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Fig. 3

image

Left panel: comparison between Ntot (HCNH+) and Ntot (HCN). The latter was derived from the H13CN J = 1− 0 line (Colzi et al. 2018b), assuming the same Tex, by correcting it for the 12C/13C ratio obtained at the Galactocentric distance of the sources from the trend of Yan et al. (2019). Ntot (HCNH+) has been rescaled to the (larger) beam of the H13CN observations, ~ 28′′. Red stars are HMPOs; blue stars are UCHIIs; black symbols are HMSCs (filled circles for quiescent,stars for warm; see Table 1). Triangles indicate upper limits on Ntot (HCNH+). The dashed line is the locus where Ntot (HCNH+) = 0.01 Ntot (HCN). Middle panel: same as left panel, but for the fractional abundances with respect to H2 calculated on a beam of ~28′′. The purple rectangle indicates the range of abundances that reproduces the observed [HCN], and [HCNH+] in the predictions of the WM (see Sect. 5 and right panel of Fig. 7). Similarly, the cyan square indicates the prediction of the CM (see Sect. 5 and left panel of Fig. 7). Right panel: comparison between the line FWHM of HCNH+, derived in this work from the J = 3−2 line, and H13 CN, derived by Colzi et al. (2018a) from the J = 1−0 line at ~87 GHz. The symbols have the same meaning as those in the left and middle panels.

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