Deep Entry of Low‐Energy Ions Into Mercury’s Magnetosphere: BepiColombo Mio’s Third Flyby Observations

Author:

Harada Yuki1ORCID,Saito Yoshifumi2ORCID,Hadid Lina Z.3,Delcourt Dominique3ORCID,Aizawa Sae3ORCID,Rojo Mathias4,André Nicolas45ORCID,Persson Moa6ORCID,Fraenz Markus7,Yokota Shoichiro8ORCID,Fedorov Andréi4,Miyake Wataru9ORCID,Penou Emmanuel4,Barthe Alain4,Sauvaud Jean‐André4ORCID,Katra Bruno3ORCID,Matsuda Shoya10ORCID,Murakami Go2ORCID

Affiliation:

1. Department of Geophysics Graduate School of Science Kyoto University Kyoto Japan

2. Institute of Space and Astronautical Science Japan Aerospace Exploration Agency Tokyo Japan

3. Laboratoire de Physique des Plasmas (LPP) CNRS Observatoire de Paris Sorbonne Université Université Paris Saclay Ecole Polytechnique Institut Polytechnique de Paris Palaiseau France

4. IRAP CNRS‐UPS‐CNES Toulouse France

5. Institut Supérieur de l’Aéronautique et de l’Espace (ISAE‐SUPAERO) Université de Toulouse Toulouse France

6. Swedish Institute of Space Physics Uppsala Sweden

7. Max‐Planck‐Institute for Solar System Research Göttingen Germany

8. Department of Earth and Space Science Graduate School of Science Osaka University Osaka Japan

9. Tokai University Kanagawa Japan

10. Graduate School of Natural Science and Technology Kanazawa University Kanazawa Japan

Abstract

AbstractAlthough solar wind‐driven convection is expected to dominate magnetospheric circulation at Mercury, its exact pattern remains poorly characterized by observations. Here we present BepiColombo Mio observations during the third Mercury flyby indicative of convection‐driven transport of low‐energy dense ions into the deep magnetosphere. During the flyby, Mio observed an energy‐dispersed ion population from the duskside magnetopause to the deep region of the midnight magnetosphere. A comparison of the observations with backward test particle simulations suggests that the observed energy dispersion structure can be explained in terms of energy‐selective transport by convection from the duskside tail magnetopause. We also discuss the properties and origins of more energetic ions observed in the more dipole‐like field regions of the magnetosphere in comparison to previously reported populations of the plasma sheet horn and ring current ions. Additionally, forward test particle simulations predict that most of the observed ions on the nightside will precipitate onto relatively low‐latitude regions of the nightside surface of Mercury for a typical convection case. The presented observations and simulation results reveal the critical role of magnetospheric convection in determining the structure of Mercury's magnetospheric plasma. The upstream driver dependence of magnetospheric convection and its effects on other magnetospheric processes and plasma‐surface interactions should be further investigated by in‐orbit BepiColombo observations.

Funder

Centre National d’Etudes Spatiales

Japan Society for the Promotion of Science

Publisher

American Geophysical Union (AGU)

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