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Fig. 5

image

Evolution of the IR flare Tb spectrum for the model with δ = 5 and Ec = 30 keV. For λ> 50 μm, the brightness temperature tends to reflect the actual electron temperature in the optically-thick upper chromosphere. The inset planel shows the flare excess emission, after subtracting the pre-flare spectrum. This highlights the positive slope of the short-wavelength branch, Tb(ν) ∝ ν2, that can be identified with the Rayleigh-Jeans law expected from an optically-thin slab.

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