Fig. F.1.
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Alternative cases with pre-shock gas density nH2 = 103 cm-3 in a slow shock scenario (vs = 10 km/s, where we compare cases of CRIR from 1ζ0 (top) to 105ζ0 (bottom). It is clear that an higher CRIR could further suppress the HNCO abundance enhanced via slow shocks.
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