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Fig. E.2.

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External FUV radiation field (in energy density) propagating inside the photoevaporating wind and outer disk surface (reference model of d203-506 with G0 = 2 × 104 and nH = 107 cm−3). The upper panels (blue spectra) are for a slab position at AV = 0.1 mag (close to the PDR surface), whereas the lower panels (red spectra) are for a position deeper inside the PDR, at AV = 0.5 mag. The disk-depth-dependent FUV field results from a FUV radiative transfer calculation that includes gas absorption, H2 fluorescent emission, and grain absorption and scattering. The resulting FUV continuum and line emission are modulated by strong H I absorption lines (Ly-α and Ly-β lines are indicated in this figure) and by a forest of H2 absorption and fluorescent emission lines. The black vertical lines show the wavelength position of the main C0 pumping transitions at 1277, 1279, and 1280 Å (∼9.6 eV). The vertical dashed gray lines show the wavelength position of the main O0 pumping transitions at 1027 and 1040 Å (∼12 eV). These photons are quickly absorbed by small column densities of gas, mainly via C0 photoionization below 1101 Å for AV < 1 mag (Fig. F.1). Lower-energy FUV photons propagate deeper inside the disk and are attenuated by dust grains.

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