Abstract

Abstract. Temporal and spatial evolution of two high-altitude plasma bubbles (evening and midnight) was observed on 4 April 2002, at geomagnetic conjugate points at Sata, Japan (magnetic latitude 24° N), and Darwin, Australia (magnetic latitude 22° S), using two 630-nm airglow imagers. The apex height of the bubbles reached ~1500km. The upward velocity of the evolution was faster in the evening (~170m/s at 20:00-21:00 LT) than around midnight (~28m/s at 23:00-00:00 LT). Bifurcating features of the bubbles into a smaller scale size of ~50km were clearly seen for both the evening and midnight bubbles, showing fairly good conjugacy between the Northern and Southern Hemispheres.

Highlights

  • Equatorial plasma bubble is commonly seen in the postsunset equatorial latitudes as a result of the Rayleigh-Taylor instability, where the low-density plasma on the bottomside of the equatorial ionosphere penetrates through the dense F -layer by polarization electric field (Kelley, 1989)

  • Kelley et al (2002) showed spectacular high-altitude plasma bubbles seen in the airglow images at Haleakala, Hawaii (20.7◦ N, 203.8◦ E; geomagnetic latitude: 21◦ N, dip angle: 37◦)

  • We report time evolution of high-altitude plasma bubbles observed on 4 April 2002, at geomagnetic conjugate points at Sata and Darwin

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Summary

Introduction

Equatorial plasma bubble is commonly seen in the postsunset equatorial latitudes as a result of the Rayleigh-Taylor instability, where the low-density plasma on the bottomside of the equatorial ionosphere penetrates through the dense F -layer by polarization electric field (Kelley, 1989). The bubbles, which are recognized as equatorial spread-F on ionograms, have initially been detected by radio-sounding techniques On the other hand, is a powerful tool to detect spatial and temporal evolution of the bubble structures from ground and satellite We report time evolution of high-altitude plasma bubbles observed on 4 April 2002, at geomagnetic conjugate points at Sata and Darwin. Poleward growth and bifurcation of the bubbles were observed in the field-of-view of all-sky airglow imagers both in the evening (21:00 LT) and around midnight

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