Ground-based noontime D-region electron density climatology over northern Norway

The bottom part of the Earth's ionosphere is the so-called D region, which is typically less dense than the upper regions. Despite the comparably lower electron density, the ionization state of the D region has a significant influence on signal absorption for propagating lower to medium radio f...

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Bibliographic Details
Published in:Atmospheric Chemistry and Physics
Main Authors: Renkwitz, Toralf, Sivakandan, Mani, Jaen, Juliana, Singer, Werner
Format: Article in Journal/Newspaper
Language:English
Published: Copernicus Publications 2023
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Online Access:https://doi.org/10.5194/acp-23-10823-2023
https://noa.gwlb.de/receive/cop_mods_00069101
https://noa.gwlb.de/servlets/MCRFileNodeServlet/cop_derivate_00067503/acp-23-10823-2023.pdf
https://acp.copernicus.org/articles/23/10823/2023/acp-23-10823-2023.pdf
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Summary:The bottom part of the Earth's ionosphere is the so-called D region, which is typically less dense than the upper regions. Despite the comparably lower electron density, the ionization state of the D region has a significant influence on signal absorption for propagating lower to medium radio frequencies. We present local noon climatologies of electron densities in the upper middle atmosphere (50–90 km) at high latitudes as observed by an active radar experiment. The radar measurements cover 9 years (2014–2022) from the solar maximum of cycle 24 to the beginning of cycle 25. Reliable electron densities are derived by employing signal processing, applying interferometry methods, and applying the Faraday-International Reference Ionosphere (FIRI) model. For all years a consistent spring–fall asymmetry of the electron density pattern with a gradual increase during summer as well as a sharp decrease at the beginning of October was found. These findings are consistent with very low frequency (VLF) studies showing equivalent signatures for nearby propagation paths. It is suggested that the meridional circulation associated with downwelling in winter could cause enhanced electron densities through NO transport. However, this mechanism can not explain the reduction in electron density in early October.