2013
DOI: 10.1017/s0263034613000591
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Excitation of lower hybrid wave by an ion beam in magnetized plasma

Abstract: Lower hybrid wave excitation in magnetized plasma by an ion beam via Cerenkov interaction is studied. The lower hybrid modes showed maximum growth rate of the instability when phase velocity of the lower hybrid mode along the magnetic field is comparable to the electron thermal velocity. We have derived the expression for the maximum growth rate and found that the growth rate of the instability increases with beam density. Moreover, the maximum growth rate of the instability scales as the one-third power of th… Show more

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Cited by 10 publications
(5 citation statements)
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References 20 publications
(34 reference statements)
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“…An ion beam moving perpendicular to B can also provide the free energy source for the finite LH wave (Prakash et al., 2013) with finite k z . Similar to the parallel electron beam source, the LH wave can be excited in magnetized plasma by a perpendicular ion beam through Cerenkov interactions.…”
Section: Origin Of the Observed Spwementioning
confidence: 99%
See 1 more Smart Citation
“…An ion beam moving perpendicular to B can also provide the free energy source for the finite LH wave (Prakash et al., 2013) with finite k z . Similar to the parallel electron beam source, the LH wave can be excited in magnetized plasma by a perpendicular ion beam through Cerenkov interactions.…”
Section: Origin Of the Observed Spwementioning
confidence: 99%
“…The maximum LH growth occurs for a wave propagation angle of 89.1 Degrees. The linear ion beam analysis of (Prakash et al., 2013) has determined that the energy to excite the LH mode is 10–100 time lower than that required for an electron beam. Thus, relatively low energy electron or ion beams could be responsible for the excited LH waves seen as SPWEs in Figures 1a and 1b.…”
Section: Origin Of the Observed Spwementioning
confidence: 99%
“…It is well known that the ion beams dominantly excite the parallel-propagating waves through the "resonant" and "non-resonant" instabilities. [11][12][13][14][15][16][17][18] The growth rates of these instabilities are usually larger than those of the other instabilities while the left-hand polarized waves are dominantly excited when the beams are relatively hot and/or weak. Heidbrink [19] analysed Alfven instabilities driven by energetic particles in toroidally confined plasmas and observed two modes of Alfven instabilities occurring due to resonance between the orbital frequencies of the energetic particles and the wave phase velocity.…”
Section: Introductionmentioning
confidence: 99%
“…Ion beam and interaction of radiation with plasma allocate a free energy source which can excite different wave modes in a plasma. Plasma waves can be stabilized or destabilized when they interact with electron or ion beams [4][5][6][7][8][9][10][11], and collisions generally have a stabilizing effect on the plasma waves [12,13]. An ion beam can destabilize Alfven waves and whistler waves if the beam speed is sufficiently large.…”
Section: Introductionmentioning
confidence: 99%