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Fig. 4.

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Spectral energy distributon of the radiation field: at the entrance of the HII region (dotted line), at the ionization front (dashed line), compared to the same initial BC03 radiation field simply truncated at the Lyman break (solid line), (a) for log U = −2, nH = 100 cm−3 and Zstars = 0.02, (b) as a function of Zstars, (c) as a function of U for nH = 100 cm−3) and Zstars = 0.02, (d) and as a function of nH for log U = −2 and Zstars = 0.02.

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