Does the HCN/CO ratio trace the star-forming fraction of gas?

We modeled emissivities of the HCN and CO J = 1–0 transitions across a grid of molecular cloud models encapsulating observed properties that span from normal star-forming galaxies to more extreme merging systems. These models are compared with archival observations of the HCN and CO J = 1–0 transitions, in addition to the radio continuum at 93 GHz, for ten nearby galaxies. We combined these model emissivities with the predictions of gravoturbulent models of star formation presented in the first paper in this series. In particular, we explored the impact of excitation and optical depth on CO and HCN emission and assess if the HCN/CO ratio tracks the fraction of gravitationally bound dense gas, f grav , in molecular clouds. We find that our modeled HCN/CO ratios are consistent with the measurements within our sample, and our modeled HCN and CO emissivities are consistent with the results of observational studies of nearby galaxies and clouds in the Milky Way. CO emission shows a wide range of optical depths across different environments, ranging from optically thick in normal galaxies to moderately optically thin in more extreme systems. HCN appears only moderately optically thick and shows significant subthermal excitation in both normal and extreme galaxies. We find an anticorrelation between HCN/CO and f grav , which implies that the HCN/CO ratio is not a reliable tracer of f grav . Instead, this ratio appears to best track gas at moderate densities ( n > 10 3.5 cm −3 ), which is below the typically assumed dense gas threshold of n > 10 4.5 cm −3 . We also find that variations in CO emissivity depend strongly on optical depth, which is a product of variations in the dynamics of the cloud gas. HCN emissivity is more strongly dependent on excitation, as opposed to optical depth, and thus does not necessarily track variations in CO emissivity. We further conclude that a single line ratio, such as HCN/CO, will not consistently track the fraction of gravitationally bound, star-forming gas if the critical density for star formation varies in molecular clouds. This work highlights important uncertainties that need to be considered when observationally applying an HCN conversion factor in order to estimate the dense (i.e., n > 10 4.5 cm −3 ) gas content in nearby galaxies.

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Publication Details

Journal
Astronomy and Astrophysics
Published
2024-11-04
DOI
https://doi.org/10.1051/0004-6361/202347879
Citations
2
Primary Topic
Geophysics and Gravity Measurements
Type
article
Field-Weighted Citation Impact
0.96

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article

Does the HCN/CO ratio trace the star-forming fraction of gas?

Ashley Bemis, C. D. Wilson, Ian Roberts, Piyush Sharda et al.
2 citations
Astronomy and Astrophysics
Geophysics and Gravity Measurements
0.96
article

Does the HCN/CO ratio trace the star-forming fraction of gas?

Ashley Bemis, C. D. Wilson, Ian Roberts, Piyush Sharda, Hao He
article en
2 citations

Abstract

We modeled emissivities of the HCN and CO J = 1–0 transitions across a grid of molecular cloud models encapsulating observed properties that span from normal star-forming galaxies to more extreme merging systems. These models are compared with archival observations of the HCN and CO J = 1–0 transitions, in addition to the radio continuum at 93 GHz, for ten nearby galaxies. We combined these model emissivities with the predictions of gravoturbulent models of star formation presented in the first paper in this series. In particular, we explored the impact of excitation and optical depth on CO and HCN emission and assess if the HCN/CO ratio tracks the fraction of gravitationally bound dense gas, f grav , in molecular clouds. We find that our modeled HCN/CO ratios are consistent with the measurements within our sample, and our modeled HCN and CO emissivities are consistent with the results of observational studies of nearby galaxies and clouds in the Milky Way. CO emission shows a wide range of optical depths across different environments, ranging from optically thick in normal galaxies to moderately optically thin in more extreme systems. HCN appears only moderately optically thick and shows significant subthermal excitation in both normal and extreme galaxies. We find an anticorrelation between HCN/CO and f grav , which implies that the HCN/CO ratio is not a reliable tracer of f grav . Instead, this ratio appears to best track gas at moderate densities ( n > 10 3.5 cm −3 ), which is below the typically assumed dense gas threshold of n > 10 4.5 cm −3 . We also find that variations in CO emissivity depend strongly on optical depth, which is a product of variations in the dynamics of the cloud gas. HCN emissivity is more strongly dependent on excitation, as opposed to optical depth, and thus does not necessarily track variations in CO emissivity. We further conclude that a single line ratio, such as HCN/CO, will not consistently track the fraction of gravitationally bound, star-forming gas if the critical density for star formation varies in molecular clouds. This work highlights important uncertainties that need to be considered when observationally applying an HCN conversion factor in order to estimate the dense (i.e., n > 10 4.5 cm −3 ) gas content in nearby galaxies.

Astronomy and AstrophysicsVol. 692
Leiden University (NL), University of Bonn (DE), University of Waterloo (CA), McMaster University (CA)
National Science Foundation, Gruber Foundation, National Radio Astronomy Observatory, Universiteit Leiden, Canada Research Chairs, Korea Astronomy and Space Science Institute, National Astronomical Observatory of Japan, Natural Sciences and Engineering Research Council of Canada, National Institutes of Natural Sciences
Openalex Percentile: Top 24%
Geophysics and Gravity Measurements
0.96
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