1983
DOI: 10.1071/ph830725
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Electron Cyclotron Maser Emission near the Cutoff Frequencies

Abstract: An earlier discussion of loss-cone driven cyclotron masers is extended to cover the case where the emission occurs close to the cutoff frequency of the 0 mode or the x mode. In general, wave growth may occur in one or two bands, and when two bands are allowed the lower band is close to the cutoff frequency. With the exception of the x mode at 8 = 1, growth in the lower band is allowed only for OJp/D. > 8 and cos 2 8 > t for the 0 mode and for OJp/Q. > {s(s-I)}-!-and cos 2 8 > (s-I)/8 for the x mode, and growth… Show more

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Cited by 27 publications
(14 citation statements)
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“…Similarly, the 2nd and 3rd harmonic noise bands extend on both sides of the stimulated resonances at 2f H and 3f H . The low frequency cutoff of the o-mode AKR near f H , rather than near the o-mode propagation cutoff at fN , is consistent with the theoretical results of Hewitt and Melrose [1983] that radiation near f H is by far the most important and the results of Wu and Lee [1979] and Hewitt et al [1982] that it is mainly directed upward. In each case, the fundamental AKR signal is clearly observed to exist only in the frequency region below the x-mode cutoff fx.…”
Section: Observationssupporting
confidence: 79%
See 1 more Smart Citation
“…Similarly, the 2nd and 3rd harmonic noise bands extend on both sides of the stimulated resonances at 2f H and 3f H . The low frequency cutoff of the o-mode AKR near f H , rather than near the o-mode propagation cutoff at fN , is consistent with the theoretical results of Hewitt and Melrose [1983] that radiation near f H is by far the most important and the results of Wu and Lee [1979] and Hewitt et al [1982] that it is mainly directed upward. In each case, the fundamental AKR signal is clearly observed to exist only in the frequency region below the x-mode cutoff fx.…”
Section: Observationssupporting
confidence: 79%
“…subject of harmonic AKR has been discussed by Lee et al [1980], 0 Hewitt et al [1982] and Hewitt and Melrose [1983]. The result of these j.nvestigations of the cyclotron instability mechanism is that the harmonics can become important at high plasma densities.…”
Section: Observationsmentioning
confidence: 98%
“…The importance of the energetic distribution function characteristics has been recently emphasized by Melrose et al [19821, Omidi and Gurnett [1982], Wu et al [1982], Dusenbery and Lyons [1982], and Hewitt and Melrose [1983].…”
Section: Discussionmentioning
confidence: 99%
“…We also estimate the parameter regimes in which our approximations break down, and in which a full relativistic treatment is required. In Section 3 we calculate the growth properties of the thermal modes due to maser action driven by a 'hot' loss cone distribution and compare our results with the corresponding results for growth in the magnetoionic modes as given by Hewitt et al (1982), Hewitt and Melrose (1983) and Melrose et al (1984). The results are summarized in Section 4.…”
Section: Introductionmentioning
confidence: 95%
“…Analytic expressions for Eh may be obtained if purely Calculations for maser emission at the fundamental-in the wave modes of a cold plasma-indicate that growth occurs in parameter regimes satisfying w ::::: fle and sin 2 0 ~ 1 (Lee et al 1980;Omidi and Gurnett 1982;Hewitt and Melrose 1983). In this case A ::::: n 2 ( vi C)2 and for a 'warm' plasma (vi C)2 ~ 1 so A will gerrerally be small.…”
Section: Dispersive Properties Of the Warm Background Plasma (A) Dielmentioning
confidence: 99%