1979
DOI: 10.1029/rg017i001p00135
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Ionospheric modification and parametric instabilities

Abstract: Thresholds and linear growth rates for stimulated Brillouin and Raman scattering and for the parametric decay instability are derived by using arguments of energy transfer. For this purpose an expression for the ponderomotive force is derived. Conditions under which the partial pressure force due to differential dissipation exceeds the ponderomotive force are also discussed. Stimulated Brillouin and Raman scattering are weakly excited by existing incoherent backscatter radars. The parametric decay instability … Show more

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Cited by 303 publications
(230 citation statements)
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(57 reference statements)
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“…These wave modes give rise to enhancements in both the E-and F-region ion and plasma line incoherent scatter spectra. These spectral enhancements are thought to be caused by excitation of instabilities (Perkins and Kaw, 1971) that include the purely growing mode (Fejer and Leer, 1972), also called the oscillating two-stream instability or modulational instability (Rietveld et al, 2002), and the parametric decay instability (Fejer, 1979). These two instabilities were first observed using the HF heating facility at Arecibo (Carlson et al, 1972;Gordon and Carlson, 1974) as summarized in the review by Carlson and Duncan (1977).…”
Section: Introductionmentioning
confidence: 99%
“…These wave modes give rise to enhancements in both the E-and F-region ion and plasma line incoherent scatter spectra. These spectral enhancements are thought to be caused by excitation of instabilities (Perkins and Kaw, 1971) that include the purely growing mode (Fejer and Leer, 1972), also called the oscillating two-stream instability or modulational instability (Rietveld et al, 2002), and the parametric decay instability (Fejer, 1979). These two instabilities were first observed using the HF heating facility at Arecibo (Carlson et al, 1972;Gordon and Carlson, 1974) as summarized in the review by Carlson and Duncan (1977).…”
Section: Introductionmentioning
confidence: 99%
“…The beam (À3 dB beam size $8.6°) was pointing into the magnetic zenith with a transmitter long pulse of 998 ms ($150 km), receiver gating of 10 ms ($1.5 km), and a data dump time of 10 ms, which was subsequently integrated for 2 s. Observations were made for 0317 -0339 and 0341-0436 UT. Pumping the ionosphere with powerful HF radio waves results in parametric decay instabilities just below the HF reflection altitude [Fejer, 1979], which produce Langmuir and ionacoustic waves to which MUIR is sensitive in the plasmaline and ion-line channels, respectively. Hence during the pump pulses, the radar can measure the pump wave reflection altitude with high temporal resolution.…”
Section: Introductionmentioning
confidence: 99%
“…ia is an ion acoustic wave of a much lower frequency. Langmuir waves have a frequency given by Fejer [1979]:…”
Section: Introductionmentioning
confidence: 99%