ST2.6 | Multiscale Solar-Wind-Magnetosphere-ionosphere Interactions: Insights from Observations and Simulations
Multiscale Solar-Wind-Magnetosphere-ionosphere Interactions: Insights from Observations and Simulations
Convener: Lei Dai | Co-conveners: C.-Philippe Escoubet, QiuGang Zong, Yukitoshi Nishimura, Yiqun Yu
Orals
| Mon, 28 Apr, 14:00–17:55 (CEST)
 
Room 0.94/95
Posters on site
| Attendance Tue, 29 Apr, 10:45–12:30 (CEST) | Display Tue, 29 Apr, 08:30–12:30
 
Hall X4
Orals |
Mon, 14:00
Tue, 10:45
The solar wind interacts with Earth's magnetosphere-ionosphere system, driving processes at kinetic, fluid, and global scales. Understanding these multiscale processes is crucial for a comprehensive grasp of solar-wind-magnetosphere interactions. This session focuses on studies using observational data and simulations to explore these interactions across various scales. At the global scale, we examine characteristics of geomagnetic storms and substorms as system responses to solar wind conditions. At the intermediate scale, we investigate phenomena such as convective flows, convective electric fields, electric current systems, Kelvin-Helmholtz (KH) instability in boundary layers, flux transfer events, high-speed jets, ULF waves, and auroral arcs. These phenomena are explored as consequences of various solar wind drivers and cross-region coupling, providing insights into the physical links within global processes. At the kinetic scale, we study kinetic processes and plasma waves to gain insights into energy dissipation mechanisms. We invite contributions that aim to elucidate multiscale dynamic processes governing energy transfer, particle acceleration, energy dissipation, and magnetosphere-ionosphere disturbances. By integrating data from space missions, ground-based observatories, and advanced numerical models, our approach will deepen the understanding of the magnetosphere-ionosphere system's responses to the solar wind, enhancing our ability to predict space weather.

Orals: Mon, 28 Apr, 14:00–18:00 | Room 0.94/95

Chairpersons: C.-Philippe Escoubet, QiuGang Zong, Lei Dai
14:00–14:10
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EGU25-9904
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On-site presentation
Linggao Kong, Lei Dai, Aibing Zhang, Georgios Nicolaou, Matthieu Berthomier, Jun Gao, Bin Su, Philippe Escoubet, Chi Wang, Lei Li, Yong Ren, Wenjing Wang, Yulong Lv, Dhirendra Kataria, Peter Wurz, Walfried Raab, Sylvain Vey, and Marius Echim

The Light Ion Analyzer (LIA) instrument, part of the Solar-wind-Magnetosphere–Ionosphere-link- Explorer (SMILE) mission, is designed to measure the ion velocity distribution function within an energy range of 5 eV up to 25 keV. LIA provides in-situ measurements of the ion velocity distribution functions of the solar-wind and magnetosheath, from which the moments can be derived on ground, serving as an upstream input for the magnetosphere-ionosphere downstream responses. Two identical 2π sr field-of-view LIA instruments are mounted on two opposite sides of the spacecraft platform, offering a combined 4π sr instantaneous field-of-view. Each LIA consists of a top-hat electrostatic analyzer, electrostatic aperture deflectors, and a microchannel plate detector for analyzing the energy, direction, and flux of ions. Depending on operation mode, the angular resolution ranges from 22.5° to 5.625° in elevation and from 30° to 7.5° in azimuth, and the time resolution spans from 0.25 to 2 seconds. This paper describes the design of the LIA, its performance, ground calibration, operation procedures, and resultant data products. 

How to cite: Kong, L., Dai, L., Zhang, A., Nicolaou, G., Berthomier, M., Gao, J., Su, B., Escoubet, P., Wang, C., Li, L., Ren, Y., Wang, W., Lv, Y., Kataria, D., Wurz, P., Raab, W., Vey, S., and Echim, M.: The Light Ion Analyzer (LIA) for SMILE mission: design, ground calibration and data products, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-9904, https://doi.org/10.5194/egusphere-egu25-9904, 2025.

14:10–14:20
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EGU25-1897
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On-site presentation
Rajkumar Hajra, Bruce Tsurutani, Quanming Lu, and Aimin Du

Supersubstorms (SSSs) are intense auroral zone geomagnetic activity associated with extremely intense westward auroral electrojet currents  (SML < -2500 nT). The nightside SSS onsets and auroral evolution were found to be substantially different than the Akasofu (1964) standard picture of auroral development for “typical” substorms. SSSs are the primary causes of intense geomagnetically induced currents (GICs) at the Mäntsälä gas pipeline, Finland, determined from a 21-year data study. From a statistical study of SSSs triggered by interplanetary shocks, during solar cycles 23 and 24, solar wind-magnetosphere energy coupling will be discussed. Magnetospheric shock compression greatly strengthens the upstream interplanetary magnetic field southward component, and thus, through magnetic reconnection at the Earth’s dayside magnetopause, greatly enhances the solar wind energy input into the magnetosphere and ionosphere during the SSS events. The additional solar wind magnetic reconnection energy input supplements the ∼1.5 hr precursor (growth-phase) energy input and both supply the necessary energy for the high-intensity, long-duration SSS events. The major part of the SSS energy is dissipated into Joule heating, distributed equally in the dayside and nightside ionosphere, giving a picture of the global energy dissipation in the magnetospheric/ionospheric system, not simply a nightside substorm effect.

How to cite: Hajra, R., Tsurutani, B., Lu, Q., and Du, A.: Solar wind-magnetosphere energy coupling during supersubstorms, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-1897, https://doi.org/10.5194/egusphere-egu25-1897, 2025.

14:20–14:30
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EGU25-7407
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ECS
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On-site presentation
Shipra Sinha, David Sibeck, Mei-Ching Fok, and Denny Oliveira

Magnetospheric substorms, characterized by the rapid release of energy stored in the magnetotail, play a central role in space weather dynamics. These events are typically triggered by enhanced magnetic reconnection between the Earth’s magnetic field and the interplanetary magnetic field (IMF). While substorms are often associated with southward IMF orientations, studies have also shown that they can occur even during northward IMF conditions, particularly when solar wind pressure pulses or strong IMF By components are present. In these cases, the location of substorm onsets and expansions can occur far from the usual midnight sector.

Notably, while the presence of an IMF By component tends to cause only small shifts in the local time sector of substorm onset (typically between ~22 MLT and ~01 MLT), solar wind pressure pulses can induce much larger shifts, potentially moving substorm onsets as far as the dawn or dusk sectors. This phenomenon suggests that ground-based observations of substorms centered around the dawn or dusk sectors could provide a unique signature of substorms triggered by pressure-induced impulses.

We provide examples of pressure-induced events exhibiting atypical onsets, with plasma splitting and propagating sunward in both pre-and post-midnight sectors. These findings suggest a likely cause for the large shifts in substorm onset locations during pressure pulses. The study highlights the need for further investigation into multiple reconnection sites and the role of solar wind pressure in shaping substorm evolution.

How to cite: Sinha, S., Sibeck, D., Fok, M.-C., and Oliveira, D.: Anomalous Substorm Signatures During Sudden Solar-Wind Pressure Enhancements, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-7407, https://doi.org/10.5194/egusphere-egu25-7407, 2025.

14:30–14:40
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EGU25-15721
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ECS
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On-site presentation
Ahmad Lalti, Jonathan Rae, and Clare Watt

The response of the outer radiation belt to large-scale variations in the solar wind is an active field of research. In this work, we use electron flux measurement from the full 7 years of the Van Allen probes mission along with solar wind properties measurements from the OMNI database at L1 and THEMIS/ARTEMIS spacecraft to investigate how the electron flux in the outer radiation belt responds to variations in the solar wind parameters across temporal scales. We find that electron flux has multiple periodicities correlated with those of the solar wind. At the largest temporal scales, we observe 0.5-year, 27-days, and 13.5-days periodicities which are most prominent near the declining phase of the solar cycle. This is consistent with the Axial Effect where the solar magnetic field is aptly modeled as a tilted dipole and the Earth encounters the fast solar wind at the observed periodicities. In addition, we observe modulations in the electron flux at lower time scales (<= 1 day). The interpretation of the higher frequency periodicity and the study of the effects of various mesoscale structures such as HFAs, foreshock bubbles, and magnetosheath jets, on the electron flux in the outer radiation belt, is still under investigation.

