Electrostatic ion cyclotron wave fields are determined in a magnetized and weakly collisional plasma. A phased‐locked Laser Induced Fluorescence (LIF) diagnostic is used to directly measure the wave perturbed ion velocity distribution. Comparing these local LIF measurements with a theoretical model uniquely determines the wave parameters, such as the wave potential, the three‐dimensional wave vector, and the effective wave damping. The self‐consistent wave–particle interaction is modeled by Boltzmann–Poisson equations in the limit of weak collisions. The wave parameters determined from local measurements agree with those determined from spatial scans.

1.
T. H. Stix, The Theory of Plasma Waves (American Institute of Physics, New York, 1992), pp. 247–262, 317–327.
2.
D. G. Swanson, Plasma Waves (Academic, San Diego, 1989), pp. 142–170.
3.
R. A.
Stern
and
J. A.
Johnson
,
Phys. Rev. Lett.
34
,
1548
(
1975
).
4.
H.
Ikezi
and
R. J.
Taylor
,
Phys. Rev. Lett.
22
,
923
(
1969
).
5.
D.
Gresillon
,
J. Phys.
32
,
269
(
1971
).
6.
F.
Skiff
and
F.
Anderegg
,
Phys. Rev. Lett.
59
,
896
(
1987
).
7.
F.
Skiff
,
IEEE Trans. Plasma Sci.
PS-20
,
701
(
1992
).
8.
N. Hershkowitz, in Plasma Diagnostics: Vol. 1, Discharge Parameters and Chemistry, edited by O. Auciello and D. L. Flamm (Academic, San Diego, 1989).
9.
F. F. Chen, in Plasma Diagnostics Techniques, edited by R. H. Huddlestone and S. L. Leonard (Academic, San Diego, 1965).
This content is only available via PDF.
You do not currently have access to this content.