SA24A-07
Profiles of Ionospheric Storm-enhanced Density during the 17 March 2015 Great Storm

Tuesday, 15 December 2015: 17:21
2016 (Moscone West)
Jing Liu1, Wenbin Wang1, Alan Geoffrey Burns2, Xinan Yue3, Shunrong Zhang4 and Yongliang Zhang5, (1)High Altitude Observatory, Boulder, CO, United States, (2)National Center for Atmospheric Research, Boulder, CO, United States, (3)UCAR, Boulder, CO, United States, (4)MIT Haystack Observatory, Westford, MA, United States, (5)Johns Hopkins University, Baltimore, MD, United States
Abstract:
Ionospheric F2 region peak densities (NmF2) are expected to show a positive phase correlation with total electron content (TEC), and electron density is expected to have an anti-correlation with electron temperature near the ionospheric F2 peak. However, we show that, during the 17 March 2015 great storm, TEC and F2 region electron density peak height (hmF2) over Millstone Hill increased, but the F2 region electron density peak (NmF2) decreased significantly during the storm-enhanced density (SED) phase of the storm compared with the quiet-time ionosphere. This SED occurred where there was a negative ionospheric storm near the F2 peak and below it. The weak ionosphere below the F2 peak resulted in much reduced downward heat conduction for the electrons, trapping the heat in the topside. This, in turn, increased the topside scale height, so that, even though electron densities at the F2 peak were depleted, TEC increased in the SED. The depletion in NmF2 was probably caused by an increase in the density of the molecular neutrals, resulting in enhanced recombination. In addition, the storm-time topside ionospheric electron density profile was much closer to diffusive equilibrium than non-storm time profile because of less daytime plasma flow from the ionosphere to the plasmasphere.