 

How to cite: Lalti, A., Rae, J., and Watt, C.: Solar wind - radiation belt coupling across scales, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-15721, https://doi.org/10.5194/egusphere-egu25-15721, 2025.

14:40–14:50
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EGU25-5806
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On-site presentation
Xiaochao Yang, Lei Dai, and Xu Wang

The Earth's outer radiation contains plenty of high-energy electrons. These electron populations exhibit high dynamics, with their fluxes varying by several orders of magnitude during magnetospheric disturbances. The enhancement of these high-energy electrons greatly increases the likelihood of spacecraft malfunction or failure and significantly influences the solar-terrestrial system's energy and mass coupling, highlighting the importance of fully understanding the mechanisms governing these dynamics from both theoretical and practical perspectives. The radial diffusion acceleration driven by ULF waves and local acceleration due to the interaction with whistler mode chorus waves were proposed to explain the enhancement of the radiation belt high-energy electrons. Recent work indicates that the magnetospheric convection, as a key dynamic process within the Earth's magnetosphere, is closely related to the dynamics of high-energy electrons in the radiation belt. Under fast solar wind conditions, the enhanced magnetospheric convection excites intense substorms, which are thought to induce rapid substorm injections of high-energy electrons, leading to relativistic electron enhancements in the outer radiation belt. Case studies and statistical analyses indicate that these injections predominantly enhance electrons in the range of hundreds of keV to 1-2 MeV beyond L ~ 4. Furthermore, in the plasmasphere, where the loss of radiation belt high-energy electrons has been traditionally believed to be dominant due to wave-particle interaction-induced scattering, we have find remarkable MeV electron enhancements. Our analysis shows that this enhancement is related to the magnetospheric convection. The research results are helpful for deepening the understanding of the formation and evolution mechanisms of high-energy electrons in the radiation belt, and also provide an important theoretical basis for further accurately predicting changes in the radiation belt environment and ensuring the safety of spaceflight activities.

How to cite: Yang, X., Dai, L., and Wang, X.: Enhancements of Radiation Belt High-Energy Electrons Driven by the Magnetospheric Convection, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-5806, https://doi.org/10.5194/egusphere-egu25-5806, 2025.

14:50–15:00
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EGU25-5491
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ECS
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On-site presentation
Rapid Relativistic Electron Enhancements During Van Allen Probes Era
(withdrawn)
Senlin Xiong, Lei Dai, Xu Wang, and Chi Wang
15:00–15:10
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EGU25-13281
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ECS
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On-site presentation
Niklas Grimmich, Pöppelwerth Pöppelwerth, Kevin-Alexander Blasl, Adriana Settino, Rumi Nakamura, Ferdinand Plaschke, Martin O. Archer, and H. Katariina Nykyri

Across the magnetopause, the velocity difference between the magnetospheric plasma and the shocked plasma of the solar wind gives rise to the Kelvin-Helmholtz instability. This instability can develop into large-scale surface waves and vortices at the magnetopause, causing the different plasma regions to mix, which plays an important role in the transfer of energy across the magnetopause. We know from spacecraft observations and simulations that the way Kelvin-Helmholtz waves grow and evolve can be different at dawn and dusk. However, very few studies have directly observed this phenomenon on both flanks of the magnetopause simultaneously. By combining measurements from the THEMIS and Cluster missions, we can report here on an event where such a simultaneous observation of the Kelvin-Helmholtz waves is possible.
    
For this event, we investigate and compare the typical wave parameters and in particular the difference in plasma mixing on the two flanks. The results presented here may help to improve our understanding of the energy transport during Kelvin-Helmholtz intervals, and may also provide new insights into the proposed dawn-dusk asymmetry of these waves.

How to cite: Grimmich, N., Pöppelwerth, P., Blasl, K.-A., Settino, A., Nakamura, R., Plaschke, F., Archer, M. O., and Nykyri, H. K.: Comparison of Kelvin-Helmholtz waves observed simultaneously at the dawn and dusk flanks of the Earth's magnetopause, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-13281, https://doi.org/10.5194/egusphere-egu25-13281, 2025.

15:10–15:20
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EGU25-3066
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On-site presentation
Su-ping Duan, Anxin Zhang, Lei Dai, Yuntian Hou, Zhaohai He, and Chi Wang

Using particle and electromagnetic field data from Magnetospheric Multiscale Spacecraft (MMS), we investigate energetic O+ ion characteristics in the strong velocity shear regions in the dusk-side low-latitude boundary layer (LLBL) during the main phase of an intense storm on 13 October 2016. In the large velocity reversal regions, O+ ion number density is very high, No+ ~ 0.3 cm-3. The pitch angle distributions of these energetic O+ ions vary distinctly across different energy ranges. The pitch angles of the lower energetic (3 keV to 10 keV) O+ ions are mostly less than 45 degrees and show a quasi-parallel distribution. Conversely, the pitch angles of the higher energetic (20 keV to 40 keV) O+ ions are dominantly in the range from 45 to 135 degrees, suggesting a quasi-perpendicular distribution. The quasi-parallel distribution of lower energetic O+ ions implies that these O+ ions are outflow along the magnetic field line from the dayside high-latitude ionosphere. Intense electric fields in the strong shear flow region can accelerate O+ ions to higher energy, altering their motion from along the magnetic field to the transverse direction in the dusk-side LLBL. Our studies present evidence for strong shear flow in the dusk-side LLBL driving energetic O+ ions to traverse the magnetic field motion. The quasi-perpendicular distribution of higher energetic O+ ions, in the inner edge of the dusk-side LLBL, may provide a new source of ring current energetic particles during the main phase of the intense storm.

How to cite: Duan, S., Zhang, A., Dai, L., Hou, Y., He, Z., and Wang, C.: Observations of energetic O+ ions with strong velocity shear in the low latitude boundary layer during an intense storm main phase, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-3066, https://doi.org/10.5194/egusphere-egu25-3066, 2025.

15:20–15:30
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EGU25-9713
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On-site presentation
Kristina Kislyakova, Yury Sasunov, Yanina Metodieva, Colin Johnstone, Helmut Lammer, and Manuel Scherf

Atmospheric loss processes together with sources and sinks at the surface govern the evolution of the atmospheric composition. At present-day Earth, the main dominant escape process is polar wind, which predominantly removes ionized oxygen atoms from the polar regions of the Earth. Although a multitude of observations that cover atmospheric escape for different activity conditions of the Sun exist, theoretical and numerical aspects of the polar outflow are still not entirely understood.

 

In this work, we investigate the role different magnetospheric conditions play in governing the polar wind escape rates from the Earth. We use the Space Weather Modeling Framework and the BATS-R-US code to determine the magnetospheric structure in the polar areas of the Earth for quiet and storm conditions. The code output includes the configuration of the magnetic field in the vicinity of an exoplanet (using the Solar Corona and Inner Heliosphere modules) for a given stellar magnetic field and plasma parameters in the vicinity of the planet. The code offers significant flexibility and allows to study a wide range of quiet and storm conditions.

 

Using the magnetic and electric fields distributions calculated with the SWMF, we apply the test particle approach to track individual ions along the magnetic field lines and collect static on atmospheric ions that are lost. Depending on their energy, cold ions can end up in different regions of the magnetosphere, such as the magnetopause, the distant tail, and the ring currents, or fall down to the atmosphere. The idea of the test particle approach is to numerically calculate the trajectory of independent and non-interacting charged/uncharged particles, where external forces are well known. Particularly, for applications of the test particle approach for planetary magnetospheres it is common to use the magnetic and electric fields from global models such as the SWMF. To obtain a general picture of the percentage of particles that escape, we will study multiple test particles with different parameters such as initial energies, locations, and pitch angles (that can be inferred from the DSMC model) to accumulate statistics. As a result, we will obtain the distribution of locations, speeds and final destinations of ions in magnetospheres and/or ionospheres of planets. One of the main advantages of the test particle approach is that it avoids very expensive calculations (in terms of computational time and computer resources) and at the same time can reproduce the main features of the studied phenomena.

