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Hard X-ray Contribution in AU Mic Flares and Its Minor Role in Atmospheric Escape

Published 20 Aug 2025 in astro-ph.SR, astro-ph.EP, and astro-ph.HE | (2508.15107v1)

Abstract: Flares from stars can significantly impact the atmospheres of their orbiting planets, yet the role of hard X-ray (HXR; 3-20 keV) emission in driving escape and tracing particle acceleration remains poorly constrained. With the aim of quantifying the HXR share of the total radiative budget, we obtained a NuSTAR observation, quasi-simultaneous with Swift and Einstein Probe observations, of the young M1Ve star AU Mic, detecting two flares. We build an empirical soft X-ray (SXR; 0.3-3 keV)-HXR scaling relation and, on that basis, quantify the HXR share of the total radiative budget, defined as the sum of extreme ultraviolet (EUV; 0.01-0.3 keV), SXR, and HXR, and assess its effect on atmospheric escape. We find that the HXR fraction is 1.7% in quiescence and rises to 3.3% at flare peaks; even adopting the EUV + SXR (collectively referred to as XUV) escape efficiency as an upper bound, HXR-powered mass loss amounts to only a few percent of the XUV-driven rate. High-energy spectral tails are detected in quiescence and in Flare 2. Both nonthermal and high temperature thermal models provide acceptable fits to the data; however, the presence of two localized Neupert effect episodes in Flare 2, combined with the implausibly large energy budget required for a 290 MK plasma, strongly favors a nonthermal interpretation. Consistent with this picture, spectral-timing analysis shows that the 6-20 keV share of the emission actually declines during flares, while heating is dominated by 3-6 keV photons-implying rapid thermalization of accelerated electrons and a predominantly thermal energy release. Overall, the flares are thermally dominated, nonthermal electrons can power chromospheric heating episodically, but HXR-induced escape appears to be marginal for the long-term atmospheric evolution of AU Mic's planets.

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