1992
DOI: 10.1017/s0022377800016639
|View full text |Cite
|
Sign up to set email alerts
|

Second-order oscillations of a Vlasov–Poisson plasma in Fourier-transformed velocity space

Abstract: We study the Vlasov–Poisson system of equations in Fourier-transformed velocity space. First we reformulate some results of the linear theory: in the new representation the van Kampen–Case eigenmodes are found to be ordinary functions with convenient continuity properties. We give a transparent derivation of the free-streaming temporal echo in terms of the kinematics of wave packets in Fourier-transformed velocity space. We further extend this analysis to include Coulomb interactions, which allows us to establ… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

0
9
0

Year Published

1994
1994
2020
2020

Publication Types

Select...
7

Relationship

0
7

Authors

Journals

citations
Cited by 16 publications
(9 citation statements)
references
References 21 publications
0
9
0
Order By: Relevance
“…The frequencies (I) and (II) have already been identified in our preliminary work on this subject [4], but not the frequency (III). We emphasize that all the three type of frequencies are listed in [13], which makes our analysis coherent with the physics litterature. To conclude this presentation, we are going to state a precise theorem giving the asymptotic behavior of the solutions of (VPL2).…”
Section: (Vpl)mentioning
confidence: 53%
See 2 more Smart Citations
“…The frequencies (I) and (II) have already been identified in our preliminary work on this subject [4], but not the frequency (III). We emphasize that all the three type of frequencies are listed in [13], which makes our analysis coherent with the physics litterature. To conclude this presentation, we are going to state a precise theorem giving the asymptotic behavior of the solutions of (VPL2).…”
Section: (Vpl)mentioning
confidence: 53%
“…By construction of g through Duhamel formula (20), g is obviously a continuous function on R + × T d × R d and C 1 on R * + × T d × R d . Furthermore, we may verify by a straightforward calculation that g is solution of the Vlasov equation (13). Consequently, we just have to prove that g, u is solution of Poisson equation (18).…”
Section: (Vplg)mentioning
confidence: 97%
See 1 more Smart Citation
“…(9) and (11) be attenuated in time?" Our interpretation of this apparent paradox is that the root of the dispersion function which lies in the lower half of its unphysical Riemann sheet has no associated eigenfunction; the damped oscillation related to this root is rather similar to the "virtual modes" found in Landau damping (Sedláček & Nocera 1992), in inhomogeneous plasmas (Sedláček 1971(Sedláček , 1994 and in the inhomogeneous vibrating string (Sedláček et al 1986): they can be aptly named "random virtual modes".…”
Section: Discussionmentioning
confidence: 87%
“…In our recent papers [1,2,3,4,5] we drew attention to an alternative approach to the problem of Vlasov plasma oscillations which is based on the Fourier transformed velocity space.…”
Section: Introductionmentioning
confidence: 99%