Fig. 6

Example of apparently highly supersonic CO spectra in molecular clouds. Upper panel: characteristic supersonic (ℳ ~ 10) spectrum in B213-L1495 observed in C18O (1−0) (blue; Hacar et al. 2013), and 13CO (red) and 12CO (1−0) (black) lines (Goldsmith et al. 2008). Mid panel: predicted 13CO (red solid line) and 12CO (1−0) (black solid line) emission from the fitted C18O (1−0) line (blue) assuming pure opacity broadening (see text). Within the velocity range where the C18O is detected, its saturated emission reproduces most of the observed linewidths of both 13CO and 12CO lines. In the case of the two additional components detected in the most abundant 13CO and 12CO isotopologues, the expected C18O emission is consistent with noise (dashed lines). The central velocity of the 7 velocity components detected in the spectra are indicated by vertical blue lines at the top of the middle panel. Lower panel: 12CO (black line) and 13CO (red histogram) emission residuals after the subtraction of the corresponding saturated C18O emission. In this last case, the observed C18O (1−0) emission (blue dotted line) is superposed for illustrative purposes. We note how our simplified LTE treatment overestimates the self-absorption of the optically thick 13CO and, particularly, the 12CO lines. The remaining emission found between some of the modeled components observed in the 13CO wings (marked by vertical red lines in the lower panel) might suggest the presence of a diffuse substratum (i.e., inter-fiber medium; green dashed line; see Sect. 4.2). The contribution of Gaussian noise with rms = 0.2 K was included in all modeled spectra.
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