 

We show that magnetospheric parameters together with the current solar conditions play an important role for atmospheric escape. We discuss the influence of atmospheric loss processes on the Earth’s atmosphere over it’s history, and discuss the importance of preexisting modeling for stellar missions such as the SMILE satellite (Solar wind Magnetosphere Ionosphere Link Explorer).

How to cite: Kislyakova, K., Sasunov, Y., Metodieva, Y., Johnstone, C., Lammer, H., and Scherf, M.: Escape of ions from Earth under various magnetospheric conditions, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-9713, https://doi.org/10.5194/egusphere-egu25-9713, 2025.

15:30–15:40
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EGU25-1362
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ECS
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On-site presentation
Manu Varghese, Jijin Raj, Balan Nanan, Qinghe Zhang, and Zanyang Xing

The important early positive part of main phase (MP) from positive main phase onset (MPO) to 0‑level of SYM-H (and Dst, up to over 200 nT) was somehow missed in the treatment of geomagnetic storms. In this paper, we include the missed positive part in MP for over 1000 (out 1360) storms (SYM-HMin ≤-25 nT) having positive MPO identified in the SYM-H index in 1981-2024 by a computer algorithm using 5 selection criteria. The missed part is included by raising the 0-level of SYM-H to MPO-level, which increases the revised storm intensity (SYM-HMinr) by up to -145 nT and revised storm impulsive strength (IpsSYM-Hr) by up to -139 nT. The inclusion of the positive part of MP therefore seems important for all aspects of global space weather. For example, IpsSYM-Hr identifies all 3 severe space weather (SvSW) events that caused power outage with a large separation of 52 nT and identifies all 9 minor-system-damage space weather (MSW) events that caused capacitor stripping and high induced voltage in power transformers from over 1000 normal space weather (NSW) events that did not cause any such damages since 1981. The included positive part of MP is explained statistically using long-term simultaneous SYM-H, solar wind dynamic pressure P and Y-component of interplanetary electric field IEFy (or VBz computed from solar wind velocity V and Bz component of IMF) data available for 156 storms since 1998. In addition, a 1-minute resolution SYM-H model developed from the existing Dst models is used to investigate the combined and relative contributions of P and IEFy on the included positive part of MP. The data statistics and model results reveal that the positive part of MP in majority (74%) of storms is contributed mainly (≥75%) by positive IEFy or increase in ring current; in a small number (6%) of storms, it is contributed mainly (≥75%) by sudden decrease in P; and in the remaining 20% of storms, it is contributed by both decrease in P and positive IEFy with major contribution from positive IEFy. In short, the important positive part of MP is caused mainly by the increase in ring current.

How to cite: Varghese, M., Raj, J., Nanan, B., Zhang, Q., and Xing, Z.: Including and explaining the important early positive part of main phase in the treatment of geomagnetic storms, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-1362, https://doi.org/10.5194/egusphere-egu25-1362, 2025.

Coffee break
Chairpersons: Yiqun Yu, Yukitoshi Nishimura, Lei Dai
16:15–16:25
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EGU25-7633
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On-site presentation
Fei He, Yong-Mei Wang, Xiao-Xin Zhang, Xiao-Hong Liu, Guo-Jun Du, Jing-Hua Mao, Peng-Da Li, Wei-Peng Huang, Tian-Fang Wang, Jiu Liu, Shui Yu, Zi-Yue Wang, Jing Li, Lei Li, Lei Dai, Sylvain Vey, Rene Berlich, Colin Forsyth, Christophe Philippe Escoubet, and Chi Wang

The aurora is the optical manifestation of the global magnetospheric dynamics. Optical imaging of aurora provide insight into the large-scale convections and wave-particle interactions in the magnetosphere, thus provide important information on the mass and energy flow in the solar wind-magnetosphere coupling system. The Ultraviolet Imager (UVI) onboard the Solar wind Magnetosphere Ionosphere Link Explorer (SMILE) satellite will image the entire auroral oval in N2 Lyman-Birge-Hopfield (LBH) band (160–180 nm) while effectively mitigating contamination from dayglow, achieving a spatial resolution of approximately 100 km or better. The SMILE spacecraft operates in a highly eccentric orbit characterized by an orbital period of approximately 50 hours. This orbit configuration is particularly well-suited for long-term continuous monitoring of northern auroras. Such insights will significantly enhance our research into energy deposition processes occurring within the ionosphere and upper atmosphere during solar wind-magnetosphere interactions. Here, we will introduce in detail the instrument, laboratory calibrations, in-flight calibration plan, and data products of SMILE UVI.

How to cite: He, F., Wang, Y.-M., Zhang, X.-X., Liu, X.-H., Du, G.-J., Mao, J.-H., Li, P.-D., Huang, W.-P., Wang, T.-F., Liu, J., Yu, S., Wang, Z.-Y., Li, J., Li, L., Dai, L., Vey, S., Berlich, R., Forsyth, C., Escoubet, C. P., and Wang, C.: The Ultraviolet Imager (UVI) for SMILE mission: Instrument, Calibration, and Products, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-7633, https://doi.org/10.5194/egusphere-egu25-7633, 2025.

16:25–16:35
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EGU25-13216
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ECS
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On-site presentation
Abiyot Workayehu, Minna Palmroth, Liisa Juusola, Markku Alho, Konstantinos Horaites, Maxime Grandin, Venla Koikkalainen, Ivan Zaitsev, Yann Pfau-Kempf, Urs Ganse, Markus Battarbee, and Jonas Suni

Bursty Bulk Flows (BBFs) are high-speed plasma flows that occur within the magnetotail plasma sheet. BBFs are known to play a crucial role in transporting energy, mass, and magnetic flux across the magnetotail, as well as to the coupled ionosphere. Understanding the ionospheric signatures of BBFs is therefore essential to advance our understanding of the coupling processes between the Earth’s magnetosphere and ionosphere. Currently, most insights into the ionospheric signatures of BBFs come from individual case studies that include simultaneous observations of BBFs in the magnetotail and field-aligned currents (FACs) in the nightside ionosphere. In this study, we utilized the 6D Vlasiator simulations to study the ionospheric signatures of BBFs in the near-Earth magnetotail. Vlasiator is a global hybrid-Vlasov model designed to simulate near-Earth space plasmas and has recently been complemented with an ionosphere model, allowing the study of magnetosphere-ionosphere coupling.

In the magnetotail, the simulation results show that a BBF with Vx ≥400,km/s emerges shortly after magnetic reconnection occurs on the dusk-side at a radius between 11 and 14 RE (where RE= 6371 km, radius of the Earth) in the current sheet plane. As the BBF moves Earthward and azimuthally dusk-ward (as seen from above the current sheet plane), clockwise (counterclockwise) flow vortices are induced on the dawn(dusk) sides of it. These vortical flows generate FACs flowing upward (out of the current sheet plane) on the dawn-side and downward (into the current sheet plane) on the dusk-side flanks, respectively.

The mapping of BBF structures onto the ionosphere shows that BBFs are primarily aligned in the East-West direction, with their ionospheric signatures appearing as enhancements in FACs, ionospheric conductances, horizontal ionospheric currents, and the formation of localized plasma flow channels. The upward and downward FACs associated with BBFs in the magnetotail consistently map to enhanced Region 2 (R2) and Region 1 (R1) FAC structures at ionospheric altitude, which are then closed in the ionosphere by north-west flowing Pedersen currents. The Earthward motion of the BBF maps to an equator-ward flow channel, while the dusk-side counterclockwise (and dawn-side clockwise) magnetotail vortical flows correspond to evening-side clockwise (and midnight-side counterclockwise) flow channels in the ionosphere. Overall, the Vlasiator simulation results show that the emergence of BBFs in the near-Earth magnetotail drives enhancements in the currents and conductances of the nightside ionosphere, while the westward drift of these enhanced structures corresponds to the dusk-ward movement of BBFs in the magnetotail.

