Ion beam driven ion-cyclotron waves in a plasma cylinder with negative ions

2001 ◽  
Vol 8 (3) ◽  
pp. 679-686 ◽  
Author(s):  
Suresh C. Sharma ◽  
M. P. Srivastava
1993 ◽  
Vol 50 (2) ◽  
pp. 331-338 ◽  
Author(s):  
S. C. Sharma ◽  
V. K. Tripathi

A helical ion beam propagating through a plasma cylinder drives electrostatic ion-cyclotron waves to instability via cyclotron interaction. Higher harmonics of the beam cyclotron frequency can be generated in this way. The growth rate increases with the harmonic number. The efficiency of beam energy transfer to the wave can be of the order of a few per cent.


1978 ◽  
Vol 19 (2) ◽  
pp. 237-252 ◽  
Author(s):  
J. P. Hauck ◽  
H. Böhmer ◽  
N. Rynn ◽  
Gregory Benford

Ion-cyclotron waves are excited by cesium and potassium ion beams in cesium and potassium Q-machine plasmas. The ion beams are injected along the magnetic field with care to avoid beam transverse velocities. The observed ion-cyclotron mode frequencies are below those driven by electron currents. These resonant instabilities are convective in character with small spatial growth rates ki/kr ≃ 0.05. Plasma ion heating is observed and is consistent with a model in which mode amplitudes are saturated by diffusion effects.


1979 ◽  
Vol 21 (1) ◽  
pp. 19-25 ◽  
Author(s):  
J. P. Hauck ◽  
Gregory Benford

We observe radial expansion of an ion beam propagating along a homogeneous guide magnetic field. The beam spreading appears to arise from interactions with beam-excited resonant ion cyclotron waves. Magnitude and scaling of the expansion agree with a theory based on a resonant diffusion process.


2008 ◽  
Vol 56 (11) ◽  
pp. 1552-1559 ◽  
Author(s):  
S.-H. Kim ◽  
J.R. Heinrich ◽  
R.L. Merlino

1976 ◽  
Vol 57 (3) ◽  
pp. 230-232 ◽  
Author(s):  
M. Sugawa ◽  
R. Sugaya ◽  
H. Nomoto

2011 ◽  
Vol 30 (1) ◽  
pp. 9-16 ◽  
Author(s):  
Asheel Kumar ◽  
V.K. Tripathi

AbstractGyrating ion beams, produced by quick ionization of neutral beams, employed for plasma heating, are susceptible to ion Bernstein and ion cyclotron instabilities. The Bernstein wave, having large parallel phase velocity, is excited via cyclotron interaction whereas the ion cyclotron wave with lower parallel phase velocity could be driven by Cerenkov interaction as well. The maximally growing modes have transverse wave number of the order of inverse ion Larmor radius. The nonlocal effects cause reduction in the growth rate.


1976 ◽  
Vol 55 (6) ◽  
pp. 345-346 ◽  
Author(s):  
P. Michelsen ◽  
H.L. Pécseli ◽  
J.Juul Rasmussen ◽  
N. Sato

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