1986
DOI: 10.1016/0032-0633(86)90117-0
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Characteristics of dawnside mid-latitude VLF emissions associated with substorms as deduced from the two-stationed direction finding measurement

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Cited by 30 publications
(29 citation statements)
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“…In this case, however, the starting longitudes of the eastward drifting become 69.1 ° and 109.8° for the first and second peaks, respectively, which seems to be rather different from the statistical results (HAYAKAWA et al, 1986a). So, it may be implied that 5 keV electrons in the evening sector injected associated with the second H- HAYAKAWA et al (1986b) exhibited a regular frequency drift of the maximum energy of the midlatitude VLF hiss (L = 3.0) observed at dawn time, of which increasing rate was mostly below 1.5 kHz/ hr. They have explained that the property is related to the energy dependence of drifting velocities of the electrons encircling from the evening to the dawn sectors through the midnight in the equatorial magnetosphere.…”
Section: Observations Of Vlf Emissions and The Analysis Of Frequency contrasting
confidence: 68%
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“…In this case, however, the starting longitudes of the eastward drifting become 69.1 ° and 109.8° for the first and second peaks, respectively, which seems to be rather different from the statistical results (HAYAKAWA et al, 1986a). So, it may be implied that 5 keV electrons in the evening sector injected associated with the second H- HAYAKAWA et al (1986b) exhibited a regular frequency drift of the maximum energy of the midlatitude VLF hiss (L = 3.0) observed at dawn time, of which increasing rate was mostly below 1.5 kHz/ hr. They have explained that the property is related to the energy dependence of drifting velocities of the electrons encircling from the evening to the dawn sectors through the midnight in the equatorial magnetosphere.…”
Section: Observations Of Vlf Emissions and The Analysis Of Frequency contrasting
confidence: 68%
“…The VLF hiss exhibited a regular frequency drift; the frequency (fmax) of the maximum energy increased with local time. It is explained that the property is due to the dispersion of the drifting velocities of energetic electrons drifting from the midnight sector of their initial injection toward the generation region (dawn sector) (HAYAKAWA et al, 1986b). This paper presents low-latitude VLF hiss observed at dawn time at Moshiri (L = 1.6) and Kagoshima (L = 1.2) stations in Japan associated with the severe magnetic storm (Kp = 8) on October 19-21, 1989.…”
Section: Introductionmentioning
confidence: 91%
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“…The typical source of these electrons and their anisotropies are the same as for protons, particle injection from the nightside plasma sheet during magnetic storms [Tsurutani et al, 1975;Delport et al, 2012], or substorms [Thorne et al, 1974[Thorne et al, , 1977Smith, 1974, 1977;Hayakawa et al, 1986;Koons and Roeder, 1990;Meredith et al, 2001Meredith et al, , 2012Li et al, 2013]. However, electrons drift from midnight through dawn, in the opposite sense as the protons.…”
Section: Introductionmentioning
confidence: 99%
“…The maximum of their occurrence corresponded to the middle latitudes (55-65 • ) which are connected with the plasmapause projection (Hayakawa et al, 1975a(Hayakawa et al, , b, 1977(Hayakawa et al, , 1986(Hayakawa et al, , 1988Dronov et al, 1985;Kleimenova, 1985).…”
Section: Plasmaspheric Hiss and Mid-latitude Hissmentioning
confidence: 99%