How to cite: Workayehu, A., Palmroth, M., Juusola, L., Alho, M., Horaites, K., Grandin, M., Koikkalainen, V., Zaitsev, I., Pfau-Kempf, Y., Ganse, U., Battarbee, M., and Suni, J.: Ionospheric signatures of Bursty Bulk Flows in the 6D Vlasiator simulations, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-13216, https://doi.org/10.5194/egusphere-egu25-13216, 2025.

16:35–16:45
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EGU25-14291
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On-site presentation
Nozomu Nishitani, Tomoaki Hori, Keisuke Hosokawa, Atsuki Shinbori, Yuki Obana, Mariko Teramoto, Kazuo Shiokawa, and Ryuho Kataoka

With increasing solar activity, both auroral precipitation region and ionospheric convection of high-latitude proper expand to lower geomagnetic latitudes, leading to difficulties in monitoring the disturbances using the pre-existing observation instruments designed for high-latitude ionospheric dynamics. The Super Dual Auroral Radar Network (SuperDARN) was originally developed for studying high-latitude phenomena, but since the early 2000s, it has expanded toward lower geomagnetic latitudes, enabling the monitoring of sub-auroral and mid-latitude phenomena. The SuperDARN Hokkaido Pair of (HOP) radars, operated by Nagoya University, Japan, are located at the lowest geomagnetic latitude (=36.9 AACGM geomagnetic latitude and are most suitable for monitoring the ionospheric and magnetospheric dynamics during geomagnetic storms including recent huge storms such as the May 2024 storm. In this paper, we report the spatial and temporal evolution of ionospheric convection associated with the auroral precipitation during huge geomagnetic storms using the SuperDARN HOP radars data, together with ground-based camera data and the particle precipitation data at Low-Earth Orbit (LEO) satellites. The majority of low latitude auroral precipitation is accompanied by the sheared zonal ionospheric flows in its vicinity, but detailed flow patterns vary from event to event. Details of the multi-event analysis result will be presented.

How to cite: Nishitani, N., Hori, T., Hosokawa, K., Shinbori, A., Obana, Y., Teramoto, M., Shiokawa, K., and Kataoka, R.: A study of ionospheric convection pattern in the vicinity of low latitude auroral precipitation during huge geomagnetic storms, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-14291, https://doi.org/10.5194/egusphere-egu25-14291, 2025.

16:45–16:55
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EGU25-12276
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Virtual presentation
Shun-Rong Zhang, Philip Erickson, Anthea Coster, and Larisa Goncharenko

An international campaign that encompassed diverse arrays of ground observations, including incoherent scatter radars and observational chains around the 60W~120E Meridian Circle, during the 10-11 Oct 2024 superstorm, was conducted to observe global upper atmospheric responses. This superstorm was driven by the arriving ICMEs which were associated with several solar eruptions on 7 and 8 Oct, 2024, respectively. Significant geomagnetic disturbances were observed as solar wind speeds elevated from 400 km/s to 800km/s, Bz turned southward reaching -24 nT initially then -41 nT at 22 UT on 10 Oct. SymH dropped to a minimum of 330 nT and Kp was above 8- for 21 hours which provided opportunities to watch spectacular auroras over around the world. These conditions triggered multi-scale global ionospheric disturbances. These disturbances are characterized by the sudden onset of the ionospheric perturbations in GNSS TEC observations, and the immediate launch of traveling ionospheric disturbances which propagated both equatorward into low latitudes (sometimes into the other hemisphere), and poleward across the polar cap from dayside to nightside. Subauroral disturbances exhibited characteristic storm-enhanced density (SED) plumes in the American longitudes, which convected sunward from dusk to noon and entered the cusp region contributing to the polar cap Tongue of Ionization (TOI) structure. Substantial equatorial ionization anomaly (EIA) poleward extension contributing to the density enhancement at the low latitude base of SED. A significant density depletion channel spanning between midlatitudes over the two hemispheres was found, accompanying the equatorial plasma bubble (EPB) development. This presentation provides a quick overview of the key observations with a focus primarily on TEC global responses.

How to cite: Zhang, S.-R., Erickson, P., Coster, A., and Goncharenko, L.: Global ionospheric disturbances during the 10-11 Oct 2024 superstorm, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-12276, https://doi.org/10.5194/egusphere-egu25-12276, 2025.

16:55–17:05
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EGU25-20463
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On-site presentation
Yue Deng, Cheng Sheng, William Bristow, Yukitoshi Nishimura, and Mark Conde

Techniques developed in the past few years enable the derivation of multi-scale regional ion convection and particle precipitation patterns from the Super Dual Auroral Radar Network (SuperDARN) and Time History of Events and Macroscale Interactions during Substorms (THEMIS) All-Sky Imager (ASI) observations, respectively. Our previous simulations driven by these multi-scale geomagnetic forcing suggest that both meso-scale ion convection and particle precipitation can intensify ionospheric and thermospheric disturbances with prominent structures and notable magnitudes. In this study, the global ionosphere–thermosphere model (GITM) is utilized to simulate the March 27th, 2014 substorm event, and simulated F-region neutral winds have been compared with scanning Doppler imagers (SDI) wind measurements at Toolik Lake (68.6°N, 149.6°W). Neutral wind variations have been further separated into large (>500 km) and meso (<500) scales. The correlation between meso-scale ion-convection and neutral wind in a localized region has been qualified through the vortices and the speed. The meso-scale neutral wind response and ramp-up time show a strong dependence on the geomagnetic conditions.

How to cite: Deng, Y., Sheng, C., Bristow, W., Nishimura, Y., and Conde, M.: F-region Neutral Wind Response to the Multi-scale Geomagnetic Forcing During the March 27th, 2014 Substorm Event , EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-20463, https://doi.org/10.5194/egusphere-egu25-20463, 2025.

17:05–17:15
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EGU25-12469
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On-site presentation
Bea Gallardo-Lacourt, Yukitoshi Nishimura, Larry Kepko, Emma L. Spanswick, D. Megan Gillies, David J. Knudsen, Johnathan K. Burchill, Susan H. Skone, Victor A. Pinto, Darren Chaddock, Jeremy Kuzub, and Eric F. Donovan

Strong Thermal Emission Velocity Enhancement (STEVE) is a fascinating optical phenomenon typically observed in the mid-latitude ionosphere. Recent observations reveal an exceptional STEVE event occurring at high latitudes, approximately 10 degrees poleward of previously documented cases. This event, recorded in Yellowknife, Canada, by a TREx RGB imager and a citizen scientist, coincided with Swarm satellite measurements of extreme westward ion drift velocities exceeding 4 km/s. Such velocities are generally associated with subauroral regions at mid-latitudes, making this high-latitude occurrence particularly striking.
Notably, this event unfolded in the absence of a substorm, a departure from previous STEVE and extreme drift velocity observations. High-latitude radars detected rapid equatorward ionospheric flows, while GOES satellites recorded no particle injections, suggesting a highly inflated inner magnetosphere.
This unique case study challenges existing paradigms of subauroral dynamics and highlights the significant influence of magnetospheric configurations on ionospheric responses. In this talk, we will discuss the characteristics of this event and examine the associated solar wind, magnetosphere, and ionosphere interactions.

How to cite: Gallardo-Lacourt, B., Nishimura, Y., Kepko, L., Spanswick, E. L., Gillies, D. M., Knudsen, D. J., Burchill, J. K., Skone, S. H., Pinto, V. A., Chaddock, D., Kuzub, J., and Donovan, E. F.: Unexpected STEVE Observations at High Latitude During Quiet Geomagnetic Conditions, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-12469, https://doi.org/10.5194/egusphere-egu25-12469, 2025.

