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Longitudinal variation in the ionosphere-plasmasphere system at the minimum of solar and geomagnetic activity: Investigation of temporal and latitudinal dependences

Klimenko, Maxim V., Klimenko, Vladimir V., Zakharenkova, Irina E., Vesnin, Artem M., Cherniak, Iurii V., and Galkin, Ivan A., 2016. Longitudinal variation in the ionosphere-plasmasphere system at the minimum of solar and geomagnetic activity: Investigation of temporal and latitudinal dependences. Radio Science, 51(12):1864–1875, doi:10.1002/2015RS005900.

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@ARTICLE{2016RaSc...51.1864K,
       author = {{Klimenko}, Maxim V. and {Klimenko}, Vladimir V. and {Zakharenkova}, Irina E. and {Vesnin}, Artem M. and {Cherniak}, Iurii V. and {Galkin}, Ivan A.},
        title = "{Longitudinal variation in the ionosphere-plasmasphere system at the minimum of solar and geomagnetic activity: Investigation of temporal and latitudinal dependences}",
      journal = {Radio Science},
     keywords = {ionosphere, longitudinal variation, plasmasphere, model, Weddell Sea Anomaly, total electron content},
         year = 2016,
        month = dec,
       volume = {51},
       number = {12},
        pages = {1864-1875},
     abstract = "{We use the Global Self-consistent Model of the Thermosphere, Ionosphere
        and Protonosphere (GSM TIP) as the first-principle calculation
        of the physical system state, the quick-run ionospheric electron
        density model (NeQuick) as the climatology background, and the
        International Reference Ionosphere-based Real-Time Assimilative
        Model for a global view of the ionospheric weather during a
        quiet period of the December 2009 solstice. The model
        computations are compared to the Constellation Observing System
        for Meteorology, Ionosphere, and Climate (COSMIC) radio
        occultation profiles, CHAMP and Gravity Recovery and Climate
        Experiment in situ densities, and GPS total electron content
        (TEC). It is shown that the plasma density in the ionosphere is
        generally larger in the American/Atlantic longitudinal sector at
        any local time. The high-latitude density enhancements are
        visible in the GSM TIP output at different altitudes but are not
        reproduced by the NeQuick empirical model. Given that
        observational data confirm an existence of the high-latitude
        areas where ionospheric densities are elevated in the altitude
        range between 300 and 480 km, we conclude that the
        N$_{m}$F$_{2}$ maximum in the GSM TIP output can be trusted.
        Indeed, such high-latitude N$_{m}$F$_{2}$, ionospheric electron
        content, and TEC maxima in the American longitude sector form on
        the proper places as shown by the GSM TIP data, COSMIC and GPS
        observations. According to our results, the high-latitude
        maximum of N$_{m}$F$_{2}$ (1) manifests itself only when the
        integration over LT or UT of the global maps for 22 December
        2009 includes nighttime, i.e., supporting an argument of its
        close association with the Weddell Sea Anomaly, and (2) also
        appears in the N$_{e}$ distribution at altitudes above the
        F$_{2}$ peak.}",
          doi = {10.1002/2015RS005900},
       adsurl = {https://ui.adsabs.harvard.edu/abs/2016RaSc...51.1864K},
      adsnote = {Provided by the SAO/NASA Astrophysics Data System}
}

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