2000
DOI: 10.1029/2000ja000230
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Excitation of Langmuir waves in interplanetary space

Abstract: Abstract. In this paper, the relation between the apparently stable or marginally stable electron reduced distribution and the excitation of Langmuir waves is discussed. It is found that the positive slope in the reduced distribution function is not always necessary for the excitation of Langmuir waves and that under certain circumstances, Langmuir waves propagating in oblique directions with respect to the ambient magnetic field can be excited by the electrons which may not have a bump in the reduced distribu… Show more

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Cited by 2 publications
(2 citation statements)
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“…Although a bump occurring at some nonzero pitch angle can generate Langmuir waves [Yoon et al, 2000], we shall limit ourselves to the more robust instability criterion requiring a localized positive gradient ∂f (v k )/∂v k > 0 in the reduced electron distribution functionf , easier to compare with the present low time resolution observations. It is not obvious to explain how such a positive slope in the electron distribution function may be formed in a magnetic hole, especially if one takes into account the fact that linear instability theory shows that "slow beams" (i.e., with velocity such that v b ≈ v te ) with a beam temperature similar to core electron temperature and density smaller (not necessarily much smaller) than the core plasma density are not sufficient to drive the plasma unstable [Gary, 1985].…”
Section: Wave Generation Mechanismmentioning
confidence: 99%
“…Although a bump occurring at some nonzero pitch angle can generate Langmuir waves [Yoon et al, 2000], we shall limit ourselves to the more robust instability criterion requiring a localized positive gradient ∂f (v k )/∂v k > 0 in the reduced electron distribution functionf , easier to compare with the present low time resolution observations. It is not obvious to explain how such a positive slope in the electron distribution function may be formed in a magnetic hole, especially if one takes into account the fact that linear instability theory shows that "slow beams" (i.e., with velocity such that v b ≈ v te ) with a beam temperature similar to core electron temperature and density smaller (not necessarily much smaller) than the core plasma density are not sufficient to drive the plasma unstable [Gary, 1985].…”
Section: Wave Generation Mechanismmentioning
confidence: 99%
“…In the standard scenario (Ginzburg & Zhelezniakov 1958), the non-linear interaction of beam-driven plasma waves leads to the appearance of rather strong radio emission -type III solar/interplanetary radio bursts. The observations of type III solar bursts and energetic particles (Lin et al 1981;Ergun et al 1998;Gosling et al 2003;Krucker et al 2007) as well as hamish@astro.gla.ac.uk, eduard@astro.gla.ac.uk theoretical (Zheleznyakov & Zaitsev 1970;Zaitsev et al 1972;Mel'Nik 1995) and numerical investigations (Magelssen & Smith 1977;Grognard 1982;Kontar' et al 1998;Yoon et al 2000;Kontar 2001b;Li et al 2006a;Ledenev et al 2004;Krasnoselskikh et al 2007) provide strong support to the standard type III model.…”
mentioning
confidence: 99%