DIKUL - logo
E-resources
Full text
Peer reviewed Open access
  • Test Particle Model Predict...
    Jolitz, R. D.; Dong, C. F.; Rahmati, A.; Brain, D. A.; Lee, C. O.; Lillis, R. J.; Curry, S. M.; Jakosky, B. M.

    Journal of geophysical research. Space physics, August 2021, 2021-08-00, 20210801, Volume: 126, Issue: 8
    Journal Article

    Extreme space weather events can episodically release solar energetic particles (SEPs) that precipitate into planetary atmospheres, leading to aurora and increased ionization. While the induced magnetosphere of Mars does not substantially obstruct SEP protons, the effect on SEP electrons is not known. We use a test particle model modified for relativistic electrons to model transport of 10–200 keV electrons from outside the bow shock and deep in the magnetotail of Mars. We find a substantial influence of curvature and gradient drifts on precipitation, leading to depletions in the bow shock and transport onto closed field lines. The model estimates ∼3% of incident flux precipitates into the Mars atmosphere for a typical SEP event under nominal solar wind conditions, exceeding the estimate from the guiding center path approximation without drift terms. Precipitation is globally patchy. The model estimates 55% of electrons precipitating into cusps along open field lines and 45% precipitating on closed field lines, suggesting drift and nonadiabatic transport mechanisms have a significant influence on precipitation. We also predict that the fraction of precipitating differential flux increases as a function of energy. We discuss how these predictions would be affected by disturbed conditions that tend to accompany the arrival of SEPs and by differing SEP electron spectra hardness and anisotropy. We finally discuss how the simulation predictions compare to observations of diffuse aurora. Key Points For a “typical” event, only 3% of incident energetic (10–200 keV) electron flux will precipitate Energetic electron depletions occur within the bow shock Precipitation is patchy, occurring along open field lines into cusps and closed field lines via drift and nonadiabatic transport mechanisms