17:15–17:25
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EGU25-15218
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ECS
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On-site presentation
Boyi Wang, Yuda Zhi, Xinyu Xu, Yukitoshi Nishimura, Primož Kajdic, Yi Wang, and Xueshang Feng

Field-aligned currents (FACs) can be generated in the magnetosphere due to dynamic pressure variations associated with foreshock transients. The mechanisms may include: a) compressions or rarefactions causing divergence or convergence of diamagnetic or inertial currents in the magnetosphere, and b) compressions or rarefactions exciting shear Alfvénic waves associated with FACs. However, whether these FACs can further affect ions and neutral particles in the coupled ionospheric-thermospheric system remains unclear.

In this study, we utilized coordinated observations from THEMIS probes, (near-)polar-orbiting satellites (DMSP and SWARM), and ground-based optical imaging to identify FACs induced by foreshock transients and investigate their effects on ions and neutral particles. Ground-based all-sky imagers show that foreshock transients can generate traveling convection vortices (TCV) auroras near the equatorial boundary of the auroral oval and field line resonance (FLR) arcs at relatively lower latitudes. Events with conjugate DMSP observations reveal that the corresponding upward FACs were associated with ionospheric ion outflows, Poynting fluxes, and low-energy electron precipitation. Events with conjugate SWARM and optical observations indicate that these FACs were also associated with neutral wind divergence at ~250 km and enhanced neutral density at SWARM altitudes. This suggests that energy heating from foreshock-induced FACs can cause neutral wind perturbations and elevate neutral particles to higher altitudes.

How to cite: Wang, B., Zhi, Y., Xu, X., Nishimura, Y., Kajdic, P., Wang, Y., and Feng, X.: Field-aligned currents induced by foreshock transients and their effects on ions and neutral particles, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-15218, https://doi.org/10.5194/egusphere-egu25-15218, 2025.

17:25–17:35
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EGU25-410
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ECS
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Virtual presentation
|
Yunfang Zhong and Hui Wang

Using Challenging Minisatellite Payload and the Republic of China Satellite-1 observations, the response of ionospheric radial current (IRC) in the F region to the enhancement of merging electric field (Em) at different magnetic local times (MLT) is investigated. Possible physical mechanisms are discussed in terms of neutral wind, conductivity, and prompt penetration electric field (PPEF). The disturbance IRC (ΔIRC) increases in the upward (downward) direction in the daytime (nighttime) within 3 h after Em enhancement. However, disturbance zonal winds increase westward (eastward) at 12–18 MLT (00–06 MLT). The reduced F region electron density may help weaken IRC at 06–12 MLT and 18–24 MLT. This work indicates that the daytime eastward (nighttime westward) PPEF drives equatorward (poleward) Hall current at low latitudes, resulting in both upward (downward) ΔIRC and eastward (westward) plasma drift at the F region magnetic equator.

How to cite: Zhong, Y. and Wang, H.: Responses of Ionospheric F layer Radial Current to the Enhanced Solar Wind Input, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-410, https://doi.org/10.5194/egusphere-egu25-410, 2025.

17:35–17:45
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EGU25-3419
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ECS
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On-site presentation
Shreedevi Porunakatu Radhakrishna, Yoshizumi Miyoshi, Yiqun Yu, and Vania Jordanova

The dusk-side mid-latitude ionosphere is characterized by fast, sunward flow channels of a few degrees in width, known as Subauroral Polarization Streams (SAPS). Occasionally, these regions exhibit distinct, latitudinally narrow enhancements in velocity, referred to as double-peak Sub-auroral Ion Drifts (DSAIDs). SAPS are associated with Region 2 Field-Aligned Currents (R2 FACs) that flow into the low-conductance sub-auroral ionosphere, while DSAIDs have been linked to the presence of a double-conductance trough in this region. Nishimura et al. (2022) demonstrated that sub-auroral ion drifts intensify in the presence of electromagnetic waves, with local plasma structures exerting greater control over the velocity characteristics of these westward flows than solar wind or global magnetospheric conditions. This study investigates the occurrence of westward ion flows in the dusk-side sector during a geomagnetic storm event, utilizing simulations from the RAM-SCB model. To explore the relationships between R2 FACs, electric fields, EMIC wave-particle interactions, proton precipitation, ionospheric conductance, and westward flows in the dusk-side sub-auroral ionosphere, we conducted two simulation studies, one with and one without EMIC waves. The simulations confirmed that EMIC wave-induced proton precipitation leads to localized enhancements in conductivity, which, in turn, generates high-speed westward flows in the dusk-side sub-auroral ionosphere. Our findings reveal the significant role of wave-particle interactions in shaping ionospheric behavior during disturbed conditions.

How to cite: Porunakatu Radhakrishna, S., Miyoshi, Y., Yu, Y., and Jordanova, V.: Westward ion drifts in the dusk-side sub auroral ionosphere: Role of EMIC wave-particle interactions, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-3419, https://doi.org/10.5194/egusphere-egu25-3419, 2025.

17:45–17:55
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EGU25-2476
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Virtual presentation
Zhaohai He, Jiyao Xu, Lei Dai, Suping Duan, Hong Gao, Guojun Wang, Ilan Roth, and Chi Wang

Previously we found that the inner radiation belt (IRB) shrinks and stretches in solar minimum and maximum. A natural problem comes up that how solar cycle effects the near-Earth space regions including plasmasphere, IRB, ionosphere, mesosphere and lower thermosphere (MLT). We present a thorough analysis of the extent of solar cycle effect on four regions by using mesospheric and thermospheric geopotential height and temperature from SABER on TIMED, ionospheric hmF2 from Chinese Meridian Project, high-energy protons in IRB and electron density in plasmasphere from Van Allen Probes within 2013-2018 intervals. By analyzing evolutions of these quantities, we find that entire IRB, ionosphere and MLT region shrink at solar minimum and stretch at solar maximum by ~103 km, 50~102 km and 1 km scales, respectively, while plasmapause shows an opposite trend. Fourier spectra of these quantities have been investigated by Lomb–Scargle periodogram. The mid-term periodic oscillations (13.5-day, 45-day, and 52-day) have been observed in MLT region, matching well with plasmapause locations and geomagnetic indices, which have not been observed in solar EUV radiation and IRB. This may indicate that those oscillations facilitate energy exchange and mass transportation between MLT region and plasmasphere due to magnetic storms and substorms. The oscillation periods of higher energy (102.6MeV) in IRB have not been observed in MLT region except for annual variations. The impact of higher energy protons on MLT regions may not be significant, although they could penetrate deeper into MLT region. Our results reveal relationships between some quantities and solar cycle multi-scale modulation, which may provide assistance and monitors for mass transportation in the near-Earth space regions.

How to cite: He, Z., Xu, J., Dai, L., Duan, S., Gao, H., Wang, G., Roth, I., and Wang, C.: Solar Activity Effects on the Near-Earth Space RegionsDuring the Descending Phase of Solar Cycle 24, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-2476, https://doi.org/10.5194/egusphere-egu25-2476, 2025.

Posters on site: Tue, 29 Apr, 10:45–12:30 | Hall X4

Display time: Tue, 29 Apr, 08:30–12:30
Chairpersons: Lei Dai, C.-Philippe Escoubet, Yiqun Yu
X4.42
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EGU25-4762
Tonghui Wang and Lei Dai

The sudden increase in high latitude ionospheric currents and two-cell convection are both important elements during geomagnetic substorms. Although simulations and statistical analyses suggest a relationship between the two phenomena in magnetosphere-ionosphere coupling, the spatiotemporal correlation of their evolution in observation has not been clearly demonstrated. Here we select multiple continuous strong substorms under a strong geomagnetic storm as a case to effectively reveal the synchronous evolution of field-aligned currents (FACs) and auroral electrojets with convection. The observation results indicate that the bidirectional convection activity between the dayside and nightside-driven affects to multiple "V" shaped movements of dawnside FACs on magnetic local time (MLT), and continuously changes the magnetic latitude (MLAT) difference of nightside FACs. Meanwhile, the dawn-dusk asymmetry of convection further affects the different evolutionary characteristics of the east-westward electrojets. These results demonstrate a strong coupling between convection and ionospheric currents, underscoring the pivotal role of convection in the progression of substorm phases.

