Space Physics and Aeronomy, Ionosphere Dynamics and Applications. Группа авторов
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СКАЧАТЬ 3 Center for Solar‐Terrestrial Research, New Jersey Institute of Technology, Newark, NJ, USA

       4 Massachusetts Institute of Technology Haystack Observatory, Westford, MA, USA

      ABSTRACT

      In the polar cap region, high‐density ionospheric structures, such as the large‐scale tongue‐of‐ionization and mesoscale polar cap patches, are frequently observed, which are of significant space weather concerns. In this chapter, recent progress on these polar cap high‐density ionospheric structures is reviewed with an emphasis on the polar cap patch. Topics include the statistical occurrence rate of patches, plasma structure and characteristics inside patches, dynamic horizontal and vertical transport of high‐density ionospheric structures, as well as the mechanisms and variability of optical patch emissions. For each topic, future works are envisioned following the progress reviews.

      Ionospheric density varies significantly and affects the propagation of radio signals that pass through the ionosphere or are reflected by it. One example of these effects is the loss of phase lock and range errors in Global Navigation Satellite Systems (GNSS) signals. Because our modern society increasingly relies on ground‐to‐ground and ground‐to‐space communications and navigation, understanding the sources of the ionospheric density variability and monitoring its dynamics during space weather events is of great practical importance (e.g., Jin et al., 2014, 2017; Moen et al., 2013; Zhang et al., 2018).

      Due to the geometry of the Earth's magnetic field, the solar wind has direct access to the high‐latitude polar cap region because the magnetic field lines there are open. The convection electric fields in the solar wind map directly down to the polar cap along the equipotential magnetic field lines (Lyons & Williams, 1984). The shape and size of the polar cap change considerably with varying solar wind and the polarity and magnitude of interplanetary magnetic field (IMF). Typically, the open‐closed field line boundary (OCB) of the polar cap expands to lower latitudes during southward IMF condition and retreats back to higher latitudes during northward IMF condition. Particles in the solar wind and magnetosheath can move along the magnetic field line down to the polar cap ionosphere and form the polar rain (Fairfield & Scudder, 1985). In the polar cap region, the most important high‐density structures in the F region and topside ionosphere are polar cap patches and storm‐enhanced density (SED) plumes and/or tongues of ionizations (TOIs) (Whitteker et al., 1978).

Schematic illustrations of an example of dynamic polar cap density structures.

      Reproduced with permission of John Wiley and Sons).

      The difference between the SED plume/TOI and polar cap patch lies in their structural size with the former/latter being of larger/smaller scale size. In addition, it has been suggested that the SED plume/TOI is the major plasma source for the patches (Foster et al., 2005). Intermittent bursts of cold (low Te) SED plasma streaming into the polar cap in the noontime cusp ionosphere were observed with the Chatanika (Foster & Doupnik, 1984) and Sondrestrom (Foster et al., 1985) ISRs. However, particle precipitations in the cusp (Rodger et al., 1994) and those within the polar cap are also proposed to be able to create patches, but of weaker effect (Hosokawa et al., 2016; Oksavik et al., 2006).

      This brief review focuses on recent progresses of polar cap patches and SED plumes/TOIs. In the following sections, we review the statistical occurrence rate of patches, plasma structure, and characteristics inside patches, as well as dynamic horizontal and vertical transport of the high‐density plasma. We also review various mechanisms and the variability of patch optical signatures. Future research directions follow progress review for each topic. The formation and evolution of the SEDs, which are closely related with patches and TOI, are reviewed separately in Chapter 7 in this book and are not included in this chapter.