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Fig. C.1.

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Inverse of the HCN emissivity (in units of the HCN conversion factor) as a function of HCN intensity. We plot the PHANGS-, NGC 4038/9-, and NGC 3256-type models from left to right as the blue, orange, and green filled contours. The black contours represent ⟨ϵHCN−1 for the models where we make a cut at 0.1 K km s−1, which is analogous to a sensitivity limit in observations. For comparison, we also show the Gao & Solomon (2004a,b) value as the black, dotted horizontal line and several published values of αHCN from observations of Milky Way clouds (Dame & Lada 2023; Shimajiri et al. 2017). The gray, filled contour represents all models. We find the HCN emissivities from the PHANGS-type models to be most strongly impacted by a sensitivity cut. These models appear to have artificially lower ⟨ϵHCN−1 (higher emissivity) as a result of the cut.

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