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Coupled Evolution of Storm-Enhanced Density, Tongue of Ionization, and Polar Ionospheric Hole during the 10 May 2024 Superstorm

ZHANG Shun-Rong,  COSTER Anthea J,  Ercha AA,  THAYYIL Jayachandran P,  ZHANG Yongliang

ZHANG Shun-Rong, COSTER Anthea J, Ercha AA, THAYYIL Jayachandran P, ZHANG Yongliang. Coupled Evolution of Storm-Enhanced Density, Tongue of Ionization, and Polar Ionospheric Hole during the 10 May 2024 Superstorm. Chinese Journal of Space Science, 2026, 46(5): 1-14 doi: 10.11728/cjss2026.05.2026-0019
Citation: ZHANG Shun-Rong, COSTER Anthea J, Ercha AA, THAYYIL Jayachandran P, ZHANG Yongliang. Coupled Evolution of Storm-Enhanced Density, Tongue of Ionization, and Polar Ionospheric Hole during the 10 May 2024 Superstorm. Chinese Journal of Space Science, 2026, 46(5): 1-14 doi: 10.11728/cjss2026.05.2026-0019

Coupled Evolution of Storm-Enhanced Density, Tongue of Ionization, and Polar Ionospheric Hole during the 10 May 2024 Superstorm

doi: 10.11728/cjss2026.05.2026-0019 cstr: 32142.14.cjss.2026-0019
More Information
    Author Bio:

    Dr. Shun-Rong Zhang, the first author and corresponding author, is a Principal Research Scientist at MIT Haystack Observatory. He has been actively involved in a diverse range of ionosphere and upper atmosphere research, encompassing geospace storm effects, variability, climatology, long-term changes, and the associated coupling processes in ionosphere-thermosphere-magnetosphere and atmospheric systems. E-mail: shunrong@mit.edu

  • Figure  1.  Solar geophysical conditions for 10–12 May 2024. IMF By and Bz (a), interplanetary electric field (b), SYM-H index (c), solar wind dynamic pressure (d), auroral AU and AL index (e)

    Figure  2.  Latitudinal and UT variations in TEC (TECU, a and d), TEC relative changes (percentage fraction) from the reference on 10 May 2024 (b and e), and dTEC (TECU, c and f) in American (left panels) and Asian (right panels) sectors which have 12-hour local time offset. Dashed lines mark the ICME arrival induced simultaneous ionospheric variations

    Figure  3.  A sequence of global TEC maps to demonstrate the SED development. TEC variations are shown as absolute difference from the reference day 10 May 2024 (left) and relative percentage (fractional) change (right)

    Figure  4.  SED plume temporal evolution in latitude for a broad longitude bin −115°E to −90°E degrees (a), and in longitude at 60°N–65°N Apex latitude (b), and at 65 N–70°N Apex latitude (c) on 10 May 2024

    Figure  5.  A polar view of TEC snapshots between 17:00–21:30 UT on 10 May 2024 to demonstrate the plasma density gradients TOI or the patch (see red arrows) and Polar Ionization Hole (back arrows). Corresponding GUVI O/N2 variations along the trajectory of the TIMED are also shown at approximate times of TEC snapshots. Note that the depletion of O/N2 inside the polar cap does not align with the region of enhanced TEC, which would suggest auroral precipitation

    Figure  6.  Same as Figure 5 but for snapshots at 21:45–08:55 UT (10–11 May 2024). Yellow arrows mark the area of enhanced TEC due to auroral particle precipitation

    Figure  7.  Longitudinal propagation inside the polar cap of density structures in TOI and patches (a and b), and dTEC fluctuations (c and d) over two apex latitude bins of 70°N–75°N (left) and 75°N–80°N (right) on 10 May 2024

    Figure  8.  A polar view of the GUVI O/N2 measurements at ~08:30 LT on 10−11 May 2024. Orbit-by-orbit variations is shown in the left panels; a smoothed version to fill the gaps is provided merely to show a big and rough picture of O/N2 distribution in the polar region

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  • 网络出版日期:  2026-06-16

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