Second-harmonic ion cyclotron resonance heating scenarios of Aditya tokamak plasma

Pramana ◽  
2015 ◽  
Vol 85 (4) ◽  
pp. 713-721 ◽  
Author(s):  
ASIM KUMAR CHATTOPADHYAY ◽  
◽  
S V KULKARNI ◽  
R SRINIVASAN
2000 ◽  
Vol 7 (5) ◽  
pp. 1467-1478 ◽  
Author(s):  
S. C. Jun ◽  
Kaya Imre ◽  
D. C. Stevens ◽  
Harold Weitzner ◽  
C. S. Chang

1991 ◽  
Vol 31 (9) ◽  
pp. 1770-1774 ◽  
Author(s):  
R. Van Nieuwenhove ◽  
R. Koch ◽  
G. Van Oost ◽  
T. Delvigne ◽  
F. Durodie ◽  
...  

1997 ◽  
Vol 36 (Part 1, No. 1A) ◽  
pp. 345-349 ◽  
Author(s):  
Mikio Saigusa ◽  
Sinichi Moriyama ◽  
Haruyuki Kimura ◽  
Kiyotaka Hamamatsu ◽  
Tsuneyuki Fujii ◽  
...  

2021 ◽  
Vol 87 (6) ◽  
Author(s):  
V. Maquet ◽  
A. Druart ◽  
A. Messiaen

In the ion cyclotron range of frequency (ICRF), the presence of a lower hybrid (LH) resonance can appear in the edge of a tokamak plasma and lead to deleterious edge power depositions. An analytic formula for these losses is derived in the cold plasma approximation and for a slab geometry using an asymptotic approach and an analytical continuation near the LH resonance. The way to minimize these losses in a large machine like ITER is discussed. An internal verification between the power loss computed with the semi-analytical code ANTITER IV for ion cyclotron resonance heating (ICRH) and the analytic result is performed. This allows us to check the precision of the numerical integration of the singular set of cold plasma wave differential equations. The set of cold plasma equations used is general and can be applied in other parameters domain.


1987 ◽  
Vol 58 (2) ◽  
pp. 124-127 ◽  
Author(s):  
K. Steinmetz ◽  
J. -M. Noterdaeme ◽  
F. Wagner ◽  
F. Wesner ◽  
J. Bäumler ◽  
...  

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