Ion Acoustic Wave Dispersion in a Highly Ionized Argon Plasma in a Magnetic Field

1968 ◽  
Vol 11 (10) ◽  
pp. 2251 ◽  
Author(s):  
Richard R. Levin
Keyword(s):  
Magnetic Field ◽  
Acoustic Wave ◽  
Argon Plasma ◽  
Wave Dispersion ◽  
Ion Acoustic Wave ◽  
Ion Acoustic

Effect of magnetic field on propagation of nonlinear ion-acoustic wave

1976 ◽  
Vol 19 (5) ◽  
pp. 762 ◽  
Author(s):  
S. G. Tagare ◽  
A. S. Sharma
Keyword(s):  
Magnetic Field ◽  
Acoustic Wave ◽  
Ion Acoustic Wave ◽  
Ion Acoustic

Nonlinear ion acoustic wave in a pair-ion plasma in a uniform weak magnetic field

2015 ◽  
Vol 90 (4) ◽  
pp. 045604 ◽  
Author(s):  
Biplab Maity ◽  
Samiran Ghosh ◽  
R Bharuthram
Keyword(s):  
Magnetic Field ◽  
Acoustic Wave ◽  
Weak Magnetic Field ◽  
Ion Acoustic Wave ◽  
Ion Plasma ◽  
Ion Acoustic

Experimental determination of ion acoustic wave dispersion relation with interferometric analysis

2021 ◽  
Author(s):  
Daniel Vech ◽  
David M. Malaspina ◽  
Cynthia Cattell ◽  
Steven J. Schwartz ◽  
Robert E. Ergun ◽  
...  
Keyword(s):  
Dispersion Relation ◽  
Acoustic Wave ◽  
Experimental Determination ◽  
Wave Dispersion ◽  
Ion Acoustic Wave ◽  
Ion Acoustic

Excitation of an ion-acoustic wave by two whistlers in a collisionless magnetoplasma

1981 ◽  
Vol 25 (2) ◽  
pp. 255-265 ◽  
Author(s):  
M. S. Sodha ◽  
Tarsem Singh ◽  
D. P. Singh ◽  
R. P. Sharma
Keyword(s):  
Magnetic Field ◽  
Acoustic Wave ◽  
Static Magnetic Field ◽  
Ponderomotive Force ◽  
Wave Power ◽  
Ion Acoustic Wave ◽  
Ion Density ◽  
Ion Acoustic

This paper presents an investigation of the excitation of an ion-acoustic wave in a collisionless hot magnetoplasma by two whistlers. On account of the interaction of the two whistlers, of frequencies ω1 and ω2, ponderomotive force at frequency △ ω(= ω1 – ω2) leads to the generation of an ion-acoustic wave. When the two whistlers have initially Gaussian intensity distributions, a d.c. component of the ponderomotive force leads to the redistribution of the background electron/ion density, and cross-focusing of the whistlers occurs. The power of the generated ion-acoustic wave, being dependent on the background ion density and powers of the whistlers, is further modified. The ion-acoustic wave power also changes drastically with the strength of the static magnetic field.

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