1977
DOI: 10.1007/bf01037725
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Parametric interaction between electromagnetic radiation and ionospheric plasma

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Cited by 87 publications
(79 citation statements)
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“…It was found that kilometer scale patches contained 15-m scale filaments associated with deep density depletions and that the filaments were bunched at 50-500 m scales. In contrast to the kilometer and subkilometer scale irregularities, as discussed in the previous paragraph, the small-scale (meters to tens of meters) irregularities have been attributed to the thermal parametric instability [Grach et al, 1978;Das and Fejer, 1979;Inhester et al, 1981;Gurevich et al, 1995] or the parametric decay of the heater wave to frequencies near the ion cyclotron frequency [Keskinen eta!., 1995]. Although the short wavelength end of the self-focusing instability (many tens of meters) remain adjacent to the medium scale irregularities, the growth times of these two classes of irregularities are very different.…”
Section: Introductionmentioning
confidence: 89%
“…It was found that kilometer scale patches contained 15-m scale filaments associated with deep density depletions and that the filaments were bunched at 50-500 m scales. In contrast to the kilometer and subkilometer scale irregularities, as discussed in the previous paragraph, the small-scale (meters to tens of meters) irregularities have been attributed to the thermal parametric instability [Grach et al, 1978;Das and Fejer, 1979;Inhester et al, 1981;Gurevich et al, 1995] or the parametric decay of the heater wave to frequencies near the ion cyclotron frequency [Keskinen eta!., 1995]. Although the short wavelength end of the self-focusing instability (many tens of meters) remain adjacent to the medium scale irregularities, the growth times of these two classes of irregularities are very different.…”
Section: Introductionmentioning
confidence: 89%
“…Artificial FAIs are generally believed to be generated by thermal parametric instabilities (TPIs) which form at altitudes slightly above the upper hybrid resonance height where the pump frequency is the Pythagorean sum of the plasma frequency and the electron gyrofrequency (Grach et al, 1977;Das and Fejer, 1979;Grach et al, 1981;Dsythe et al, 1982;Dsythe et al, 1983). In the nonlinear stage of evolution, the TPI goes over to the resonance instability developed by Gurevich (1975, 1977) and expanded upon by Inhester (1982).…”
Section: Discussionmentioning
confidence: 99%
“…The threshold pump field amplitude needed for irregularity generation was estimated experimentally by Djuth et al (1985). Excitation thresholds for the thermal oscillating two-stream instability, which is thought to initiate the resonance instability, were predicted by Grach et al (1977), Das and Fejer (1979), and Dysthe et al (1983). Grach et al (1978) and Dysthe et al (1982) also anticipated a hysteresis effect associated with the resonance instability and wave trapping, such that irregularities can be maintained by pump waves with amplitudes below their excitation threshold.…”
Section: Introductionmentioning
confidence: 99%