2024A&A...692A.146B


Query : 2024A&A...692A.146B

2024A&A...692A.146B - Astronomy and Astrophysics, volume 692A146 (2024/12-1)

Does the HCN/CO ratio trace the star-forming fraction of gas? II. Variations in CO and HCN emissivity.

BEMIS A.R., WILSON C.D., SHARDA P., ROBERTS I.D. and HE H.

Abstract (from CDS):

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, fgrav, 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 fgrav, which implies that the HCN/CO ratio is not a reliable tracer of fgrav. Instead, this ratio appears to best track gas at moderate densities (n > 103.5 cm–3), which is below the typically assumed dense gas threshold of n > 104.5 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 > 104.5 cm–3) gas content in nearby galaxies.

Abstract Copyright: © The Authors 2024

Journal keyword(s): ISM: clouds - ISM: general - ISM: molecules - galaxies: general - galaxies: ISM - galaxies: star formation

Simbad objects: 18

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Number of rows : 18
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 M 31 AGN 00 42 44.330 +41 16 07.50 4.86 4.36 3.44     ~ 13622 1
2 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
3 NAME Perseus Cloud SFR 03 35.0 +31 13           ~ 1553 0
4 NAME California Molecular Cloud MoC 04 10.0 +39 00           ~ 188 1
5 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
6 NAME Ori A MoC 05 38 -07.1           ~ 3187 0
7 NAME Ori B MoC 05 41 43.0 -01 54 44           ~ 1498 0
8 NAME Orion Molecular Cloud MoC 05 56 -01.8           ~ 1227 1
9 NGC 2623 LIN 08 38 24.016 +25 45 16.29 14.10 13.99 13.36     ~ 533 2
10 UGC 4881 IG 09 15 55.5 +44 19 58   14.9       ~ 178 0
11 NGC 2903 AGN 09 32 10.111 +21 30 02.99 10.44 9.75 9.07 8.68   ~ 1204 3
12 NGC 3256 Sy2 10 27 51.284 -43 54 13.55   11.83 11.33 10.62 11.9 ~ 920 2
13 NGC 4038 EmG 12 01 53.002 -18 52 03.32   10.91   9.74 11.0 ~ 1364 1
14 NAME Antennae IG 12 01 53.170 -18 52 37.92           ~ 1749 0
15 NAME Ophiuchus Molecular Cloud SFR 16 28 06 -24 32.5           ~ 3969 1
16 NAME the Brick MoC 17 46 09 -28 43.8           ~ 226 0
17 NAME Aql Region reg 18 31.1 -02 10           ~ 456 0
18 NGC 6946 H2G 20 34 52.332 +60 09 13.24   10.5       ~ 2661 2

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