How to cite: Wang, T. and Dai, L.: Convection driven field-aligned currents and auroral electrojets during continuous strong substorms, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-4762, https://doi.org/10.5194/egusphere-egu25-4762, 2025.

X4.43
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EGU25-5032
Xu Wang, Lei Dai, Yong Ren, Senlin Xiong, and Chi Wang

Earth's outer radiation belts are highly dynamic during geomagnetic storms. Using electron flux  data from 226 keV to 2.6 MeV measured by the Van Allen Probes, we statistically analyzed the peak flux position (Lpeak)  and inner boundary position (Lmin) of the outer radiation belt across different storm phases: pre‐storm quiet time, main phase, early recovery phase, and later recovery phase. This analysis covered 196 geomagnetic storm events from October 2012 to September 2019. Our results indicate that: (a) During the pre‐storm, Lpeak decreases with increasing energy. From the pre‐storm to the early recovery phase, Lpeak shifts inward for energies below 1 MeV and outward for energies above 1 MeV. For all energies, Lpeak converges to approximately L =∼ 4.3–4.6 in the early recovery phase. (b) Below approximately 1 MeV, Lmin generally move inward from the main phase to the early recovery phase. Above 1 MeV, Lmin remains nearly unchanged across different storm phases. (c) The half‐width (Lpeak-Lmin) of the outer belt decreases during the main phase for energies below 1 MeV and increases during the recovery phase for energies above 1.5 MeV. (d) In the early recovery phase, Lpeak and Lmin at 593–742 keV show a moderate correlation with storm intensity (∣CC∣∼0.7–0.8), while Lpeak and Lmin at energies greater than 1.1 MeV exhibit low correlations (∣CC∣≤∼0.4) during each phase. These results confirm the complex,energy dependent morphology of the outer radiation belt throughout geomagnetic storm phases.

How to cite: Wang, X., Dai, L., Ren, Y., Xiong, S., and Wang, C.: The Evolution of Earth's Outer Radiation Belt Over  Geomagnetic Storm Phase in Van Allen Probe Era, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-5032, https://doi.org/10.5194/egusphere-egu25-5032, 2025.

X4.44
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EGU25-5057
Yong Ren and Lei Dai
Understanding electron kinetic processes is crucial for elucidating the energy conversion mechanisms in magnetic reconnection. Non‐Maxwellian electron distributions are strong indicators of kineticscale processes near the electron diffusion region, yet they remain incompletely understood. Using in‐situ spacecraft data from 29 magnetopause reconnection events, we unambiguously identify a non‐Maxwellian capsule electron distribution near the electron diffusion region. This distribution comprises an elongated component parallel with the magnetic field at lower energies and a butterfly component (with peaks at pitch angles near 45° and 135°) at higher energies. We provide evidence that these distributions are partly linked to
electron trapping and preferential heating along the direction of magnetic fields. The parallel electric potentials needed for the parallel heating may be linked to kinetic Alfvén waves. These capsule‐like electron distributions are also found to generate whistler emissions. Our results suggest that these kinetic processes are prevalent in magnetic reconnection.

How to cite: Ren, Y. and Dai, L.: Capsule Electron Distributions Near the Diffusion Region of Magnetic Reconnection, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-5057, https://doi.org/10.5194/egusphere-egu25-5057, 2025.

X4.45
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EGU25-4746
Kailai Wang, Lei Dai, Shan Wang, Yong Ren, Minghui Zhu, Chi Wang, Benoit Lavraud, Christopher Philippe Escoubet, and James L. Burch

Magnetic reconnection converts magnetic energy into particle energy, with ion outflows serving as a prominent manifestation, particularly in geospace. However, ion processes and signatures related to energy conversion remain incompletely understood in collisionless magnetic reconnection. In this study, we analyze in-situ data and simulations to identify a distinct signature in the off-diagonal component of the ion pressure tensor. This signature displays a bipolar reversal that correlates with ion outflows across the reconnection X-line. The bipolar signal reflects distorted velocity distributions during ion acceleration. The primary cause of this distortion is partial cyclotron motion around the reconnected magnetic field, combined with the acceleration by reconnection electric fields. Hall electric fields further enhance this cyclotron motion by inducing dawnward ion motion as ions enter the current layer from the inflow region. The bipolar reversal in the off-diagonal ion pressure term is a candidate for supporting ion-scale reconnection electric fields.

How to cite: Wang, K., Dai, L., Wang, S., Ren, Y., Zhu, M., Wang, C., Lavraud, B., Escoubet, C. P., and Burch, J. L.: Off-diagonal Ion Pressure Term in Collisionless Magnetic Reconnection, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-4746, https://doi.org/10.5194/egusphere-egu25-4746, 2025.

X4.46
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EGU25-5715
Xiyu Liu, Yiqun Yu, Jiaojiao Zhang, Longxing Ma, Tao Yan, Depeng An, Longhui Liu, Jinbin Cao, and Chi Wang

Large-scale current systems are often disturbed during geomagnetically active time. Based on previous simulations, our work proposes that except for the substorm current wedge (SCW) that connects tail current to ionosphere via a pair of Region-1 sense field-aligned currents (FACs), there exists another wedge-shaped current structure in the nightside current system during substorms, connecting the ring current to the ionosphere. We refer to this structure as the ring current wedge (RCW). The RCW is difficult to be distinguished from the SCW using observations from ground-based magnetometer stations because of their similarity and close distribution in latitude. Furthermore, due to its shorter duration compared to SCW, RCW is often overlooked in previous studies. In this paper, we use global MHD simulations to investigate the storm event on December 1, 2023, in which the IMF Bz reversal from ~+5 nT to ~-25 nT, providing favorable conditions for magnetotail reconnection. During a strong substorm injection, both tail current and ring current were interrupted in midnight sector, forming distinct SCW and RCW structures that lasted for ~30 minutes. Additionally, by superposing SuperDARN global convection images with AMPERE-derived FACs, a reversed, counter-clockwise convection cell was observed at mid-latitudes in the duskside ionosphere, as expected to be formed between SCW and RCW. The reverse convection confirmed that SCW and RCW are different current structures.

How to cite: Liu, X., Yu, Y., Zhang, J., Ma, L., Yan, T., An, D., Liu, L., Cao, J., and Wang, C.: Ring current wedge in nightside during substorms, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-5715, https://doi.org/10.5194/egusphere-egu25-5715, 2025.

X4.47
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EGU25-6385
C.-Philippe Escoubet and the Cluster-MMS team

Various mechanisms have been proposed to explain magnetosheath High Speed Jets (HSJs), such as bow shock ripples, solar wind discontinuities, foreshock transients, pressure pulses, nano dust clouds or shock reformation. It is however difficult to directly associate these mechanisms to HSJs due to the lack of simultaneous measurements at key locations, near the bow shock and both upstream and downstream of it.  We will use a special Cluster campaign, where Cluster 1 was lagged 5 hours behind Cluster 2 and 8 hours behind Cluster 3/Cluster 4 (with separation distances ranging of 3.8 RE and 5.1 RE respectively), to obtain near-Earth solar wind measurements upstream of the bow shock, together with simultaneous measurements in the magnetosheath. The event of interest is first observed by ACE on 13 January 2019, around 07:30 UT, as a short 20-minute period of large IMF-Bx (with a cone angle around 140 deg.). This large IMF-Bx period is also observed, one hour later, by THEMIS B and C (ARTEMIS) and Geotail, which were at 60 and 25 RE from Earth on the dawn side. Cluster 1 and Cluster 2 just upstream of the bow shock, at 17 RE from Earth, observed also such large IMF-Bx period together with energetic ions reflected from the bow shock and Hot Flows Anomalies (HFAs) at the beginning and end of the large IMF-Bx interval. Finally, Cluster 3 and 4 and MMS1-4, a few RE from each other downstream of the shock, observed HSJs embedded in a turbulent magnetosheath for 15 minutes around 08:30 UT. In the first part of the interval, Cluster 3/4 and MMS1-4 observed five HSJs quasi-simultaneously and in the second part, Cluster 3/4 observed three HSJs and MMS only one. The end of the first part is associated with an increase of the magnetic field at MMS in the magnetosheath and upstream in the foreshock at Cluster and Geotail. ACE observed a discontinuity where IMF-By becomes dominant for a few minutes in the middle of the large IMF-Bx interval. These observations will be discussed as possible additional HFA or short, large-amplitude magnetic structure (SLAMS). Ground-based observations from all-sky imager at Yellow River Station and the magnetometer data from SuperMAG showed diffuse auroral brightening and Pc5 ULF waves during the observations of magnetosheath HSJs.

