2018
DOI: 10.1002/2017ja024639
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Observation and Numerical Simulation of Cavity Mode Oscillations Excited by an Interplanetary Shock

Abstract: Cavity mode oscillations (CMOs) are basic magnetohydrodynamic eigenmodes in the magnetosphere predicted by theory and are expected to occur following the arrival of an interplanetary shock. However, observational studies of shock‐induced CMOs have been sparse. We present a case study of a dayside ultralow‐frequency wave event that exhibited CMO properties. The event occurred immediately following the arrival of an interplanetary shock at 0829 UT on 15 August 2015. The shock was observed in the solar wind by th… Show more

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Cited by 24 publications
(51 citation statements)
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“…This is consistent with the spacecraft potential data from THEMIS-D that indicate the spacecraft, which was in the posmidnight sector, crossed the plasmapause at L ∼ 5.4 at ∼0650 UT, as shown in Figure 3d of Takahashi et al (2018). The frequency (f T1 , Figure 2d) of the fundamental toroidal (T1) wave that is determined by applying the cross-phase technique (Waters et al, 1991a) to the EMMA data for 0900-1000 UT (Takahashi et al, 2018) decreases monotonically with L, consistent with the n e profile. The frequency (f T1 , Figure 2d) of the fundamental toroidal (T1) wave that is determined by applying the cross-phase technique (Waters et al, 1991a) to the EMMA data for 0900-1000 UT (Takahashi et al, 2018) decreases monotonically with L, consistent with the n e profile.…”
Section: Observatory Locationssupporting
confidence: 89%
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“…This is consistent with the spacecraft potential data from THEMIS-D that indicate the spacecraft, which was in the posmidnight sector, crossed the plasmapause at L ∼ 5.4 at ∼0650 UT, as shown in Figure 3d of Takahashi et al (2018). The frequency (f T1 , Figure 2d) of the fundamental toroidal (T1) wave that is determined by applying the cross-phase technique (Waters et al, 1991a) to the EMMA data for 0900-1000 UT (Takahashi et al, 2018) decreases monotonically with L, consistent with the n e profile. The frequency (f T1 , Figure 2d) of the fundamental toroidal (T1) wave that is determined by applying the cross-phase technique (Waters et al, 1991a) to the EMMA data for 0900-1000 UT (Takahashi et al, 2018) decreases monotonically with L, consistent with the n e profile.…”
Section: Observatory Locationssupporting
confidence: 89%
“…These initial variations are followed by damped E and B oscillations, which have been attributed to multiharmonic cavity mode oscillations (Takahashi et al, 2018). These initial variations are followed by damped E and B oscillations, which have been attributed to multiharmonic cavity mode oscillations (Takahashi et al, 2018).…”
Section: Cavity Mode Oscillations and Flrmentioning
confidence: 96%
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