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Table 5.

HCN/CO(1–0) vs. Σmol relations.

m (unc.) b (unc.) σ Σmol res. HCN/CO res. Σmol method Reference
(1) (2) (3) (4) (5) (6) (7)
0.61 (0.10) −2.64 (0.21) 0.28 260 pc 260 pc beam-matched this work
0.72 (–) −2.88 (–) 300 − 600 pc 300 − 600 kpc beam-matched Gallagher et al. (2018b)
0.81 (0.09) −3.80 (0.21) 120 pc 650 pc CO-weighted average Gallagher et al. (2018a)
0.50 (0.10) −2.40 (0.20) ∼2 kpc ∼2 kpc beam-matched Jiménez-Donaire et al. (2019)
0.41 (0.03) −2.70 (0.08) 0.14 ∼100 pc 1 − 2 kpc CO-weighted average Neumann et al. (2023b)
0.71 (0.03) −3.30 (0.80) ∼0.1 pc ∼0.1 pc beam-matched Tafalla et al. (2023)
0.59 (0.03) −2.64 (0.04) 0.18 1 − 2 kpc 1 − 2 kpc beam-matched Neumann, Jiménez-Donaire et al. (in prep.)

Notes. Best-fit lines of HCN/CO vs. Σmol of the form shown in Eq. (10), with slope m (column 1), intercept b (column 2) and respective uncertainties. σ (column 3) denotes the 1-sigma scatter of the significant data about the fit line. The lines are plotted in Fig. 9. Columns 4 and 5 list the respective x- (Σmol) and y-axis (HCN/CO) resolutions. “Beam-matched” (column 6) refers to a matched resolution of the x- and y-axis data, and “CO-weighted average” denotes a CO intensity-weighted average measurement of Σmol, adopted in Gallagher et al. (2018a) and Neumann et al. (2023b). The differences between the physical scales and methodologies are discussed in the text.

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