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Table 5.

Spearman rank coefficients and p-values.

Quantities ρ p-value
Global L HCN / L HCO + $ L^\prime_{\rm HCN}/L^\prime_{\rm HCO^+} $ vs.
αAGN 0 . 17 0.23 + 0.24 $ -0.17^{+0.24}_{-0.23} $ 0 . 38 0.31 + 0.41 $ 0.38^{+0.41}_{-0.31} $
log ( L AGN bol / erg s 1 ) $ \log(L_{\mathrm{AGN}}^{\mathrm{bol}}/\mathrm{erg\,s}^{-1}) $ + 0 . 00 0.26 + 0.27 $ +0.00^{+0.27}_{-0.26} $ 0 . 44 0.34 + 0.38 $ 0.44^{+0.38}_{-0.34} $
 log(LIR/L) + 0 . 11 0.26 + 0.25 $ +0.11^{+0.25}_{-0.26} $ 0 . 42 0.33 + 0.39 $ 0.42^{+0.39}_{-0.33} $
 log(SFR/M yr−1) + 0 . 09 0.26 + 0.24 $ +0.09^{+0.24}_{-0.26} $ 0 . 44 0.33 + 0.38 $ 0.44^{+0.38}_{-0.33} $
S60/S100 + 0 . 02 0.25 + 0.25 $ +0.02^{+0.25}_{-0.25} $ 0 . 47 0.34 + 0.36 $ 0.47^{+0.36}_{-0.34} $
 [N II]122/[O III]88 + 0 . 50 0.32 + 0.25 $ +0.50^{+0.25}_{-0.32} $ 0 . 10 0.09 + 0.42 $ 0.10^{+0.42}_{-0.09} $

Resolved L HCN / L HCO + $ L^\prime_{\rm HCN}/L^\prime_{\rm HCO^+} $ vs.
αAGN 0 . 22 0.22 + 0.23 $ -0.22^{+0.23}_{-0.22} $ 0 . 31 0.26 + 0.44 $ 0.31^{+0.44}_{-0.26} $
log ( L AGN bol / erg s 1 ) $ \log(L_{\mathrm{AGN}}^{\mathrm{bol}}/\mathrm{erg\,s}^{-1}) $ + 0 . 05 0.25 + 0.24 $ +0.05^{+0.24}_{-0.25} $ 0 . 47 0.34 + 0.36 $ 0.47^{+0.36}_{-0.34} $
 log(LIR/L) + 0 . 23 0.25 + 0.23 $ +0.23^{+0.23}_{-0.25} $ 0 . 29 0.25 + 0.45 $ 0.29^{+0.45}_{-0.25} $
 log(SFR/M yr−1) + 0 . 23 0.25 + 0.22 $ +0.23^{+0.22}_{-0.25} $ 0 . 29 0.25 + 0.45 $ 0.29^{+0.45}_{-0.25} $
S60/S100 + 0 . 07 0.24 + 0.24 $ +0.07^{+0.24}_{-0.24} $ 0 . 47 0.34 + 0.35 $ 0.47^{+0.35}_{-0.34} $
 [N II]122/[O III]88 + 0 . 38 0.32 + 0.26 $ +0.38^{+0.26}_{-0.32} $ 0 . 21 0.19 + 0.46 $ 0.21^{+0.46}_{-0.19} $

Notes. We performed Spearman rank correlation analyses using the Monte Carlo perturbation plus bootstrapping method as implemented by pymccorrelation (Privon et al. 2020, see Sect. 5.2 for detail). Correlation coefficients ρ and p-values are the median and range of the 16 and 84 percentiles. Corresponding plots are shown in Figs. 2 and 3.

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