Abstract
We investigated the relationship between post‐midnightF‐region field aligned irregularities (FAIs) andF‐layer altitude by analyzing data of a 30.8‐MHz radar installed 5at Kototabang, Indonesia (0.2°S, 100.3°E; geomagnetic latitude 10.4°S) and an ionosonde installed at Chumphon, Thailand (10.7°N, 99.4°E; geomagnetic latitude 3.3°N). Chumphon is located near the geomagnetic equator on approximately the same meridian as Kototabang. Case studies show that the altitude of theF‐layer rose at Chumphon a half hour before the post‐midnight FAIs appeared at Kototabang. The Doppler velocity of theE‐region FAIs observed simultaneously by the 30.8‐MHz radar was downward, indicating that theF‐layer uplift was not caused by the electric field. We also investigated seasonal variations of the post‐midnight FAI occurrence and theF‐layer altitude. Both the post‐midnight FAIs and the uplift of theF‐layer were frequently seen around midnight between May and August. The seasonal variation of the midnightF‐layer uplift around the geomagnetic equator coincided with that of the post‐midnight FAI occurrence at Kototabang. These results suggest that the uplift of theF‐layer would play an important role in the generation of post‐midnight FAIs. We evaluated the linear growth rate of the Rayleigh‐Taylor instability based on the altitude of theF‐layer observed at Chumphon. The result shows that the uplift of theF‐layer can enhance the growth rate because gravity‐driven eastward electric current increases. Therefore, we interpret that the observed FAIs were accompanied by plasma bubble, the growth rate of which was reinforced by the upliftedF‐layer.
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