1985
DOI: 10.1007/bf00214993
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Observations of ion cyclotron waves near synchronous orbit and on the ground

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Cited by 77 publications
(32 citation statements)
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“…The wave growth rates are controlled by the ring current anisotropy, ion composition, and cold plasma density (Kozyra et al, 1984;Horne and Thorne, 1998). For a detailed review of EMIC waves, see Fraser (1985), Anderson et al (1992), and Millan and Thorne (2006 Global statistical models of the average intensities of equatorial (À151ol m o151) plasmaspheric hiss derived from Combined Release and Radiation Effects Satellite (CRRES) observations are shown as a function of L and MLT for different levels of magnetic activity in the top panels of Fig. 3 (Meredith et al, 2004).…”
Section: Major Types Of Waves Capable Of Violating the First And Secomentioning
confidence: 99%
“…The wave growth rates are controlled by the ring current anisotropy, ion composition, and cold plasma density (Kozyra et al, 1984;Horne and Thorne, 1998). For a detailed review of EMIC waves, see Fraser (1985), Anderson et al (1992), and Millan and Thorne (2006 Global statistical models of the average intensities of equatorial (À151ol m o151) plasmaspheric hiss derived from Combined Release and Radiation Effects Satellite (CRRES) observations are shown as a function of L and MLT for different levels of magnetic activity in the top panels of Fig. 3 (Meredith et al, 2004).…”
Section: Major Types Of Waves Capable Of Violating the First And Secomentioning
confidence: 99%
“…According to the statistical studies of satellite observations such as of Anderson et al [1992a, 1992b] and Fraser and Nguyen [2001], it is evident that the wave events near the equatorial region have unique features. One property is that wave events with linear polarization are frequently observed [ Young et al , 1981; Fraser and McPherron , 1982; Fraser , 1985; Anderson et al , 1992b, 1996; Fraser and Nguyen , 2001]. The dispersion relation of heavy ions indicates that any branch of the wave mode should be predominantly left‐hand (L) or right‐hand (R) polarized except for a few exceptions near the crossover frequency or at oblique propagation near the multi‐ion hybrid resonances [e.g., Rauch and Roux , 1982; Fraser , 1985].…”
Section: Introductionmentioning
confidence: 99%
“…One property is that wave events with linear polarization are frequently observed [ Young et al , 1981; Fraser and McPherron , 1982; Fraser , 1985; Anderson et al , 1992b, 1996; Fraser and Nguyen , 2001]. The dispersion relation of heavy ions indicates that any branch of the wave mode should be predominantly left‐hand (L) or right‐hand (R) polarized except for a few exceptions near the crossover frequency or at oblique propagation near the multi‐ion hybrid resonances [e.g., Rauch and Roux , 1982; Fraser , 1985]. Because wave surveys involve a wide range of observed frequency relative to the ion cyclotron frequency, it is highly unusual that a significant number of wave events are linearly polarized.…”
Section: Introductionmentioning
confidence: 99%
“…[1][2][3][4][5][6][7][8][9][10][11] Previous nonlinear studies have typically considered this mode operating in isolation with the plasma stable to other instabilities. [12][13][14][15] Exceptions include the competitive interaction of the proton cyclotron anisotropy instability and the mirror instability, which has been studied for nondrifting components.…”
Section: Introductionmentioning
confidence: 99%