1982
DOI: 10.1088/0031-8949/1982/t2b/040
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Thermal Cavitons

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Cited by 107 publications
(103 citation statements)
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“…The FAIs we observe are understood to be produced at the upper-hybrid resonance height (Grach et al, 1977;Das and Fejer, 1979;Grach et al, 1981;Dysthe et al, 1982Dysthe et al, , 1983. On the basis of calculations outlined below, we expect Omode radiation from HAARP to penetrate to this height for both zenith and magnetic zenith pointing and to generate FAIs with roughly comparable characteristics in either case.…”
Section: Zenith and Magnetic Zenith Pointingmentioning
confidence: 79%
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“…The FAIs we observe are understood to be produced at the upper-hybrid resonance height (Grach et al, 1977;Das and Fejer, 1979;Grach et al, 1981;Dysthe et al, 1982Dysthe et al, , 1983. On the basis of calculations outlined below, we expect Omode radiation from HAARP to penetrate to this height for both zenith and magnetic zenith pointing and to generate FAIs with roughly comparable characteristics in either case.…”
Section: Zenith and Magnetic Zenith Pointingmentioning
confidence: 79%
“…6, it appears that irregularities are not produced until the heater power reaches about one fifth its maximum while irregularities can be maintained virtually until the time heating is discontinued. Grach et al (1978) and Dysthe et al (1982) predicted this kind of hysteresis, arguing that it should be possible to maintain irregularities with less power than is necessary to excite them because differential heating by the the resonance instability increases in efficiency with the intensity of the irregularities. Some preliminary evidence for their hypothesis was available at that time (Erukhimov et al, 1978;Stubbe et al, 1982;Kopka et al, 1982).…”
Section: Hysteresis and Striation Formationmentioning
confidence: 99%
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“…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%
“…Upper-hybrid waves can also be generated through the linear mode conversion of the pump wave in the vicinity of existing density striations (Mishin et al, 2004(Mishin et al, , 2005. Upper hybrid wave trapping within the striations leads to ohmic heating, deepening of the striations, and thermal parametric instability (Grach et al, 1981;Dsythe et al, 1982). Subsequent wave growth leads to explosive growth through resonance instability (Vas'kov and Gurevich, 1977).…”
Section: Discussionmentioning
confidence: 99%