EGU26-11760, updated on 14 Mar 2026
https://doi.org/10.5194/egusphere-egu26-11760
EGU General Assembly 2026
© Author(s) 2026. This work is distributed under
the Creative Commons Attribution 4.0 License.
Poster | Tuesday, 05 May, 14:00–15:45 (CEST), Display time Tuesday, 05 May, 14:00–18:00
 
Hall X4, X4.165
The Martian Ion Foreshock Boundary
Karim Meziane1, Christian Mazelle2, Abdelhaq Hamza1, Cyril Simon-Wedlund3, Cesar Bertucci4, Jasper Halekas5, David Mitchell6, Jared Espley7, and Shannon Curry8
Karim Meziane et al.
  • 1Physics Department, University of New Brunswick, Fredericton, Canada (karim@unb.ca)
  • 2IRAP, Université de Toulouse, CNRS, UPS, CNES, Toulouse, France
  • 3Institute of Physics/Lustbühel Observatory, University of Graz, Graz, Austria
  • 4IAFE/CONICET, University of Buenos Aires, Ciudad Autónoma de Buenos Aires, Argentina
  • 5Department of Physics and Astronomy, University of Iowa, Iowa City, IA, USA
  • 6Space Sciences Laboratory, University of California, Berkeley, USA
  • 7NASA Goddard Space Center, Greenbelt, Maryland, USA
  • 8Laboratory for Atmospheric and Space Physics, University of Colorado, Boulder, USA

Planetary bow shocks are sites where a fraction of the solar wind is accelerated to suprathermal energies. In the terrestrial foreshock, sunward propagating ion beams of several keV collimated along the interplanetary field lines (Field-Aligned Beams) are usually observed within a region upstream from the quasi-perpendicular shock. Numerous observations indicate that these beams are not seen along IMF lines that make an angle larger than 70o with the local shock normal (θBn), thereby marking the spatial location of the ion foreshock boundary. The ion foreshock boundary reflects the maximum level of energization that solar wind ions can reach via coherent interaction with a planetary shock. In the present study, the Martian ion foreshock boundary is investigated for the first time using MAVEN particle and magnetic field data. More than fifty spacecraft orbit segments were scrutinized to identify the presence of FAB events. The shock geometry associated with each FAB event was determined using a bow shock model. The obtained results clearly indicate that no FAB is observed for a shock-θBn larger than 51o. Our results indicate that the Martian ion foreshock boundary is located downstream of the expected location based on the terrestrial case. This finding is in good agreement with a recent report showing that FABs observed in the Martian foreshock have noticeably lower speeds than those observed at Earth. The characteristics of both the terrestrial and Martian ion foreshock boundaries provide new and relevant insights into the mechanisms responsible for FAB formation at planetary bow shocks. Furthermore, the present results point to a spatial boundary where ultra-low frequency waves excited by the beams are found.

How to cite: Meziane, K., Mazelle, C., Hamza, A., Simon-Wedlund, C., Bertucci, C., Halekas, J., Mitchell, D., Espley, J., and Curry, S.: The Martian Ion Foreshock Boundary, EGU General Assembly 2026, Vienna, Austria, 3–8 May 2026, EGU26-11760, https://doi.org/10.5194/egusphere-egu26-11760, 2026.