Magnetosonic wave instability by proton ring distributions: Simultaneous data and modeling

2013 ◽  
Vol 118 (7) ◽  
pp. 4053-4058 ◽  
Author(s):  
Fuliang Xiao ◽  
Qinghua Zhou ◽  
Zhaoguo He ◽  
Chang Yang ◽  
Yihua He ◽  
...  
2006 ◽  
Vol 73 (4) ◽  
pp. 320-324 ◽  
Author(s):  
M Salimullah ◽  
M I U Khan ◽  
M K Islam ◽  
M R Amin ◽  
P K Shukla

2010 ◽  
Vol 115 (A11) ◽  
pp. n/a-n/a ◽  
Author(s):  
Lunjin Chen ◽  
Richard M. Thorne ◽  
Vania K. Jordanova ◽  
Richard B. Horne

2018 ◽  
Vol 45 (19) ◽  
pp. 10,160-10,166 ◽  
Author(s):  
Zhigang Yuan ◽  
Zhihai Ouyang ◽  
Xiongdong Yu ◽  
Shiyong Huang ◽  
Fei Yao ◽  
...  

2011 ◽  
Vol 116 (A8) ◽  
pp. n/a-n/a ◽  
Author(s):  
M. F. Thomsen ◽  
M. H. Denton ◽  
V. K. Jordanova ◽  
L. Chen ◽  
R. M. Thorne

Author(s):  
Lunjin Chen ◽  
Richard M. Thorne ◽  
Vania K. Jordanova ◽  
Michelle F. Thomsen ◽  
Richard B. Horne

2016 ◽  
Vol 823 (2) ◽  
pp. 84 ◽  
Author(s):  
Tomohiro Ono ◽  
Takayuki Muto ◽  
Taku Takeuchi ◽  
Hideko Nomura

1987 ◽  
Vol 38 (3) ◽  
pp. 473-481 ◽  
Author(s):  
D. B. Melrose

A kinetic theory for nonlinear processes involving Langmuir waves, developed in an earlier paper, is extended through consideration of three aspects of the temporal evolution, (i) Following Falk & Tsytovich (1975). the dynamic equation for the rate of change of one amplitude at t is expressed as an integral over T of the product of two amplitudes at t – T and a kernel functionf(T); two generalizations of Falk & Tsytovich's form (f(T) ∝ T) that satisfy the requirement f(∞) = 0 are identified, (ii) It is shown that the low-frequency or beat disturbance may be described in terms of fluctuations in the electron number density, and that its time evolution involves an operator that is essentially the inverse of f(t). (iii) The transition from oscillatory evolution in the reactive or ‘coherent-wave’ version of the three-wave instability to the secular evolution of the resistive or ‘random-phase’ version is discussed qualitatively.


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