Long-term ionospheric cooling: Dependency on local time, season, solar activity, and geomagnetic activity

Abstract
<p>Ionospheric ion temperature Ti is an excellent approximation to neutral temperature Tn in the thermosphere, especially for altitudes below 300 km. This analysis of long-term Ti trends in the F region over different local times is based on a database of incoherent scatter radar (ISR) observations spanning more than three solar cycles during 1968\textendash2006 at Millstone Hill and represents an extended effort to a prior study focusing on noon-time only. This study provides important information for understanding the difference between the ISR and other results. A gross average of the Ti trend at heights of Ti \~ Tn (200\textendash350 km) is \~ -4 K/decade, a cooling trend close to the Tn estimation based on the satellite neutral density data. However, there exists considerable variability in the cooling: it is strong during the day and very weak during the night with a large apparent warming at low altitudes (200\textendash350 km); it is strong at solar minimum for both daytime and nighttime. The strongest cooling for altitudes below 375 km occurs around 90\textendash120 solar flux units of the 10.7 cm solar flux, not at the lowest solar flux. There appears more cooling toward high magnetic activity, but this dependency is very weak. No consistent and substantial seasonal dependency across different heights was found. We speculate that a fraction of the observed cooling trend may be contributed by a gradual shifting away from the sub-auroral region at Millstone Hill, as part of the secular change in the Earth\textquoterights magnetic field. In this 39 year long series of data record, two anomalous Ti drops were noticed, and we speculate on their connection to volcano eruptions in 1982 and 1991.</p>
Year of Publication
2013
Journal
Journal of Geophysical Research: Space Physics
Volume
118
Number of Pages
3719-3730
Date Published
06/2013
URL
http://doi.wiley.com/10.1002/jgra.50306
DOI
10.1002/jgra.50306