How to cite: Escoubet, C.-P. and the Cluster-MMS team: Hot flow anomalies and magnetosheath high speed jets observed by Cluster and MMS during a Cluster large separation campaign , EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-6385, https://doi.org/10.5194/egusphere-egu25-6385, 2025.

X4.48
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EGU25-8392
Lei Dai, Yimin Han, Chi Wang, Shuo Yao, Gonzalez Walter, Suping Duan, Benoit Lavraud, and Yong Ren

Using solar-wind-magnetosphere-ionosphere conjunction observations, we investigate the geomagnetic responses to fluctuating IMF Bz from interplanetary Alfven waves. Interplanetary Alfven waves transmit intensified IMF Bz to the magnetosheath, leading to intervals of large magnetic shear angles across the magnetopause and magnetopause reconnection. Such intervals are promptly followed by hundreds of nT increases in AE/AU index within 10-20 min. These observations are confirmed in multiple events in corotating interaction region (CIR)-driven geomagnetic storms. To put the observations into context, we propose a phenomenological model of strongly-driven magnetosphere convection/substorm (Dai et al.,2023). The substorm electrojet is linked to the enhanced magnetopause reconnection in the short timescale of re-establishing the ionosphere electric field and the two-cell convection. The substorm expansion may reslut from magnetosphere convection driven by dayside reconnection (Dai et al.,2024). Implications for the upcoming SMILE mission will be discussed.

How to cite: Dai, L., Han, Y., Wang, C., Yao, S., Walter, G., Duan, S., Lavraud, B., and Ren, Y.:  Geoeffectiveness of Interplanetary Alfven waves: Unsteady Magnetopause Reconnection and Directly-Driven Substorms, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-8392, https://doi.org/10.5194/egusphere-egu25-8392, 2025.

X4.49
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EGU25-10464
Nigang Liu

Aurora, a natural light display in the Earth’s upper atmosphere, is produced by the interactions between downward-transiting electrons and atmospheric molecules. Like other geospace phenomena, aurora fundamentally depends on solar wind activity. However, directly testing this relationship has been challenging due to observational limitations. In this study, using observations from solar wind, the magnetosphere, the ionosphere, and the ground, we show that an interplanetary shock can trigger lower-band chorus waves in the magnetosphere. These waves subsequently drive magnetospheric electron precipitation and the diffuse aurora phenomenon. Our findings highlight diffuse aurora as a significant manifestation of the solar wind–magnetosphere–ionosphere coupling process.

How to cite: Liu, N.: Shock-induced diffuse aurora from electron scattering by chorus waves, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-10464, https://doi.org/10.5194/egusphere-egu25-10464, 2025.

X4.50
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EGU25-13176
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Highlight
Tuija Pulkkinen, Timothy Keebler, Yuxi Chen, and Xiantong Wang

To capture physics in global, meso, and kinetic-scales, the Magnetohydrodynamics with Adaptively Embedded Particle-In-Cell (MHD-AEPIC) model couples the FLexible Exascale Kinetic Simulator (FLEKS) particle-in-cell (PIC) code with the Space Weather Modeling Framework (SWMF) global MHD simulation of Earth’s magnetosphere. This powerful code saves computational cost over global kinetic simulations via a flexible coupling, allowing the kinetic code to be activated in customizable smaller regions below the global scale as well as adapt the spatial coverage of the kinetic region at runtime. In this presentation, we summarize ongoing work and recent model capabilities in various physics domains. Specifically, MHD-AEPIC has been used to simulate magnetotail reconnection for multiple extreme geomagnetic storm events, showing global impacts of kinetic physics far downtail. The PIC region has also been placed over the dayside magnetopause to study reconnection onset and x-line topology, with the kinetic physics producing multiple highly-dynamic x-lines that can extend past the terminator in local time even under idealized conditions. Configured to cover the dayside solar wind-magnetosphere coupling, the MHD-AEPIC simulation can also produce the ion and electron foreshocks that have been the focus of earlier large-scale kinetic simulations. Finally, we highlight the unique capabilities of MHD-AEPIC to produce particle distributions and differential fluxes analogous to observations by magnetospheric missions such as MMS. The simulated distributions can be extracted from any location in the kinetic code, and the individual particles can be traced backward and forward in time to identify source and loss regions. Unlike test particle simulations, the particles in MHD-AEPIC control the plasma state variables of the simulation, which allows us to examine self-consistent mesoscale features such as bursty bulk flows and their evolving distribution functions. With these capabilities, the MHD-AEPIC model represents a major step forward in realistic magnetospheric simulations that can be carried out with current computational resources over time scales of a geomagnetic storm.

How to cite: Pulkkinen, T., Keebler, T., Chen, Y., and Wang, X.: MHD-AEPIC: Coupled MHD-kinetic simulation of global, meso-, and small-scale magnetospheric phenomena, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-13176, https://doi.org/10.5194/egusphere-egu25-13176, 2025.

X4.51
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EGU25-14327
Syau-Yun Hsieh and David Sibeck

Transient increases in the H components of dayside ground magnetograms have long been associated with southward IMF turnings (DP2 convection patterns) and abrupt enhancements in the solar wind dynamic pressure (sudden impulses and storm commencements). The amplitudes of these perturbations peak under the equatorial electrojet, indicating that both the pressure changes and the southward IMF turnings apply duskward electric fields to the dayside equatorial ionosphere.  Southward IMF turnings increase the likelihood of reconnection on the dayside magnetopause, drive sunward flows in the magnetosphere towards the dayside reconnection line on the magnetopause, and apply the required duskward electric fields to the ionosphere.   However, compressions of the magnetosphere drive antisunward flows and are associated with dawnward (not duskward) electric fields in the dayside magnetosphere.  The contradiction can be resolved if it is supposed that the same sudden compressions of the magnetosphere also enhance reconnection on the dayside magnetopause.  Thus one would expect the strongest north/south perturbations in equatorial ground magnetograms to be associated with BOTH southward IMF turnings and increases in the solar wind dynamic pressure.  We present results from a statistical survey of OMNI solar wind,  GOES magnetospheric, and equatorial ground magnetometer observations.

How to cite: Hsieh, S.-Y. and Sibeck, D.:  Transient Magnetic Field Signatures Under the Equatorial Electrojet , EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-14327, https://doi.org/10.5194/egusphere-egu25-14327, 2025.

X4.52
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EGU25-21029
Yiqun Yu, Longxing Ma, Ziming Wei, Depeng An, Haijun Wu, Haoyu Lu, and Jinbin Cao

The ring current, one of the most important current systems around the Earth, intensifies during geomagnetic storms and is believed to be the main reason for large-scale magnetic field perturbations in the geospace environment. Understanding how the ring current builds up and evolves during geomagnetic storms is of great importance not only for advancing the knowledge of the Sun-Earth system but also for improving the modeling capability of predicting hazardous space weather events. In this study, we establish a kinetic ring current model, named STRIM, based on the bounce-averaged Fokker-Planck equation. The STRIM comprehensively embraces key physical processes in association with ring current dynamics, such as plasma source injections from the nightside plasmasheet and transport around the Earth, charge-exchange with neutral hydrogens, Coulomb collisions with thermal plasma, diffusive wave-particle interactions, field line curvature scattering, as well as precipitation loss down to the upper atmosphere. The electric fields needed for particle motion can be optionally taken from empirical models or self-consistently calculated, while the magnetic field configuration is obtained from the Tsyganenko 2005 model plus the IGRF internal model. Simulation results are verified against published literatures and validated with in-situ satellite or ground-based observations and are found to have the same high-level capability and fidelity as other well-known published models. We also discuss future tasks of fostering the model’s performance, such as advancing it to be bounce-resolved, to include N/S asymmetry in precipitation, or to implement a flexible outer boundary.

