Most present Ion Cyclotron Resonant Frequency (ICRF) heating codes and antenna codes assume the antenna sitting in a vacuum region and consider the fast wave only, which implicitly performs an abrupt density transition from vacuum to above lower hybrid (LH) resonance. We studied the impact of densities that decay continuously inside the antenna box on near field patterns and power coupling. A new full wave code based on the COMSOL Finite Element Solver has been developed to investigate this topic. It is shown that: up to the memory limits of the adopted workstation, the local RF field pattern in low-density regions below the LH resonance changes with the grid size. Interestingly and importantly, however, the total coupled spectrum is independent to the mesh size and is weakly affected by the presence of the density profile inside the antenna box in dipole phasing. Thus one can drop out this density for coupling studies. Simulation also shows that varying the density gradient in the fast wave evanescence region has no significant effect on wave coupling.

1.
J.
Jacquot
 et al,
Phys. Plasma
21
,
061509
(
2014
)
2.
V.
Lancellotti
 et al,
Nucl. Fusion
46
(
2006
)
S476
S499
3.
A.
Messiaen
 et al,
Nucl. Fusion
50
025026
(
2010
)
4.
P. M.
Bellan
,
Phys. Plasma
1
(
11
),
Nov. 1994
5.
T.H.
Stix
,
waves in plasmas
,
AIP Press
(
1992
)
6.
J.
Jacquot
 et al,
PPCF
55
115004
(
2013
)
7.
L.
Lu
,
L.
Colas
,
Private communication
(
2013
)
8.
D. A.
D’Ippolito
 et al,
Phys. Plas
,
15
,
102501
(
2008
)
9.
K.
Crombé
 et al,
AIP conf. proc.
1580
,
318
321
(
2014
)
10.
A.
Messiaen
 et al,
PPCF
,
53
(
2011
)
085020
11.
D.
Van Eester
 et al,
PPCF
,
55
025002
(
2013
)
12.
D.
Milanesio
, et al,
PPCF
,
55
045010
(
2013
)
This content is only available via PDF.