Space Weather & Heliophysics

Magnetic Interaction of Stellar Coronal Mass Ejections with Close-in Exoplanets: Implication on Planetary Mass Loss and Ly-α Transits

By Keith Cowing
Status Report
astro-ph.SR
November 20, 2024
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Magnetic Interaction of Stellar Coronal Mass Ejections with Close-in Exoplanets: Implication on Planetary Mass Loss and Ly-α Transits
Density evolution of planetary material during the interaction of a CME with the planet HD189733b as seen in the polar plane (𝑥𝑧 plane). Black streamlines show the magnetic field lines representing the evolution of the magnetosphere during the interaction. Different snapshots are the same as figure 3. This case considers a CME magnetic field of 𝐵𝑧 = +1 G (Case I). — astro-ph.SR

Coronal Mass Ejections (CMEs) erupting from the host star are expected to have effects on the atmospheric erosion processes of the orbiting planets. For planets with a magnetosphere, the embedded magnetic field in the CMEs is thought to be the most important parameter to affect planetary mass loss.

In this work, we investigate the effect of different magnetic field structures of stellar CMEs on the atmosphere of a hot Jupiter with a dipolar magnetosphere. We use a time-dependent 3D radiative magnetohydrodynamics (MHD) atmospheric escape model that self-consistently models the outflow from hot Jupiters magnetosphere and its interaction with stellar CMEs. For our study, we consider three configurations of magnetic field embedded in stellar CMEs — (a) northward Bz component, (b) southward Bz component, and (c) radial component.

We find that both the CMEs with northward Bz component and southward Bz component increase the planetary mass-loss rate when the CME arrives from the stellar side, with the mass-loss rate remaining higher for the CME with northward Bz component until it arrives at the opposite side. The largest magnetopause is found for the CME with a southward Bz component when the dipole and the CME magnetic field have the same direction.

We also find that during the passage of a CME, the planetary magnetosphere goes through three distinct changes – (1) compressed magnetosphere, (2) enlarged magnetosphere, and (3) relaxed magnetosphere for all three considered CME configurations. We compute synthetic Ly-α transits at different times during the passage of the CMEs.

The synthetic Ly-α transit absorption generally increases when the CME is in interaction with the planet for all three magnetic configurations. The maximum Ly-α absorption is found for the radial CME case when the magnetosphere is the most compressed.

Gopal Hazra, Aline A. Vidotto, Stephen Carolan, Carolina Villarreal D’Angelo, Dúalta Ó Fionnagáin

Comments: 15 pages, 12 figures, to appear in MNRAS, comments are welcome
Subjects: Solar and Stellar Astrophysics (astro-ph.SR); Earth and Planetary Astrophysics (astro-ph.EP)
Cite as: arXiv:2411.06283 [astro-ph.SR](or arXiv:2411.06283v1 [astro-ph.SR] for this version)
https://doi.org/10.48550/arXiv.2411.06283
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Submission history
From: Gopal Hazra
[v1] Sat, 9 Nov 2024 20:54:39 UTC (25,146 KB)
https://arxiv.org/abs/2411.06283

Astrobiology,

Explorers Club Fellow, ex-NASA Space Station Payload manager/space biologist, Away Teams, Journalist, Lapsed climber, Synaesthete, Na’Vi-Jedi-Freman-Buddhist-mix, ASL, Devon Island and Everest Base Camp veteran, (he/him) 🖖🏻