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Fig. 22

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χ2 difference between simulations of the 2010 data and the best fit without atmospheric escape as a function of the stellar wind density, assuming a constant escape rate and ionizing flux ( = 2 × 109 g s-1 and Fion = 10  F, thick blue line). The intersection with the black dotted lines gives the proton density above which an absorption signature would have been detected at more than 1, 2 or 3σ in the 2010 observations. The upper limit on the proton density decreases with higher escape rates ( = 2 × 1010 g s-1 and Fion = 10  F, blue dotted line) and increases with higher ionizing fluxes ( = 2 × 109 g s-1 and Fion = 20  F, blue dash-dotted line).

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