Langmuir wave decay in turbulent inhomogeneous solar wind plasmas

Author(s):  
C. Krafft ◽  
A. Volokitin
Keyword(s):  
2015 ◽  
Vol 809 (2) ◽  
pp. 176 ◽  
Author(s):  
C. Krafft ◽  
A. S. Volokitin ◽  
V. V. Krasnoselskikh

1993 ◽  
Vol 41 (11-12) ◽  
pp. 823-832 ◽  
Author(s):  
Jerold P. Thiessen ◽  
Paul J. Kellogg
Keyword(s):  

1987 ◽  
Vol 92 (A6) ◽  
pp. 5865 ◽  
Author(s):  
H. C. Koons ◽  
J. L. Roeder ◽  
O. H. Bauer ◽  
G. Haerendel ◽  
R. Treumann ◽  
...  

2001 ◽  
Vol 18 (4) ◽  
pp. 355-360 ◽  
Author(s):  
A. J. Willes ◽  
Iver H. Cairns

AbstractBeam-driven Langmuir waves in the solar wind are generated just above the electron plasma frequency, which fluctuates in the inhomogeneous solar wind plasma. Consequently, propagating Langmuir waves encounter regions in which the wave frequency is less than the local plasma frequency, where they can be reflected, mode converted to transverse electromagnetic waves, and trapped in density wells. The aim here is to investigate Langmuir wave reflection and mode conversion at a linear density gradient for typical solar wind parameters. It is shown that higher mode conversion efficiencies are possible than previously calculated, but that mode conversion occurs in a smaller region of parameter space. In addition, the possibility of detecting mode conversion with in situ spacecraft Langmuir wave observations is discussed.


2010 ◽  
Author(s):  
A. Zaslavsky ◽  
A. S. Volokitin ◽  
V. V. Krasnoselskikh ◽  
M. Maksimovic ◽  
S. D. Bale ◽  
...  

1998 ◽  
Vol 11 (2) ◽  
pp. 851-856 ◽  
Author(s):  
W. M. Macek

AbstractThe question of the boundaries of the heliosphere is considered. The termination heliospheric shock should exist because the solar wind plasma flowing supersonically away from the Sun must make a transition to a subsonic flow. The heliopause is at the outermost extend of the solar wind. Beyond the heliopause lies the (very local) interstellar wind. Intensity of radio emissions at 2 to 3 kHz detected by the Voyager plasma wave instrument in the outer heliosphere can be explained provided that the electron beams generating Langmuir waves exist in the post-shock plasma due to secondary shocks in the compressed solar wind beyond the termination shock. The field strengths of Langmuir waves required to generate the second harmonic emissions are 50 – 100 μ V m-1. Alternatively, the emissions are generated in the vicinity of the heliopause. The Voyager 1 and 2 are proceeding toward a likely source region for Langmuir wave and these waves may be observed in situ in the near future.


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