triggered by an alpha particle beam in a magnetized electron proton plasma. For differential alpha particle speeds above the threshold for instability the destabilization depends upon the plasma βi = vth.i/vA, where vth.i is the thermal velocity of the i plasma component and v A is the Alfvén velocity. For any given finite-amplitude wave frequency, there is always a βi value such that above this value the system is destabilized further. For drift alpha particle speeds well above the instability threshold the destabilization can occur for any βi. It is also shown that the presence of the large-amplitude wave can trigger purely electrostatic ion-acoustic instabilities. The unstable waves are supported by the proton core. Copyright 2006 by the American Geophysical Union.