How to cite: Yu, Y., Ma, L., Wei, Z., An, D., Wu, H., Lu, H., and Cao, J.: A storm-time ring current model (STRIM), EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-21029, https://doi.org/10.5194/egusphere-egu25-21029, 2025.

X4.53
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EGU25-3379
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ECS
Minghui Zhu, Lei Dai, Chi Wang, Walter Gonzalez, Andrey Samsonov, Xiaocheng Guo, Yong Ren, Binbin Tang, and Qiuyu Xu

Magnetospheric convection is a fundamental process in the coupling of the solar wind, magnetosphere, and ionosphere. Recent studies have shown that dayside magnetopause reconnection drives magnetospheric convection, progressing from the dayside to the nightside within approximately 10-20 minutes in response to southward turning of the interplanetary magnetic field (IMF). In this study, we use global magnetohydrodynamic (MHD) simulations to investigate the influence of ionospheric conductance on dayside-driven convection. We conduct three simulation runs: two with normal ionospheric conductance and one with nearly infinite conductance. The temporal and spatial pattern of magnetospheric convection largely remain consistent across all three simulation runs. Comparing the results, we observe a reduction of 20% in magnetospheric convection and a 30% increase of ionospheric Region 1 field-aligned current (FAC) and Pedersen current in the run with nearly infinite conductance, compared to the normal conductance model. The results indicate that ionospheric conductance does not affect the response time of enhanced magnetospheric convection to the solar wind. We suggest that the 10-20 minutes timescale for establishing magnetospheric convection corresponds to the anti-sunward drag of reconnected magnetic field lines from the sub-solar point to the flank magnetopause. In cases of larger ionospheric conductance, the ionosphere footprints of dragged field lines become more stationary, potentially resulting in larger Region 1 FAC and ionosphere Pedersen current. A larger Pedersen current is associated with stronger sunward J×B force in the ionosphere, which corresponds to a stronger anti-sunward force in the magnetosphere, thereby reducing sunward convection of closed field lines.

How to cite: Zhu, M., Dai, L., Wang, C., Gonzalez, W., Samsonov, A., Guo, X., Ren, Y., Tang, B., and Xu, Q.: The Influence of Ionospheric Conductance on Magnetospheric Convection during the Southward IMF, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-3379, https://doi.org/10.5194/egusphere-egu25-3379, 2025.

X4.54
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EGU25-1367
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ECS
A 'wave-like' evolution of polar cap patches modulated by enhanced magnetopause reconnection and extended magnetotail reconnection
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Duan Zhang, Qinghe Zhang, Kjellmar Oksavik, Binbin Tang, Yongliang Zhang, Michael Lockwood, John C. Foster, Shun-Rong Zhang, Larry R. Lyons, Zan-Yang Xing, Yong Wang, and Yu-Zhang Ma
X4.55
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EGU25-2528
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ECS
Wenhao Chen, Tieyan Wang, Chao Xiao, and Xiaoxiao Qin

The Earth's magnetospheric cusp serves as a key channel for solar wind particles to enter the magnetosphere and for ionospheric ions to escape. The plasma density is central to understanding of these processes. Based on Cluster observation (collected between 2001 and 2010) of 878 cusp-crossing events, we performed a statistical study on the three-dimensional distribution of cusp ion density, as well as the primary influencing factors.
Our findings show that the highest density occurs around MLT=12 in both hemispheres, declining as MLT shifts away from noon. In SM coordinates, the maximum density appears near the equatorward boundary along the X direction, while variations in the Z direction are relatively small. This feature can be explained by the inhomogeneity of magnetic pressure. We also observed that solar wind ions, as the main source, most effectively enter the cusp around noon and diffuse toward dawn and dusk. As the AE index grows, the polar ionosphere becomes increasingly important, supplying particles from a wide range of MLT values to the cusp. Finally, the cusp density is found to be correlated with dipole angle, suggesting the cusp’s ability to funnel charged particles depends on how Earth’s magnetic field is oriented.

How to cite: Chen, W., Wang, T., Xiao, C., and Qin, X.: Statistics of the Density Distribution in the Earth’s Cusp Region: Cluster Observations, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-2528, https://doi.org/10.5194/egusphere-egu25-2528, 2025.

X4.56
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EGU25-3168
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ECS
Hyangpyo Kim, Rumi Nakamura, Jaeheung Park, Adriana Settino, and Kyoung-Joo Hwang

We present multi-scale observations of a foreshock transient and its impact on the magnetosheath, magnetosphere and ionosphere, utilizing the data from Cluster, THEMIS, ground-based radars, and magnetometers. During the storm recovery phase on March 25, 2015, the Cluster spacecraft observed the foreshock transient at GSE (8, -0.5, -13) Re. Subsequently, THEMIS A and E, residing in the equatorial plane, detected large-scale high-speed jets in the postnoon sector between 7 and 9 Re from Earth. At geosynchronous orbit, GOES-13 crossed the magnetopause, during which strong poleward plasma convection and tongue of ionization (TOI) were detected by incoherent scatter radars at Prince George, Saskatoon, Kapuskasing, and Rankin Inlet stations and GPS total electron content (TEC) measurements. The signature of field-aligned currents was observed by ground magnetometers. These simultaneous observations indicate that the foreshock transient plays an important role in energy transfer between the solar wind, the magnetosphere, and the ionosphere. This event provides the first observational evidence that a foreshock transient can lead to significant disturbances in the coupled magnetosphere-ionosphere system, being an important ingredient in space weather.

How to cite: Kim, H., Nakamura, R., Park, J., Settino, A., and Hwang, K.-J.: Foreshock transient impact on the magnetosheath, magnetosphere and ionosphere, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-3168, https://doi.org/10.5194/egusphere-egu25-3168, 2025.

X4.57
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EGU25-4585
Yongcun Zhang, Mingtao Cheng, Lei Dai, Zheng Wang, Xiaochao Yang, and Chi Wang

 

Previous research has established that in geospace, the total electron content (TEC) in the ionosphere can be modulated efficiently by ultralow frequency (ULF) waves in high-latitude regions. However, the correlations between TEC variations and ULF waves in middle-latitude and low-latitude regions remain inadequately explored. In this study, using ground-based magnetometer data from the Chinese Meridian Project, we identified ULF wave events within Pc4 frequency bands in the midlatitude region. During the period from July 1 and December 30, 2023, we identified 438 distinct ULF wave events in the Pc4 band, thereby creating a comprehensive ULF wave database. Statistical analysis indicated that Pc4-band ULF wave events predominantly occurred on the dusk side in midlatitude regions. Notably, on August 24, 2023, simultaneous observations of geomagnetic disturbances and TEC disturbances at the similar frequency were recorded, suggesting a potential correlation between Pc4 ULF waves and TEC variations at midlatitudes. Through quantitative analysis, we infer that ionospheric TEC variations were possibly triggered by Pc4 ULF waves during this event.This result provides direct observational evidence of the modulation of the TEC by Pc4 ULF waves in the midlatitude region. These findings broaden our understanding of the coupling between the solar wind-magnetosphere-ionosphere in midlatitude regions, and have the potential significance on evaluating the effect of space weather of this coupling process.

How to cite: Zhang, Y., Cheng, M., Dai, L., Wang, Z., Yang, X., and Wang, C.: Modulation of the TEC in the Midlatitude Region by ULF Waves: Preliminary Conjunctional Observations between LFWR and GNSS in the Chinese Meridian Project, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-4585, https://doi.org/10.5194/egusphere-egu25-4585, 2025.