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Fig. 9

image

Spectra 12CO2 and 13 CO2 for models with different destruction rates at a spectral resolving power R = 2200 appropriate for JWST-MIRI. The abundance floor is taken to be 10−8. The black line shows the model results for a constant abundance as used in Bosman et al. (2017). The regions were the Q-branch flux is extracted is shown in the black lines. The 13CO2 Q-branch is blended with the 12CO2 P(23) line. The neighbouring P(21) line is indicated. Note that the models with destruction rates of 10−11 and 10−10 s−1 are indistinguishable in their 12CO2 spectra.

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