1976
DOI: 10.1029/ja081i010p01707
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coherent generation of VLF hiss

Abstract: VLF hiss is proposed to result from convective beam amplification of incoherent Cerenkov whistler radiation by the beam of precipitating auroral electrons. The beam amplification mechanism is investigated by using the lowest‐order WKB wave kinetic equation and linear growth rates. It is shown that incoherent Cerenkov radiation cannot produce strong VLF hiss without beam amplification and that the beam amplification mechanism can account for the observed bandwidth and power fluxes of strong VLF hiss when the el… Show more

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Cited by 226 publications
(180 citation statements)
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“…In contrast to the purely electrostatic Langmuir waves well studied in past, analogous investigations in magnetized plasmas at oblique propagation, however, require the full apparatus of electromagnetic plasma dispersion theory and less work on this has appeared in the literature (see e.g. Kennel, 1966;Maggs, 1976;Lin et al, 1984;Morgan et al, 1994;Willes and Cairns, 2000;Kopf et al, 2010).…”
Section: Discussion and Summarymentioning
confidence: 99%
“…In contrast to the purely electrostatic Langmuir waves well studied in past, analogous investigations in magnetized plasmas at oblique propagation, however, require the full apparatus of electromagnetic plasma dispersion theory and less work on this has appeared in the literature (see e.g. Kennel, 1966;Maggs, 1976;Lin et al, 1984;Morgan et al, 1994;Willes and Cairns, 2000;Kopf et al, 2010).…”
Section: Discussion and Summarymentioning
confidence: 99%
“…[30] The second panel in Figure 8 shows the VLF activity throughout the flight, indicating, through coherent generation of whistler mode VLF hiss, the large-scale electron precipitation [Maggs, 1976]. There was strong VLF hiss throughout T + 0 to T + 450s, when the rocket flew through the 3 large arcs seen in the all-sky and Polar images.…”
Section: Flight Surveymentioning
confidence: 99%
“…Hence when the S3 and S4 baselines imply smaller electric fields compared to the 34 baseline, the wavelengths must be less than roughly 30 m. Above the lower hybrid frequency (8 kHz at 266 s and 6 kHz at 406 s), plasma waves often become short wavelength when auroral hiss propagates onto the lower hybrid resonance cone [Maggs, 1976;Paschmann, 2002], which explains why the baselines imply different electric fields at higher frequencies. However the situation below 5 kHz is different.…”
Section: In Situ Datamentioning
confidence: 99%