Electron heating by mode-converted ion-Bernstein waves in ICRF heating of tokamak plasmas

1987 ◽  
Author(s):  
A. K. Ram ◽  
A. Bers
1982 ◽  
Vol 20 (4) ◽  
pp. 1273-1278 ◽  
Author(s):  
D. Q. Hwang ◽  
G. Grotz ◽  
J. C. Hosea

2001 ◽  
Vol 41 (8) ◽  
pp. 1021-1035 ◽  
Author(s):  
K. Saito ◽  
R. Kumazawa ◽  
T. Mutoh ◽  
T. Seki ◽  
T. Watari ◽  
...  

2012 ◽  
Vol 52 (8) ◽  
pp. 082003 ◽  
Author(s):  
X.J. Zhang ◽  
Y.P. Zhao ◽  
B.N. Wan ◽  
X.Z. Gong ◽  
Y. Lin ◽  
...  

1992 ◽  
Vol 48 (3) ◽  
pp. 465-476
Author(s):  
Masao Sugawa

When Bernstein waves (B waves) are excited in a magnetized plasma, their self-interaction by nonlinear Landau damping (NLD) becomes the dominant mechanism for the electron heating of the bulk plasma. We examine this behaviour numerically. This occurs only for B waves with relatively small k∥ because the damping of the B waves becomes very small. This occurs in the relatively broad B-wave frequency range betweenω/ωc = 1.45 and 1.78. For B waves with large k∥ (k∥R > 0.15), virtual waves are not generated via self-interaction due to NLD because the quasi-linear cyclotron damping of the B waves becomes the dominant mechanism. The numerical results agree well with experimental ones.


1992 ◽  
Vol 32 (3) ◽  
pp. 465-479 ◽  
Author(s):  
M Brambilla ◽  
A Cardinali

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