2013
DOI: 10.1002/jgra.50344
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Substorm‐associated explosive magnetic field stretching near the earthward edge of the plasma sheet

Abstract: [1] We report a detailed analysis of explosive local magnetic field line stretching just before dipolarization observed by one of Time History of Events and Macroscale Interactions during Substorms (THEMIS) satellites during the pseudo-breakup followed by local substorm of 6 January 2008. At the end of the substorm growth phase, this satellite (THEMIS-C) was located at r~6.3 R E near the convection boundary of 10 keV electrons. Penetration of the hot electron plasma sheet to the region of trapped energetic ion… Show more

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Cited by 17 publications
(8 citation statements)
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References 70 publications
(137 reference statements)
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“…It is commonly agreed that the appearance of a ballooning perturbation (i.e., a bubble or a bubble-blob pair) in the near-Earth tail provokes its destabilization and under certain conditions may trigger substorm. Previously it was suggested that ballooning-type perturbations can appear in the near tail either due to earthward floating plasma bubbles, as initially proposed by Erickson and Wolf [1980] and observationally evidenced by Baumjohann et al [1989], Angelopoulos et al [1992], and others or in result of ballooning/interchange instability growth [e.g., Roux et al, 1991;Saito et al, 2008;Coroniti, 2010, 2011;Panov et al, 2012;Kozelova and Kozelov, 2013]. The present study points to one more possibility, namely, that ballooning perturbations can be transported to the near tail by propagating ballooning waves.…”
Section: 1002/2014ja020081supporting
confidence: 71%
See 1 more Smart Citation
“…It is commonly agreed that the appearance of a ballooning perturbation (i.e., a bubble or a bubble-blob pair) in the near-Earth tail provokes its destabilization and under certain conditions may trigger substorm. Previously it was suggested that ballooning-type perturbations can appear in the near tail either due to earthward floating plasma bubbles, as initially proposed by Erickson and Wolf [1980] and observationally evidenced by Baumjohann et al [1989], Angelopoulos et al [1992], and others or in result of ballooning/interchange instability growth [e.g., Roux et al, 1991;Saito et al, 2008;Coroniti, 2010, 2011;Panov et al, 2012;Kozelova and Kozelov, 2013]. The present study points to one more possibility, namely, that ballooning perturbations can be transported to the near tail by propagating ballooning waves.…”
Section: 1002/2014ja020081supporting
confidence: 71%
“…[], Angelopoulos et al . [], and others or in result of ballooning/interchange instability growth [e.g., Roux et al ., ; Saito et al ., ; Pritchett and Coroniti , , ; Panov et al ., ; Kozelova and Kozelov , ]. The present study points to one more possibility, namely, that ballooning perturbations can be transported to the near tail by propagating ballooning waves.…”
Section: Discussionmentioning
confidence: 52%
“…Equatorward movement of the boundaries seen prior to the onset caused by the stretching of field lines in the magnetotail during the growth phase of a substorm [Kozelova and Kozelov 2013]. As seen in Figure 8, the mean field is much weaker (stretching) during sawtooth events compared to shock related onsets as also indicated in Figure 7a, where the oval boundaries, during sawtooth events, were located equatorward of the boundaries during shock related onsets.…”
Section: Discussionmentioning
confidence: 71%
“…A similar outward radial current, inward radial electric field has been suggested by Lui and Kamide [] to develop after substorm current disruption during dipolarization. Recently, using measurements from THEMIS C during two substorms, Kozelova and Kozelov [] found the inner plasma sheet edge outward E ψ ‐inward J ψ signature of Figure during the “explosive” growth phase stretching of the magnetic field, and the reverse‐signed signature after substorm onset when the Harang discontinuity apparently passed earthward of THEMIS.…”
Section: The Quiet Evening Arcmentioning
confidence: 99%